donation to help support this service.
If there is a link to a previously
answered question, be patient. Since the files containing the older
answers are rather large, it takes some time (maybe as much as 15
seconds or so) to find the appropriate bookmark.
t 2 and 82=vt where
v is the speed she left the road and t is the time to hit. I find that
t =0.61 s and v =134 ft/s=91 mph. Other guesses would be drops of 7 ft, 8 ft, and 9 ft giving speeds of 85 mph, 79 mph, and 74 mph,
respectively.
Hope this helps. There is no additional information which I can add.
R and with a speed v ,
the acceleration points toward the center of the earth and
has a magnitude a=v 2 /R ; this is
called the centripetal acceleration. Of course there has to
be a force which provides the acceleration and that is
simply the weight of the satellite. If you are close to the
earth's surface (compared to the radius R E
of the earth) the weight is mg and so
F=ma or mg =mv 2 /R E ;
so the speed you must have to orbit close to the surface of
the earth is v =√(gR E ).
The value of the acceleration g gets smaller as you
get farther away from the surface.
Rosetta , was sent to a comet and orbited it;
the escape velocity from the comet is only about 1 m/s so
the probe orbitted with a smaller speed than this.
N W mv 2 /r=W-N
or N=W -mv 2 /r . So, when
v gets big enough N =0; so the ring could
be taken away and this would be the right speed for a "real"
orbit at this r . And the ring would not work
for speeds larger than the orbital speed, the object would
leave the ring; any smaller v
would result in the speed remaining constant as the mass
rolled around.
L i ,
a weight W i , and a center of gravity
r i . Since the panels are uniform and have
weight density of 2.08 lb/ft, r i =½L i
and W i =2.08L i . I
will also specify the number of panels with the length L i
to be N i . The center of gravity of a
stack of panels of length L i is r i = ½N i W i L i /(N i W i ).
Now, suppose there are two different lengths stacked. Then
the position of the center of gravity is
r CG =(½N 1 W 1 L 1 +½N 2 W 2 L 2 )/(N 1 W 1 +N 2 W 2 )
=½x2.08x(N 1 L 1 2 +N 2 L 2 2 )/(2.08x(N 1 L 1 +N 2 L 2 ))
=½(N 1 L 1 2 +N 2 L 2 2 )/(N 1 L 1 +N 2 L 2 ).
So, if you have j different lengths, the final answer is
r CG =½(N 1 L 1 2 +N 2 L 2 2 +...N j L j 2 )/(N 1 L 1 +N 2 L 2 +...N j L j ).
The more compact way to write this is
r CG =½ΣN i L i 2 /ΣN i L i .
Here Σ denotes summing from i=1 to i=j.
Note that the denominator is the total weight of
the whole stack divided by 2.08 and that the
weight per foot is not needed to find the
location of the center of gravity.
groundrules forbid unphysical questions, and an infinite
number of windmills is obviously unphysical. However, let's
investigate whether a reasonable number of windmills could
have a significant impact on the weather. At the end of 2018
the total global wind power was about 600 GW, that's 0.6x1012
W; the total world power production is about 44x1012
W; an average hurricane has about 1.5x1012 W; the
Nagasaki atomic bomb was about 1013 W (1014
J and I guessed the time of the explosion was 10 s). It has
been
estimated that if we put wind farms covering all land
and all off-shore water, 80x1012 W would be
generated. That same
article estimated that you would need to have enough
wind mills to generate more than 250x1012 W to
have a noticeable effect on weather, about four times the
number feasible.
Bay of Fundy during tidal changes; it is harder for the
windmills because it is not easy to estimate the energy of a
"typical" storm, so the following calculation is a very
approximate one. A typical windmill generates about 3x106
W and guess that a typical strong storm is 10 times smaller
than a hurricane, 1.5x1011 W; so the percentage
by which the energy of the storm is reduced is 0.02%, so
5000 windmills would use up most of the wind energy.
r about the axis with
some frequency f (f times around every
second) and, if r is in ft, the speed it travels is
v =2πrf ft/s. For example if you are
doing 2 revolutions per second and r =2 ft, v =25
ft/s=17 mph. But, since the speed depends on r ,
every point moves with a different speed, the top being the
fastest. I have shown also the weight w and
centrifugal force c F with which the rope exerts on you; w
is the same for any piece of the rope the same size but
c depends on r , the largest being at the very
top in the figure and also at the very bottom as. When the
rope is straight up as shown, the forces F are
their smallest because c and w are in
opposite directions; when the rope is straight down, the
forces F are their largest because c and
w are in the same direction. But to actually
calculate the force is a formidable problem because we need
to add all the pieces which are all different (this adding
is integration in calculus if you have ever studied it).
Just to give you some idea of the answer you sought I will
assume that the rope has a negligible weight and the whole 3
lb is located in the middle of the rope and is a distance of
3 ft from the axis. You want v =10 mph=14.7 ft/s,
and c=mv 2 /r =6.75 lb. (Here
m is the mass which is 3/32 lb/(ft/s2 ), but
you don't need to worry about that.) So, at the top, the
force to hold it is 6.75-3=3.75 lb and at the bottom it is
6.75+3=9.75 lb. This is what you are calling the "equivalent
weight", I guess.
P =290/0.5=580 ft lb/s=1.055 horsepower=786 W.
t later. The moving
paper moves with velocity v perpendicular to the
not-moving edge and the intersection point moves with
velocity u along the not-moving edge. The distance
moved is v Δt and the distance
between the earlier and later edges of the moving paper is s =v Δt cosθ .
During this time interval, the intersection point has moved
a distance u Δt and s =u Δt sinθ.
Therefore,v Δt cosθ=u Δtsinθ
or u=v /tanθ. Suppose we want
u =2c and cause the paper to move with a
speed of v=c /2; then θ= tan-1 (v /u )=tan-1 (0.25)=140 .
So, indeed, the point of intersection can move faster than
the speed of light. How can this be? Isn't c the
universal "speed limit"? It is the limit for transmitting
information or for any object with mass; this intersection
neither has mass nor transmits any information. There is a
similar example where something can have a speed greater
than the speed of light without violating special
relativity. Imagine pointing a laser at the moon and
sweeping the spot on the moon across the surface by rotating
the laser; because of the long arm, it would be pretty easy
to get the spot going faster than c but, just as in
your example, the spot has no mass and conveys no
information.
discussion there.
ad absurdum .
v+c , still illuminating the
front of the ship. But that is not what he is doing. Instead
he is saying that there will be Cerenkov radiation (from the
flashlight, I guess) which is like the shock wave of a
supersonic aircraft. This is in the form of a cone behind
and that is the light supposedly illuminating the back. I
find this a very far fetched example and would advise you to
simply ignore it!
here .
W 1 ,
the weight of the rider; W 2 ,
the weight of the driver; W 3 ,
the weight of the motorcycle; D f etc .;
N 1 , the force up on the
rear wheel by the road; N F N 1 +N 2 =W 1 +W 2 +W 3
and F-f-D =0. The most important thing to appreciate
is that f is proportional to the normal force, f=C (N 1 +N 2 )
where C is some constant. So when the rider falls
off, W 1 disappears and so N 1
and N 2 get smaller and so f gets
smaller. F, however, does not depend on N 1
because it is static friction; it is determined by how much
power is being delivered by the engine so it does not
change. I will denote the new frictional force as
f' and note that it is smaller than
f F-f'-D =Ma where M
is the mass of the rider plus bike, M 2 +M 3 =(W 2 +W 3 )/g .
where g is the acceleration due to gravity.
Finally, the bike has an acceleration a =[(F-f'-D )/(W 2 +W 3 )]g .
m at sea level is
given by F 0 =mMG /R 2 =W
where R is the radius of the earth, M is
the mass of the earth, and G is the universal
gravitational constant; if you go up to an altitude h ,
the weight gets smaller, Fh =mMG /(R+h )2 .
Therefore, if you want to hover at an altitude h you must
exert an upward force of Fh = [R 2 /(R+h )2 ]W
where W is the weight at sea level. Even several
hundred miles is small compared to R which is about 4000
miles, so we can make an estimate by doing a binomial
expansion: R 2 /(R+h )2 =(1+(h /R ))-2 ≈1-(2h /R )+…
So suppose that h=R /20; then Fh ≈0.9W .
(The exact calculation would be 0.907W .) You asked
for the force "in terms of g-factors"; that would be the
factor of W , [R 2 /(R+h )2 ].
1% of that exerted by the radiation. By the way, light
having momentum is not a "theory", it is a well-measured
fact.
H and the number of times she
jumped during the semester N . The total time, in
seconds, that
child spent in the air would be T =0.072N √H
if H is measured in inches and T =0.045N √H
if H is measured in centimeters. For example, if
the child typically jumped 8 inches and jumped 200 times,
the total air time is T =0.072x200x√8=40.7
seconds. I would only worry that an elementary school
student might not be familiar with a square root. (You only
asked for an equation; I can also post the derivation of the
equations I posted here if you are interested.
recent answer . Think of the
passer as your pirate ship and the receiver as the target on
the ground. If the passer (ship) in the first figure is not
running (moving), the ball will go to the location of the
receiver (target) who will receive (which will be hit.) it
if not running. If the passer (ship) is running (moving), he
(it) will give his (its) velocity to the ball (cannonball),
in addition to the velocity he (it) imparts by throwing
(shooting); if the receiver (ship) is not running (moving),
he (it) will not catch it (be hit) because it will go to the
position he (the target) would have been if he (it) were
running (moving) too.
bike
plus rider needs to be halfway between the two axles
for the wheels to have equal friction. The left-to-right
location would have nothing to do with having equal
friction, so that can be ignored for your purposes; however,
since the the legs are moving up and down and forwards and
backwards, not sideways, the left-to-right centering never
changes anyway. The first figure shows one pedal up and one
down; the second figure shows level pedals. In the first
case, the right knee is quite forward and the left leg is
straight down; in the second case the right knee is less
forward than in the first case and the left knee is slightly
less forward than the right but substantially forward from
the first case. To my mind it is a tossup as to which has
the center of gravity more forward; and besides, where is
the center of gravity of the bike rider system? Furthermore,
in my opinion, any difference between the two cases will
make a trivial difference regarding whether one wheel or the
other is more likely to lose traction. In addition, if you
have an extreme lean or you are on terrain which is sloping
upward in the direction you are turning, you are less likely
to catch your pedal on the ground if it is all the way up.
Do whatever you are most comfortable with; this issue does
not merit "a great debate"!
is rate of change of velocity, then why a body is said to have a constant
acceleration due to gravity when a body is at rest at a plane horizontal surface?
g plays an
important role for the body which, if its mass is m ,
has a weight W given by W=mg .
E to each, E =½mv 2 ,
where m is the mass and v is the speed.
Therefore, ½m t v t 2 =½m b v b 2
or v b =v t √(m t /m b ).
Putting in the masses of the tennis ball and the baseball,
m t =0.058 kg and m b =0.145
kg, I find v b =58 mph.
W =3000
lb=13,345 N, 1.5 ft=0.467 m, 8.6 ft=2.62 m, 25 ft=7.62 m, and
6 ft=1.83 m. The answer depends on which way the wind blows.
So, I will make the calculation for the wind blowing
directly on the largest surface whose area will be A =7.62x0.467=3.56
m2 . There is a pretty good approximation for
calculating the drag force F on an object of cross
section A in a wind with speed v , F =¼Av 2 ,
so v =2√(F /3.56). (N.B. ,
this works only in SI units.) The forces on your mass are
shown in the figure. When I do the analysis I find F =3576
N=804 lb, and v =63.4 m/s=142 mph. Please keep in
mind that this is an approximation as are all calculations
of air drag.
A ,
thickness t , and temperatures T in
inside and T out outside. The rate of
heat flowing through the material depends on four things:
what the material is, what A is, what t is,
and the temperature difference ΔT =|T out -T in |.
(This assumes that conduction through the container is the
most important means of having heat flow, not convection or
thermal radiation.) So take two examples: inside cold water
at 10 C, outside room temperature at 200 C,
ΔT =190 C; and inside hot soup at 900 C,
outside room temperature at 200 C, ΔT =700 C.
So the soup would cool down faster than the cold water would
heat up. Why would evaporation have anything to do with it?
via one of the springs attached to it, on
its neighbor which then propogates the push to the next
neighbor, etc . Clearly, the speed of this sound,
displacements of molecules, will depend on the spring
constant of the springs; but the spring constants are an
approximate measure of the appropriate modulus. If we think
of the spacing of the molecules as being roughly constant
regardless of the composition of the solid, the mass of a
molecule is going to be proportional to the density. But,
the mass of a particle on a spring determines the speed of
the motion of the particle—the greater the mass, the more
slowly the particle moves when attached to a spring. By this
reasoning, the speed of sound depends on both modulus and
density.
is a battery. As long as it
can supply the current needed at the right voltage (power),
no other battery need be added.
y=x tanθ -(½g /(v 0 cosθ ))x 2
where the acceleration due to gravity is g =9.8 m/s2 ,
θ is the launch angle, and v 0
is the launch speed. In fact, since speeds are relatively
modest, air drag will probably be negligible. If you include
air drag, each bounce segment will be a different shape
because the drag depends on the speed of the ball.
F W F'= F -W F' v . Your coworker is right
that the force which provides the acceleration,
F' F W
F has a magnitude twice the weight of
the adult, approximately 1640 N (360 lb), so F' =820
N. If this force acts over 0.5 m for the adult, he launches
with a speed of about 3.2 m/s, while the force acting over
0.25 m launches super child with a speed of about 7.3 m/s.
With these initial speeds, the adult goes up about 0.5 m while
the child goes up about 2.7 m. Now, we must calculate the
height the adult will rise on the moon exerting the same
force over the same 0.5 m; but now the launching force is
F'=F-mg /6=1640-137=1503 N. I find the launching
speed to be about 4.3 m/s and the height to be about 5.5 m.
So the adult on the moon goes about 5.5/2.7=2 times as
high as child with equal leg strength does on earth, and
about 11 time higher than he could jump on earth; the reason
for this large factor of 11 is twofold—first, the fact
that the weight is much smaller means that the given leg
strength will be much more effective in accelerating during
the launch; second, once launched the weaker gravity cause
him to slow down more slowly. So your coworker's
guess about how the compared jumps would be is pretty far
off, a factor of two in terms of height achieved. However,
he got it qualitatively correct that a smaller person with
equally strong legs could jump higher on earth; it just
doesn't work out quantitatively when comparing to the jump
on the moon.
But, what is the real difference? If you look at the videos
they look like they are taken in slow motion, but they are
not. Because the gravity is much smaller, it will take much
more time to get up to and back down from a given height;
even if the height achieved by the super child on earth were
exactly the same as for the adult on the moon, the two would
appear very different because the child would be back to
ground level much faster than the adult would be.
gedanken , a
thought experiment; the cone is at the point of unstable
equilibrium and you would not be able to actually balance a
cone on its tip in the laboratory. Any force which has no
vertical component and has a line of action through the
center of mass will cause horizontal translational motion
but no rotational motion. In fact, any force passing through
the center of mass will cause no rotational motion. The more
general case is shown in the diagram. The effect of the
horizontal component (F x F y )
is to reduce the normal force (N mg Fy >mg , the cone would have an
acceleration in the y
direction as well, fly off the surface. The components of
the acceleration would be ax =Fx /m and ay = (Fy /m )-g.
In no case would the cone have any rotational motion.
ion propulsion in this link by NASA.
Mythbusters episode debunking the scene from that Sandra Bullock movie, but I'm interested in the theoretical point at which it could happen.
The diagram above shows the forces on the bus if it is turning
right (as seen by the driver) around a circle of radius R
(center to your left), traveling with speed v ; the
coefficient of static friction between the tires and the
road is μ . The bus is just about to skid and so
the frictional forces are at their limits, μN . The driver's side tires have a normal
force N 1 and a frictional force f 1 =μN 1 ;
similarly, the tires on the other side have a normal force
N 2 and a frictional force f 2 =μN 2 .
The weight of the bus, W=mg , acts at the center of mass of
the bus; I will assume that the center of mass is halfway
between the left and right wheels. The bus is in equilibrium
in the vertical direction, so N 1 +N 2 =mg .
The bus has a centripetal acceleration to your left a=v 2 /R
so f 1 +f 2 =mv 2 /R.
The greatest that f=f 1 +f 2 =can
be is f=μ (N 1 +N 2 )=μmg=mv2 /R.
Therefore the smallest radius that the bus can have if
its speed is v is R min,slide =v 2 /(μg ).
In your case, v =50 mph=22 m/s, g =9.8 m/s2 ,
and μ≈ 0.8 for rubber on dry asphalt, R min,slide ≈ 62
m=203 ft.
But you are interested
in the radius when the bus will start to tip over; this
happens when N 2 =f 2 =0,
N 1 =mg , f 1 =mhv 2 /R . Now we need to calculate
the torque about some axis and set it equal to zero, but
that axis must pass through the center of mass because the
bus is accelerating. Now, you need to know the height above
ground h of the center of mass and the distance 2d ,
between the left and right wheels. Doing that, the torque equation is (mhv 2 /R )-mgd =0
or R max,start =hv 2 /gd.
This is the radius at which the bus will just start to
tip. For smaller radii the inner wheels will
come
off the ground but the bus will not tip over until you
reach some critical smaller radius. So let's just guess that
approximate values of h and d are
equal at
about 2 m each: R max,start =v 2 /g =49
m=161 ft. This choice of h and d result in
the bus never tipping because it would slide before it
started to tip; to reach this point, f =μmg=mv 2 /R ,
μ= 222 /(9.8x49)=1.01.
Consider the bus when it has tipped through some angle
θ relative to the horizontal as shown in the second
figure. Now the moment arms to compute torques are D=d cosθ-h sinθ
for N=mg and H =h cosθ +d sinθ
for f=mv 2 /R . (I
must admit that it took me a while of floundering with my
trig to figure these out!) So now the torque equation is
mgD =Hmv 2 /R or, R=Hv 2 /(gD ).
In the graph below you can see that, for d=h , the radius gets
smaller and smaller as the tip angle gets larger; all these
calculations assume that the bus does not skid, but unless there is
something else besides static friction to provide the
centripetal acceleration it will likely skid before it tips. Note that if the bus tips until the center of mass is directly above
the outer wheels, where D =0 and θ= 450
for d=h , it is on the verge of
fully tipping over. The bus
will roll over when the angle it makes with the ground is greater
than tan-1 (d /h ).
If you manage to get the bus on two wheels and at the angle
just before it tips over you can go essentially straight
(making small steering corrections), not turning as the
video
linked to above. The bottom line is that a bus is extremely
unlikely to roll over in a turn because it will likely skid
before it rolls. I think my choices of d and h are very
reasonable and probably, because so much of the weight is in
the frame, suspension, axles, transmission, and engine of the bus, the center of gravity is
likely to be lower than 2 m making a roll even less likely.
It would be a different story for a train on tracks where
the "friction" is almost limitless because the train is
constrained by the track from moving sideways ("skidding")
at all.
does stop but only for zero time. But an engineer will have to take into account that a real pendulum might stick for a brief time, maybe a microsecond, at the extrema. But I cannot give you an answer to your question because the amount of stick time will depend entirely on the details of the construction of the pendulum.
(I believe that the main reason for sticking would be the
difference between static and kinetic coefficients of
friction.)
h , plays more roles than just
setting the smallest value of something. Most famous of this
role is that, if you have electromagnetic waves with a
frequency f , the smallest amount of energy, called
a photon, which
such electromagnetic waves can have is hf . But,
this idea of minimum amount possible does not extend to
everything, certainly not to something like the number of
digits in any irrational number like π . The idea
that something has a minimum value usually has to do with
what we call "fields"; when the electromagnetic field is
quantized, the photon is the "messenger" which conveys the
field.
More interesting, I believe, is the role played by Planck's
constant in the structure of systems of particles like atoms
or atomic nuclei. The great hypothesis by Niels Bohr that the
hydrogen atom can only exist in particular energies owes its
inception to the idea of quantization. He assumed that the
electron in a hydrogen atom moved in circular orbits but not
in any old orbit but only in those for which the angular
momentum was quantized, L=nh /(2π ) where
n =1, 2, 3, 4…; the angular momentum is the
product of the electron mass, the orbit radius, and the
speed of the electron. This led to quantized energy levels;
this model excellently explained everything known about the
hydrogen atom at that time. See the Wikepedia article on the
Bohr
model. (The Bohr model, while easy to visualize, is a
very simplistic and incorrect compared to the correct modern
quantization of the atom.)
If you think about it,
energy quantization is an astounding surprise. It is like
saying that a pendulum may have an amplitude of 50
or 70 but not 60 . But nature does hand
us surprises sometimes.
But energy quantization does not apply to everything. If a
system of particles is not bound together it can have any
amount of energy.
What
is not known but speculated about is whether space and time are
quantized. Is there a shortest possible distance? Is there a
shortest possible time? Nobody knows but speculations called the
Planck
length and the
Planck time
are extraordinarily small, far smaller than current measuring
capabilities.
Finally, look
at the following Q&A for another example of the role of Planck's
constant.
x
and linear momentum p , and the product of their
uncertainties cannot be smaller than the rationalized Planck
constant, h /(2π ). So, the more
accurately you measure either, the less accurately you can
know the other. Another pair are energy E and time
t . So, for example, if a radioactive system has a
half life of Δt , the most accurately you can
measure the energy is ΔE >[h /(2π )]/Δt .
F AB on object B,
object B exerts an equal and opposite force F BA =-F AB
on object A. F AB tends
to accelerate object B and F BA
tends to accelerate object A.
F AB on object B,
object B exerts an equal and opposite force F BA =-F AB
on object A. F AB tends
to accelerate object B and F BA
tends to accelerate object A.
These are two equations for two unknowns, v and
t , and can be solved using simple algebra. The
solutions are t =0.563 s and v =7.33 ft/s=5
mph.
v . There is no difference in the
"damage".
θ subtended by 300θ= 300/5000=0.06
radians=3.440 . Looking at the diagram, cosθ=R /(R+d )=[1+(d /R )]-1 ≈1-(d /R );
therefore d≈R (1-cosθ )=9 miles.
Now, you are probably thinking that all the sound waves move
in straight lines, that the sound waves coming from the
detonation are radiating out as shown in my second figure
thereby missing the earth's surface except very close to the
source. But, since sound is composed of waves, it is subject
to diffraction. Huygen's principle says that the wave a
short time later is determined by treating each point on the
wave front as a new point source. Finally, I have drawn one
of the wave fronts which is off the earth in the earlier
picture and how Huygen's principle predicts the wave a short
time later. Note that the wave where it originally ended is
now bending and lengthening; this is diffraction and allows
the sound to follow the contour of the earth. This is the
same principle where when you speak to someone on the other
side of a sound-absorbing wall with an opening in it (but
she is not visible to you), you can be heard just fine;
sound diffracts around corners.
mg f down which the upper
cube exerts on it in the direction of the flow, and the
force f up which the lower cube exerts on it opposite the
direction of the flow. Notice that all cubes exert pushing
forces on their neighbors, not pulling, so "sucked" is never
what is going on. Now, the cubes are flowing downstream with
constant velocity, so the sum of all forces in that
direction must add to zero (note that only the downstream
component of the weight is mg θ
pushes the water downstream): f up -f down -mg sinθ =0.
So, f up =f down +mg sinθ.
So, you see, gravity and the water upstream push the
water downstream while the water downstream tries to hold
the water back. There is a greater force upstream from the
water itself than there is a force downstream. Without
gravity or with no slope to the riverbed the water would not
flow at all.
Here is a nice explanation of how magnets are rated.
Here is a real-world example.
mg , that component is mg sinθ
where θ is the angle of the ramp, 100
in your case. The force pointing up the ramp which
must be applied is therefore mg sinθ.
Note that the speed is irrelevant.
earlier answer . I am sure that astronomers are perfectly
aware that masses will alter the position of the images they
observe relative to the objects they are observing are not
perfect. However, the position recorded is simply the
position in our sky at this time .
Positions of objects can change simply because they are
moving.
link .
Kind regards
lifts the airplane. Regarding
"scientific/reliable" and "uncredited/verified", I am not
writing an encyclopedia here where footnotes and references
are required. I am presenting myself as someone who has a
degree of expertise in physics who can answer questions
about the subject; it is your responsibility, since there
can be lots of BS on the internet, to convince yourself that
I do indeed have some physics credibility. To that end I
post information about myself, on the page
"The
Physicist" where you can get the information you need to
judge my qualifications. Incidentally, the reason I chose
the video which I did was because the Bernoulli aspect of
wing lift is presented as the whole story in a great many
introductory physics textbooks and only when I was taking
flying lessons years ago did I learn that "angle of attack"
is much more important in actually creating lift; I like the
way this video presented both of these important concepts.
t over which the
fish is accelerating and the change in linear momentum Δp =m Δv ; F =Δp /Δt .
In your case, the mass is m =1 lb=0.45 kg and the speed is
v =23
mph=10 m/s so the change in momentum is 4.5 kg⋅m/s if
the fish starts at rest and accelerates to 23 mph or
vice versa . I
will assume that the line does not break and then compare
forces with the pound-test of the line; then I will compare
with a four pound test leader. If your
rod had zero flex, was perfectly rigid, the fish would be
unable to move at all unless the line broke, so assuming
that he could exert a force of four pounds or more which he
probably could, you would lose that fish. If he hit the fly
going 23 mph and stopped in 0.1 seconds, the average force
would be 4.1/0.1=41 N=9.2 lb—bye bye fish! But, that is unrealistic because
what really happens is that the rod bends and what that does
is lengthen the time the strike lasts; that means that the
force on the line will be smaller. Suppose that it takes 2 s for
the fish to get up to his maximum speed while hooked; during
that time the average force exerted will be 4.5/2=2.25
N=0.51 lb, and you have caught that fish. Now you understand
why fishing rods are designed to bend.
3 .
The closest metal to this is germanium with a density of
5.32 g/cm3 ; but germanium is brittle and would
not be pliable. Lead has a density of 11.34 g/cm3
and silver 10.49 g/cm3 , both about twice as dense
as your sample. So it must be something else. To sort it out
would require a chemical analysis, I guess.
R=v 2 sin(2θ )/g
where R =130 ft, v is the speed, θ is the
launch angle, and g=32 ft/s2 is the gravitational
acceleration; the "optimum" launch angle is 450
for maximum range. So v =√(130x32)=64.5
ft/s=44 mph. For a smaller launch angle the speed would be
larger; e.g . at 300 , v =50 mph.
earlier
answer . The issues you raise could mostly be handled by
making a judicious choice of target. Stellar evolution is
reasonably well understood and the life time and age of a
star could be decuced from its properties. For example, if
the star you have in mind is within a million years of
running out of fuel and is a million light years away, it
would foolish to plan a journey there. Regarding distortion,
the earlier answer emphasizes that problem but the most
important distortion is that caused by the high speed of the
vehicle itself; "distortion" due to motion of the target
star itself as well as gravitational lensing could be
adjusted for in flight if you could actually see and lock
onto the star at high speeds. Your last question has no
answer because you need to specify how small a lag you would
call "current"; we are quite close to the sun but light from
it takes about 8 minutes 20 seconds to get to us.
(To give a background on why I asked the question. I have a habit of clicking my pens on my desk so they shoot a few inches into the air. I always try to catch them right at the height of their motion. I started wondering how long I actually had to do that. When I asked some engineering friends they said the pen instantaneously goes from traveling up to falling down. I’m not sure if that’s true but if so it introduces a bit of a crisis. If the pen spends zero time at its maximum height, is it ever actually there? And would I ever be able to actually catch it at is maximum height? Can something be somewhere but spend zero time there?)
To get more technical, what is the probability of finding
the object at a particular point? It is zero. That is
probably what is bothering you. So you could ask for the
probability of catching the pen during the interval 1/1000th
of a second before and after the zero speed time. I will not
get into quantum physics here, but you cannot know precisely
both the speed and location of your pen at any time; but
this truth implies an incredibly small uncertainty,
certainly not important for a macroscopic object like your
pen. One final thought, we do not know whether or not there
exists a shortest possible time or length, sometimes
referred to as the Planck length and the Planck time; if it
exists, the Planck time is expected to be about 5x10-44
s, so perhaps your pen stands still for that time!
faq page .)
2 until they get all the
way to the ground. The air drag is a force on the falling
object upward (opposite the velocity) which gets bigger as
the object falls faster; eventually the drag force becomes
equal in magnitude to the weight which is a force down, so
the object falls with constant velocity after that. That
speed is called the terminal velocity and that depends on
both the mass and the geometry of the object. The speed of
120 mph is the approximate terminal velocity of a falling
person. A bowling ball would have a much larger terminal
velocity and a feather a much smaller one. If the earth had
no atmosphere, anything would continue accelerating until it
hit the ground. If you want to learn more about air drag,
you can find links to many of my older answers on the
faq
page . If there were no air in the hole you want to drill
and the earth were a uniform sphere (which it isn't), the
speed would be about 18,000 mph at the center.
etc .
Is a block of iron a "different type" of solid from a block
of tin? Yes. Similarly, a plasma composed of iron ions is a
"different type" of plasma than one composed of tin irons.
v . I will assume that the time which the
collision lasts, Δt , is the same for any situation
I consider. There will be two extremes for a collision—perfectly
elastic where energy and linear momentum are conserved, and perfectly inelastic
where the objects are stuck together after the collision and
energy is not conserved but linear momentum is. The impulse
received by the object originally at rest (your opponent) is
equal to the linear momentum he has after the collision and
is equal to F Δt ; since I specified that Δt
is the same for all collisions, the force experienced is
F=mv' /Δt , where v' is the speed of the struck
object after the collision. First consider a collision
between two equal masses m . For the elastic
collision the incoming mass is at rest after the collision
and the outgoing mass has a speed v ; for the inelastic
collision both masses (stuck together) have a speed ½v .
Therefore the force experienced by your opponent is given by
½mv /Δt ≤F ≤mv /Δt .
Now suppose that your mass M is much larger than your
opponent's mass m , M>>m . In this
case, the inelastic collision will have both objects moving
with approximately a speed of v ; the elastic
collision will have M moving
approximately with the speed v and m
moving approximately with the speed 2v . Therefore
the range of possible values for F experienced by
m is mv /Δt ≤F ≤2mv /Δt ,
which is twice the force for equal masses. So my simplistic
view is that being anchored to the floor is like increasing
your mass allowing you to deliver more impulse to your
opponent as compared with if you are flying toward him which is
more like the collision of equal masses. As I said, it is
much more complicated than this but this might give a little
insight. I would welcome any comment on this treatment.
(Lengthy enough answer for you?)
that direction.
2 )=102,900 N
and the total area is (4 m)x(7 m)=28 m2 . So the
pressure is 3675 N/m2 . Other units used for
pressure which you might prefer are 375 kg/m2 or
76.75 lb/ft2 .
earlier answer (skip down to the
last paragraph ).
p =q d q separated by some distance
d ; imagine these as vibrating
sinesoidally along the direction of the vector d p p here .
Brief Answers to Big Questions ) it is stated that a chemical rocket with a thrust velocity of 3 km/sec, that jettisons 30% of its fuel, attains a velocity of 'about half a km/sec'. Using
Tsiolkovsky's rocket equation I get a value of 1.07 km/s.
Have I made a mistake?
earlier answer , v=u ln[(M+m )/M ]
where M+m is the initial mass, m is the
fuel burned, u is the exhaust speed, and v
is the speed acquired by the rocket. So I find v=3ln(0.7-1 )=1.07
km/s. I do not know how Hawking came up with his answer, but
it might hinge on what he means by "30% of its fuel"; you
and I have interpreted that to mean the exhausted fuel has a
mass equal to 30% of the mass of the rocket before the fuel
was burned, hence M /(M+m )=0.7. Also, maybe
he was thinking about a launch from earth which would
require some of the energy from the rocket to overcome the
gravitational force and the energy loss from air drag. Or
maybe he was guesstimating the effects of efficiency of the
engines. In any case, you did not make a mistake.
0 C, if the air
in the bottle chilled to that temperature, the pressure in
the bottle would be smaller than 15 psi. Using the
Gay-Lussac Law, P /T =const., I find the
pressure would be about 11 psi, a net of about 7 psi. (If
you want to check this, you must use absolute temperature,
not 0 C.)
FAQ
page you will find many links to earlier answers which
relate to this.
laminar
which means that if you focus your attention on a small
volume of the fluid it will move along a smooth line and be
followed and preceded by many other small volumes following
the same smooth line. Under other circumstances, the fluid
will become turbulent , moving chaotically. So
something happens which causes the smoke from your incense
stick to change from laminar to turbulent at some point.
This is usually quantified by a dimensionless variable
called the Reynolds' number, Re=ρuL /μ
where ρ is the density of the fluid, u
is its speed, L is a length which describes the
geometry, and μ is the dynamic viscosity of the
fluid. So, Re changes in such a way that the
original laminar flow becomes turbulent after rising a
certain distance from the source of the smoke.
a
or in zero field but having a uniform acceleration a ;
buoyancy would be observed in an accelerating rocket ship in
empty space.)
E i A =½mv i 2 +mgh ,
E f A =½mv f 2
and so v f =√(v i 2 +2gh ).
Exact same calculation for E B .
d =0 in your (simplistic) W=f x
d definition of work. If the saucer is rising with a
constant speed v, then when it has gone some distance d, the
thrust T has done W saucer =Td
and gravity has done work W gravity =-mgd
because T=mg for it to be rising with constant speed. The
net work W on the saucer is still zero, W =W gravity +W saucer =0.
Your last question "…simply converts KE to PE…"
is again using PE unnecessarily. Gravity does work on an
object as it falls because there is a force mg
acting down.
This is the most popular way to explain the answer without
resorting to very opaque mathematics, but I find it just a bit
unsatisfying even though it is certainly correct. I found a more
convincing argument put forward by Eltjo
Paselhoff on the website
quora.com . Suppose we plot the velocity v as a
function of time t for the upward trip. At t =0
the magnitude of the slope must be larger than g
because the air drag is slowing the ball down as well. As the
ball gets higher, its speed decreases so the air drag gets
smaller so that finally at the top of its trajectory it is at
rest and the magnitude of the slope is equal to g . Now,
the ball falls back down and speeds up because air drag is
smaller than weight; eventually, though, the two forces become
close to equal and the speed becomes constant at the terminal
velocity v T . One more thing you must
understand now is that the area under the velocity curve is the
distance traveled by the ball, so since up and down go the same
distance the green and red areas need to be the same. The only
way this can be is if the time to fall is larger than the time
to rise.
F - F f F
web site which gives the details of the
solution of the physics problem but is still quite readable.
For the casual reader, I will include here an overview.
Newton's second law is an inhomogeneous second-order
differential equation. What makes the equation inhomogeneous
is the presence of the driving force, the signal your
amplifier sends to the speaker; with no driving force, the
solution of the problem would be x t (t )=A t e-γt ωt+φ t )
where ω is the natural frequency the speaker
would vibrate with on its own, γ is a parameter
which describes the damping of the speaker, and A t
and φ t are constants
determined by the initial conditions. If the
driving force is present, F=F 0 cos(ω 0 t +ψ ),
the solution is a linear combination of the what is called
the steady state solution , x s (t )=A s sin(ω 0 t+φ s ),
and the solution for the undriven oscillator x t (t )
which is referred to as the transient solution: x t (t )=A t e-γt ωt+φ t )+A s sin(ω 0 t+φ s ).
The constants A t and φ t
are determined by the initial conditions (speed and position
of the speaker) and the constants A s and
φ s are determined by the driving
force (F 0 and φ t ).
Because of the damping term e-γt
Below are shown a couple of examples:
These show the total displacement for different initial
conditions. In both cases the speaker started at rest. The first
shows the starting position at zero, the second shows the
starting position at 0.5. The important thing is that they both
end up, after the transient has died, as the same.
0 . I found a
little
calculator you can play with; a screenshot is shown
below. All you would need to vary are the velocity, the
angle, and the height of the dock. I found that if I chose
the initial speed to be 26 ft/s (about 18 mph) the distance
the dog would go for a 450 jump would be about 21
ft from a zero-height dock. Now, when I do the calculations
for the 24 in=2 ft and 16 in=1.33 ft, I find the best angles
and distances (for 26 ft/s) are (43.50 , 22.9 ft)
and (42.50 , 22.3 ft), respectively. All in all,
there is just about no difference.
Note that I have not included any air drag. I believe the speed
of the dog is low enough to make drag negligible.
D is hinged to a wall. A force F T d from the hinge; we would find
experimentally that if T =F (D /d )
the stick would not rotate. We would conclude that the net
torque about the hinge is now zero and that this torque
changes linearly with the distance. Of course, the torque
exerted by F T τ=FD-Td= 0.
This is not the most general case but I feel you wanted to
be convinced that torque depends on where the force is
applied relative to an axis about which you are computing
torques, which was easy to see.
first and
second times. In a nutshell, if there is not air moving
over the wings with sufficient speed, there is not
sufficient lift on the airplane for it to leave the ground.
I agree that Mythbusters'
version of this is not the same as I understand your
question and previous questions where whatever the conveyer
is doing, the plane is not moving forward through the air;
the Mythbusters have the conveyer at rest relative to the
plane but moving forward with the same speed as the plane,
so the wheels are not spinning.
I guess it is possible
that a propeller plane could take off from rest since the props
send a wash of air over the wings, but probably not unless there
were a pretty hefty headwind; you do see some planes, designed
for flying into and out of tight places, which take off in a
very short
distance.
Let's just call a truce on this whole thing. A 747 at rest for
any reason is not going to take off. And practical problems with
the fabrication and utilization of this stupid treadmill will
ensure that it is never constructed or tested.
L a distance d from where you are viewing
it. You can see that the angle subtended by the moon is 31
arcminutes≈0.520 . The angle is expressed in
radians as θ=L /d. To convert that to degrees,
multiply by 180/π , so θ= (L /d )x57.3
in degrees. For example, your 19 km dreadnought 100 km away
would have θ =10.90 , about 21 times
larger than the moon.
earlier answer which answers
the same question except for the earth-moon and sun-earth
pairs. For your question it is the electrical force which
holds the electron in its orbit. There is an important
difference, though. The electron-proton system, if you look
at in classical electromagnetic theory, should radiate
energy (it is essentially a tiny antenna) and fall into the
proton. This does not happen; the reason is that for such
small systems classical physics does not work and this was
one of the milestones of physics when Niels Bohr proposed
his model
of the hydrogen atom where certain orbits simply did not
radiate. To understand the details of quantum mechanics,
which eventually evolved from the Bohr model, would require
a much longer explanation.
etc . For
a more detailed explanation, see
this link .
Rutherford scattering ) does result in the
angular momentum of the moving charge q about an axis passing
through the fixed charge is conserved. It is not hard to
understand. What is the condition for which angular momentum
is conserved? There must be no torques on q . The
expression for torque is τ r F qr xE r E
r and E r E q and its
angular momentum will remain constant.
Wikepedia : "Gravitational waves carry energy away from their sources and, in the case of orbiting bodies, this is associated with an in-spiral or decrease in orbit. Imagine for example a simple system
of two masses—such as the Earth–Sun system—moving slowly compared to the speed of light in circular orbits. Assume that these two masses orbit each other in a circular orbit in the
x–y plane. To a good approximation, the masses follow simple Keplerian orbits. However, such an orbit represents a changing quadrupole moment. That is, the system will give off gravitational waves.
In theory, the loss of energy through gravitational radiation could eventually drop the Earth into the Sun. However, the total energy of the Earth orbiting the Sun (kinetic energy + gravitational potential energy) is about 1.14×1036 joules of which only 200 watts (joules per second) is lost through gravitational radiation, leading to a decay in the orbit by about 1×10−15 meters per day or roughly the diameter of a proton. At this rate, it would take the Earth approximately 1×1013 times more than the current age of the Universe to spiral onto the Sun. This estimate overlooks the decrease in
r over time, but the majority of the time the bodies are far apart and only radiating slowly, so the difference is unimportant in this example."
So the answer is that the energy comes from the orbiting
earth which causes its orbit to get smaller as it loses
energy; however, as the calculation shows, the loss of
radius of the orbit is trivially small.
c where c is the speed of
light. In order to see the effect which I think interests
you, you need to choose a much larger much larger speed for
the rocket; I will choose v =0.8c , 80% the
speed of light. I will choose my unit of length to be one
light hour and my unit of speed to be light hours per hour,
so c =1, v =0.8, and L =1. First,
look at what an earth-based observer will measure with his
clock. If t is the time when the light
arrives at the rocket, then vt =0.8t =x and
ct=t =(L-x )=(1-x ); solving, x =0.8/1.8=0.444
and t=x /0.8=0.556. Also, note L-x =(1-x )=0.556.
But, what you asked for is how long a clock on the rocket
takes to see the light. The important thing is that the
distance between the earth and the satellite is not 1 light
hour any more, it is length contracted such that the
distance seen for L by the rocket is L'=L √[1-(v /c )2 ]=0.6
rather than 1. Of course the same factor occurs for x' =0.6x =0.267
and the time this happens is t'=x' /0.8=0.333
because even though the distance to the satellite is
shorter, it still zips past the rocket with a speed of 0.8c .
Finally, c' =(L'-x' )/t' =(0.6-0.267)/0.333=1!
So, you see, c really is the speed seen by all
observers.
relative to what . As a concrete
example, suppose that you throw the bottle with a velocity
of 20 mph relative to you (the speed you would throw it if
you were at rest on the ground). But you are are at rest
relative to the car, so you and anybody else in the car
would see it moving forward with a speed of 20 mph. But
someone by the roadside would see it moving forward with a
speed of 70 mph. Somebody in a car going in the same
direction as you with a speed of 70 mph would see the bottle drop
straight down to the ground (no horizontal velocity). If you
threw it backwards (relative to the direction of your car)
with a speed of 50 mph, someone by the roadside would see it
drop straight to the ground (see a
Mythbusters episode).
-29 g/cm3 ,
so it isn't even close.
https://www.bbc.com/news/science-environment-47873592
Why this cannot be done by one single telescope and how the group of telescope functions in order to work (I cannot think why it needed so many to be focused in a single point). Also the earth is rotating so most of them are not aligned with the point of focus.
Second question is why we only have an image? if we can take a photo, we can surely take more photos and create a video. In that way we can see the moving plasma or whatever is there.
-3 m wavelength; this
wavelength is expected to originate only from the accretion
disk-7 m. Increasing the
size of a telescope gives it better resolution, so the size
S for a millimeter telescope comparable to the best
optical telescopes would be S =10-3 (10/5x10-7 )=20,000
m=10 km; but, looking at an object so far away (55 million
light years) would be impossible for visible light, but
since the earth has a diameter of about 13,000 km, we can
get very much better resolution with a large millimeter
telescope array by having the individual telescopes have
separations comparable to the size of the earth. Although the size is very
huge, the total area of all the radio telescopes is
extremely
small, so trying to make an image would be like blacking out
99.999% of the mirror in an optical telescope—you
would still get an image but you would have to wait a very
long time. So the data from all the telescopes in the array
were gathered over many hours during a 10 day observation
period. Then, all the data had to be put together using a
computer to reconstruct the image; the data analysis took
two years to complete, a very difficult problem.
Finally, you should ask what the dark circular region in the
center is—it is not the black hole itself which has
zero size. The outer edge is what is called the photon
radius, the distance from the black hole where a photon will
orbit. Somewhere inside of the photon radius is the event
horizon, the sphere inside of which nothing, including light
can escape.
A warning: as I clearly state on the site, I do not usually
answer complex questions in
astronomy/astrophysics/cosmology, so take what I say with a
grain of salt!
L was quantized, L=n ℏ where ℏ
is the rationalized Planck constant. This was actually
wrong, but it gave the right answer for the spectrum of
light observed from a hydrogen atom and that was a great
leap forward; but purely empirical. Improvements
and
extensions of this model were made, but they were all
equally empirical. Still, this first empirical model set
everyone on the right track to achieve a more fundamental
model. During this time, it was beginning to be understood
that trying to imagine a model based on classical ideas,
ideas like an electron orbiting in a circular orbit, were
invalid at such tiny scales—that realization ultimately gave
rise to the development of quantum mechanics. You can no
longer even think of an electron as a little point charge
when it is bound in an atom. Rather, you solve an equation,
known as the Schrodinger equation, which gives you a
mathematical function, called the wave function, which tells
you the likelihood of finding the electron at any particular
place in space. So the best way to think of an electron in
an atom is akin to picturing a cloud over which the electron
is smeared. The shape of this cloud is dependent on four
quantum numbers which quantize the energy, the angular
momentum, the projections of the angular momentum and the
spin angular momentum on some axis. Some examples are shown
in the figure. To visualize the "clouds", imagine rotating
each around a horizontal axis through the center; so, e.g. ,
the upper right cloud is donut-shaped.
ground rules , you would have seen that "I no longer answer questions which are based on premises like:
'...if we could travel faster than the speed of light...' or
'...ignoring the fact that nothing can go faster than the speed of light...',
'...if I were traveling at the speed of light...', etc."
Suppose that you were traveling at 99.99% the speed of
light. The light which you would see if at rest would be
visible, but in your moving frame the wavelength would be
Doppler-shifted to a longer wavelength, into the region of
far infrared which your eye cannot detect.
241 Am. In addition to
the four energies of alpha particles there are gamma rays of
energies up to about 100 keV. I cannot explain why water is
the least absorptive than any other material you tested.
here , the
second is linked to from that answer.
F =m a
In rotational physics, moment of inertia I plays
the role of mass and angular acceleration α F r τ r x F τ Iα .
I do not know much about engineering notation semantics but
if what you say is correct, that torque means that which is
zero if the object is not rotating at all (or with a
constant angular velocity), then that is what would be
called net torque in physics which seems to make
more sense to me. According to Wikepedia, mechanical
engineers (and also British physicists) refer to (physics)
torque as moment of force , not torque moment as you
state. Similarly, the definition by mathematicians is that
torque is equal to the rate of change of angular momentum
which is exactly the same as τ Iα
and so torque, again contrary to your
statement, is the same as in physics. So, I read the
Wikepedia article differently from you and, to me, there is
no difference in anybody's definition of what I would call
torque other than semantics. And I read nothing there which
implies that the word torque means the sum of all moments of
force to an engineer. So my final answer is that everybody's
definitions of the physical quantities are the same, only
the words used to label them differ.
Why doesn't the moon fall to the earth?
the volume of a sphere of radius R is 4πR 3 /3;
the cross sectional area A of a sphere of
radius R is πR 2 ;
the air drag force on an object having speed v
is proportional to Av 2 ; and
the terminal velocity U of an object of mass
m is
proportional to √(m /A ).
I
will use subscripts 1 and 2 to denote the original and final
drops, respectively; so m 2 =2m 1 and
R 2 /R 1 =21/3 .
Therefore, A 2 /A 1 =22/3 .
Finally, U 2 /U 1 =[(m 2 /m 1 )(A 1 /A 2 )]1/2 =[2⋅ 2-2/3 ]1/2 =21/6 .
So, finally, U 2 =10⋅ 21/6 =11.22
cm/s.
R with the current
I distributed uniformly throughout the wire. The
figure shows the field due to the wire, the vector
B having a constant magnitude at a
distance r from the axis of the cylinder defined by
the wire and always tangential to the circle of radius r
around the wire. Hence field lines, as shown are circles,
the direction defined by the right-hand rule as shown. The
magnitude of the field is determined by Ampere's law,
∫B ⋅ ds μ 0 I enc
where the integration
is all the way around the path defined by the circle and
I enc is the amount of current which passes
through the area defined by that closed path. Given the
cylindrical symmetry of this special case, the integral is
simple because B is constant and B s
∫B ⋅ ds πrB=μ 0 I
so Br>R =μ 0 I /(2πr )
for r>R . This is only correct outside the wire
itself because the integration path to determine B
inside the wire encloses less current. Inside, I enc =I (r 2 /R 2 )
so Br<R =μ 0 Ir /(2πR 2 )
for r<R. Note that when r=R both results
give the same value of B , B =μ 0 I /(2πR ).
So, the field increases linearly with r inside the
wire and decreases like 1/r outside.
The questioner also
wanted to express this in terms of the velocity
v Q=-e and having a density of
n
electrons/m3 . The fact that the electrons have
negative charge means that, in the figure above, the
direction of v t the
electrons go a distance ΔL and so sweeps out a
volume ΔV which contains a total charge ΔQ =-ne ΔV =-ne ΔL (πR 2 I =ΔQ /Δt=-ne (ΔL /Δt )(πR 2 )=-nevπR 2
v in a cylindrical beam of radius R . The second part of my answer showed you how to relate
I in the first part of the answer to the charge, speed, density of charges, and
R . So the quantity you seek results from setting
I=nQvπR 2 into
B=μ 0 I /(2πR ) (assuming that "adjacent" means right on the edge of the moving charge distribution).
In the first case the two electrons are very close together and are moving to the right at say 50 m/s, what would be the
"B" field be 50 mm directly above, i.e. in the positive y axis above these electrons?
In the second case, same two electrons traveling to the right at 50 m/s but this time they are separated. Call the first electron,
"e1"and the second "e2".
The first electron e1 is located directly 1 mm below the point of interest where I want to calculate the combined
"B" field. The second electron e2 is located directly 98mm below e1 or 99 mm below the point of interest where I want to determine the combined
"B" field. In effect from the first case I have moved e1 closer to
"B" by 49 mm and e2 farther away by 49 mm.
I was using the formula B=μ 0 NqV /(4πR 2 ) where
μ 0 is permeability of free space, N is the number of charges, q is charge on an electron and V is the velocity of the electrons, R is the vertical distance between the charges and the point of interest for
"B" the strength of the magnetic field.
B R B V B=μ 0 Nq V R πR 3 );
note that the magnitude of V R VR sinθ where θ is the angle between
V and R θ =900 , your equation is correct. Be
careful, though, because the direction matters when you are
adding vectors from two sources; the case you are looking at
has the point the same side of both electrons so the
magnitude is the sum of the magnitudes, but if you look at a
point between the electrons, the magnitude will be the
magnitude of the difference. The form of Ampere's law which
I used in the earlier answer is simply not applicable in
this situation because making reference to a current I only
makes sense in magnetostatics. Finally, I should note that
all this is only approximately correct when you are in a
nonrelativistic regime which you certainly are for V =50 m/s.
twin
paradox (I have attached here the figure from that post for
your convenience) which shows how the traveling twin "sees" how the
earth clock runs by having the earth-bound twin send him one
message per year; this is different from your situation where
essentially a daily rather than an annual message is sent, but
the ideas are identical. When he arrives home, the traveling
twin has "seen" the same number of years (days) on earth pass as
the earth-bound twin has but, as you can see, a different number
of years (days) have passed on his on-board clocks. "Watching"
some clock in another frame of reference is not in any way
relevant to time in your frame; the traveling twin would count
his birthdays using his clock, not earth's clock. Note also that
the traveling twin "sees" the earth spinning very slowly on the
trip out but spinning very rapidly on the trip home.
mv 2 ,
so it is natural to think that the maximum possible kinetic
energy would be ½mc 2 . But
Newtonian physics is not valid at speeds close to c ,
and in relativity the kinetic energy is ½mv 2 /√[1-(v 2 /c 2 )].
To learn more, see an
earlier answer to the same question; you might also look
at the answer following that one.
earlier answer . Spin is nothing more than a
specification of the angular momentum of a system; e.g. ,
the spin quantum number of an electron, proton, neutron, and
other so-called fermions is s =½. The actual
angular momentum is given by S =ℏ√(s (s +1))
where ℏ is the rationalized Planck's constant. Usually, we think of spin
as the intrinsic angular momentum of an elementary particle
or entire quantum system like an atom; particles may also
have orbital angular momentum, for example an electron
orbiting around a nucleus in an atom. But each angular
momentum will be quantized (have a specific quantum number)
and the total angular momentum J of any angular
momentum number j will be J =ℏ√(j (j +1)).
Orbital angular momentum quantum numbers are integers rather
than half integers like electrons; so, an electron in a
"p-orbit" in a Bohr atom has an orbital quantum number 1 and
a spin quantum number ½. As to where the idea came from,
there were several things which suggested it. The experiment
which showed that spin of an electron was the
Stern-Gerlach experiment , but there were also hints from
spectroscopy and, notably, that there were twice as many
states in quantum systems (like atoms) as expected from the
Pauli exclusion principle .
0 relative to the normal of the plane
of its orbit but that axis precesses around the
perpendicular axis about once every 26,000 years. This
precession is caused by torques exerted on the earth by the
sun and the moon. Currently the axis is pointing almost
exactly to the the north star, Polaris; however, in a few
thousand years there will be some new star taking that role.
The last ice age was about 2.4 million years ago and lasted
much longer than 26,000 years, so the answer to your
question is that it pointed many directions during the ice
age. You are asking about the geographic north pole which is
essentially constant in its location (although the land
masses move over the surface because of plate techtonics).
The gravitational north pole, though, is forever wandering
around and has actually jumped to the southern hemisphere
around Antactica and back many times.
My third
book , PHYSICS IS … The
Physicist Explores Attributes of Physics , has a chapter
titled Physics Is Beautiful , devoted to beauty and
elegance. However, I have never thought of it as art. A
sunrise over the Sangre de Christo mountains is beautiful
but you would certainly not call it art. I found that it is
impossible to find an unambiguous or not vague definition of
art; art is qualitative which sets it apart from science
which is quantitative. And, consider this: There are many
paintings of the of Chartre Cathedral, four of which I have
copied here, and all are indisputedly art; there is no
"correct" painting of this subject. The theory of
electromagnetism, on the other hand, is beautiful and the
only one of its kind; you might think up another
electromagnetic theory, but it would be wrong even though it
might be considered very imaginative, creative, even
beautiful. There is no well-defined test which specifies
which painting is the best; there is a test as to which is
the theory of electromagnetism —it must
quantitatively describe what really happens in nature and if
it fails to do so, it is false. I have always thought of
string theory as not a theory (and not beautiful) because it
makes no attempt to quantitatively interface with the real
world and is therefore not falsifiable.
F=- μs N
(negative because the force is opposite the velocity. where
μs is the coefficient of static
friction between rubber and dry asphalt which is about
0.5-0.8, and N is the normal force of the truck on
the road which, on level ground, is the weight; I will
choose μs = 0.65, halfway between the
extremes. At this point I will switch to SI units which
scientests prefer: weight N =7,200 lb=32,027 N, mass
M =32,027/9.8=3,268 kg, and speed v =45 mph=20.1
m/s. Now, using Newton's second law, F=Ma =- μs N ;
so acceleration a =-6.37 m/s2 . Now, you
can compute the time to stop: v =0=v 0 +at =20.1-6.37t,
so t=3.16 s. Finally, the distance traveled is d =v 0 t +½at 2 =20.1x3.16-½x6.37x3.162 =31.7
m=104 ft. It is interesting that this answer is independent
of how heavy the truck is. The reason is that the
acceleration is proportional to the weight/mass which is
just 9.8 m/s2 .
-5 s and the
acceleration is about 2.3x107 m/s2 .
The corresponding force to stop the beanie baby is
F=ma=.0128x2.3x107 ≈3x105 N≈67,000
lb. I think that if the beany baby hit you anywhere except
possibly your limbs, you would be killed. Keep in mind that
this is a very rough calculation, but certainly in the right
ballpark.
V= 4πr 3 /3 is
the volume of a sphere and if it is increasing with a constant rate dV /dt=C ,
then C =4πr 2 dr /dt .
Solving, dr /dt=C /(4πr 2 ) which is velocity at which the
surface is expanding.
So the acceleration of the surface is (d2 r /dt 2 )=-[2C /(4πr 2 )]dr /dt=- 2C 2 / [(4π )2 r 5 )] or, combining all constants,
kr -5 . I just don't see if the radius of the
sphere is expanding at a rate of Cr -2 , how it is accelerating at kr -5 ?
k is k =- 2C 2 / (4π )2 .
I think that the problem you are having is that you have
carried the minus sign into your constant. But that minus
sign is important because it tells you (since everything
else in k is constant) that the radius of the surface is
increasing, but the rate at which it is increasing is
decreasing as r changes. So, if the volume of
a sphere is increasing with a constant rate, its radius is
increasing like 1/r 2 , but the rate at
which the speed of the surface is decreasing goes
like 1/r 5 .
recent answer
is very similar to yours.
here . For example, for your current weight, a 5K race at
3.1 mph (which is about equal to 5 km/hr, so it takes one
hour for you to complete), I find "You burned 1151 calories
on your 5 kilometer run. At that pace, your calorie burn
rate is 230 calories per mile and 1151 calories per hour."
Sorry, I could not find any information on temperature and
humidity.
v Mv 2 .
where M is the mass of the universe except for your
mass. And just a minute ago that energy was not there.
Obviously, the total energy of that universe cannot be the
same in all frames. But, if you stay in one frame and keep
track of the total energy of the universe in your frame, it
will not change.
g 2 . The acceleration due to gravitation does
vary at various places on the earth. The animation shows you
how it varies. The variation is small, no larger than 50
milligals; a gal is 1 cm/s2 =0.01 m/s2 ,
so 50 milligal=0.005 m/s2 . So, compared to 9.8
m/s2 , the variations are only on the order of 0.05%. There
are several reasons for gravitational variations, notably:
altitude (the farther you are from the
center of the earth, the weaker the gravity);
local geology (large volumes of more
dense earth will increase the gravity);
the earth is
not a perfect sphere.
If you want a lot
more detail, see the
Wikepedia article on the earth's gravity.
N =0.001, N would be the number of
seconds it would take for the intensity of the light to drop
to 0.1% of its original value. Using
Wolfram Alpha , I
find N
f in water is a
quadratic
function of the velocity v , f= ½ρw CD Av 2 , where
ρw = 103
kg/m3 is the density of water, A
is the area presented to the onrushing water as the
object falls, and CD is a constant which depends on the
geometry of the object, called the drag coefficient. For a sphere of radius R
the drag coefficient is given by CD =0.47 . The upward force f is
only one force on the object as it sinks; it also has a
weight down W=mg and a buoyant force up B=Vρw g
where V =4πR 3 /3
is the volume of the sphere. If the sphere is
solid and has a density ρ=m /V , we can
write B=mg (ρw /ρ ).
Also note that we can write R as R =3 m /(4πρ )].
Finally, we can write the total force on a sphere: F =[mg (ρw -ρ )/ρ ]+½ρw CD Av 2 .
Note that when a speed is reached where F =0, the
sphere will fall with a constant velocity called the
terminal velocity, vt =√{[mg (ρ-ρw )/ρ ]/[½ρw CD A ]} .
So, let's do a specific example to be able to answer your
question for a particular situation. Suppose we have two 1
kg balls of solid iron for which ρ= 7.87x103
kg/m3 . Then the radius of each ball will be R =0.0312
m. Doing the arithmetic, F =-8.56+0.72v 2 .
So each of two balls of mass 1 kg, tied together will
accelerate until their speeds would be vt =F =-17.1+1.14v 2 .
So one ball of mass 2 kg will accelerate until
vt =√(17.1/1.14)=3.87 m/s.
You could do more examples to come to the conclusion that
the answer to your question is that, in general, two spheres
tied together will not sink at the same rate as one sphere
with their combined mass. I am sure, by carefully tailoring
the shapes of the objects, you could force the rates be the
same, but that is not you would find in general.
f can be approximated as f ¼Av 2
where A is the area presented to the onrushing air
and v is the speed. (You will note that Av 2
is not the same dimensionally as a force; this approximation
only works if you work in SI units, A in m2 ,
v in m/s and f in N.) So the net force
F on each ball (which I assume to be solid) is F =¼Av 2 -mg
where m is its mass; and, by Newtons second
law, the acceleration a is a =(¼Av 2 /m )-g ;
and there is a velocity U , called the terminal
velocity, at which the drag equals the weight so the
acceleration is zero and U= 2√(mg /A ).
Iron and aluminum have different densities, but it is pretty
straightforward to compute the radii of each
ball and from that compute A for each. I find A Fe =0.014
m2 and A Al =0.0064 m2 .
The accelerations are a Fe =-(9.8-3.5x10-4 v 2 )
and a Al =-(9.8-1.6x10-3 v 2 ).
At any given speed the magnitude of the acceleration for the
iron ball is larger than for the aluminum ball. The terminal
velocities would be U Fe =170 m/s and
U Al =78 m/s. The iron ball always has a
larger speed than the aluminum ball and will hit the ground
first.
It is also enlightening to find the distance traveled as a
function of time, s= (U 2 /g )ln(cosh(gt /U )).
This may beyond your math ability (ln is a natural logarithm
and cosh is a hyperbolic cosine), but the graph shows the
behavior of each ball and clearly the iron ball is falling
faster. Note that for the first few seconds (6 or 7 s) the
balls pretty much keep pace with each other and after about
15 s both have nearly reached their respecitve terminal
velocities because the curves are nearly linear.
When this kind of problem is
presented as an exercise in elementary physics, it is
usually assumed that the density of the earth is uniform
throughout—a cubic meter of earth from the surface has
the same mass as a cubic meter at the center. In this case,
it is easy to show that the acceleration due to gravity,
g (r ), is linear: g (r )=9.8(r /R )
m/s2 where r is the distance from the
center and R is the radius of the earth. Since the
acceleration is always toward the center, you speed up until
you reach the center (not decelerate as you suggest) and
then slow down until you reach the other end, neglecting any
frictional forces. More realistically there will be at least
air drag which will get bigger as you speed up until you
eventually reach a constant speed; then at the center, you
start slowing down until you stop somewhere before the other
end. Then you speed up back to the center getting there with
a smaller speed than the last time you were at the center,
etc. eventually stopping at the center as
k =9.8/R
N/m.
But, the earth is not a uniform
sphere. The core is much denser than the mantle and
therefore the acceleration is not a nice linear function.
The figure shows that the acceleration is almost constant
until about one third of the way to the center. The above
qualitative description of your motion remains the same
except for the similarity to the simple spring.
mg )
decreases linearly to zero at the center. In the realistic
model, the weight remains constant for a while, then increases
slightly, then falls almost linearly to zero at the center.
First, though, let me
address your reference to the ball being "heavier" or
"lighter" depending on the spin on the ball. This is totally
incorrect as the ball always has the same weight, a force
which points vertically downward. The way that the ball
moves results from the forces which the ball experiences
after it leaves your racquet; there is the weight straight
down, the force the ground exerts on it when it hits, and
the forces which the air exerts on it. The figure above
shows a ball with top spin; the top of the ball is spinning
in the same direction as the ball is moving to the right.
(If you are confused, the diagram is shown in the frame of
the ball, so the air is shown like a wind blowing in the
opposite direction as the ball is moving.) Here the ball is
experiencing the force of its weight straight down (not
shown), a drag force to the left slowing it down (not
shown), and an aerodynamic force called the magnus force
F F
For
completeness I would like to talk about what happens when
the ball hits the ground because these are strategically
important in tennis. Shown in the second figure are the
forces (in red) which the ground exerts on the ball in top
and back spin cases. For clarity, I have not shown the
forces due to the weight or the air. In each case there is a
normal force N
f which slows down the spin
in both cases. In the the top spin case, the friction both
slows down the spin and speeds up the ball so it comes up
faster and lower than a nonspinning ball would; in the the
back spin case, the friction both slows down the spin and
slows down the ball so it comes up slower and higher than a
nonspinning ball would. If the spin were large enough, the
back spin ball could actually bounce straight up or even
backwards!
hf , which the photon
had is given to the electron; the electron ends up with a
kinetic energy equal to hf minus the
binding energy it had in the atom. The rest mass of the
electron remains unchanged.
17 kg/m3 , so your volume would be
about 102 /2x1017 =5x10-16 m3 .
So, if you are a cube, your dimensions would be 3 5x10-16 =8x10-6
m ≈10 microns. A flea has a size of about 1
mm=1000 microns, one hundred times bigger than the
compressed you. And, yes, you would still have a mass of 100
kg.
link .
R , the R ω ,
etc . all distract from the crux of the problem, in
my opinion). I have redrawn the problem showing some axially
symmetric object of radius R , mass m rolling down
an incline of angle θ without
slipping. There are only three forces acting on the object,
the frictional force f N ,
mg N
f a F ma
and Στ Iα );
here I is the moment of inertial about the axis
about which torque is calculated and α
F ma
I find N=mg cosθ and ma =mg sinθ
-f. The first equation nails N , one of our
unknowns, the second is one equation for the two remaining
unknowns, so we are not done. So the only place to get a
second equation is the rotational form of Newton's second
law; I think this is the trickiest part of this problem. I find many students
have an inclination to choose the symmetry axis to sum
torques; they have been told, when they learned statics of
non point objects, that you can choose any axis you like,
but this is not a statics problem and there is a very
important constraint—Newton's laws are not valid
in an accelerating system , and the center of the
rolling object is accelerating. (See correction below!) So Στ Iα
yields Iα=Ia /R=mgR sinθ ,
or a= (mR 2 /I )g sinθ ;
knowing a , then f =m (g sinθ -a )
But, what is I ? It isn't what you look up in a book
because usually what is listed is the moment of inertia
about an axis passing through the center of mass (Icm ).
Here the axis is a distance R from the center of
mass, so using the parallel axis theorem, I=Icm +mR 2 .
I will do one example, a solid sphere where Icm =2mR 2 /5,
so I =7mR 2 /5, so a =5g sinθ /7
and f =2mg sinθ /7. If you sum torques
about the center of mass, you get the wrong answer.
OK, I slipped up here, albeit in a fairly minor way. While
it is true that Newton's laws are not correct in an
accelerating frame of reference, there is one exception: the
sum of the torques about an axis passing through the center
of mass is indeed Icm α .
A little detail I had forgotten about classical mechanics.
Let me work that out for my example: Icm α= 2maR /5=fR ,
so, using the result above, f =2ma /5=m (g sinθ-a )
or a =5g sinθ /7. Then it
easily follows that f =2mg sinθ /7.
But you should try to sum torques about an axis halfway
between the point of contact and the center of mass—you
will not get the right answer.
Nevertheless, it is important that your students be careful
in choosing the axis. I have edited the original answer
somewhat.
Most Massive Black Holes . This is the most
up-to-date information I could find.
article I found, recent research indicates that the
outer core rotates with the same speed as the mantle (once a
day) but the inner core's rotational speed is slightly
faster by about 0.3-0.5 degrees per year.
CD
for the three shapes, determined experimentally, are shown
in the figure. The drag force is given by FD = ρv 2 CD A
where ρ is the density of the air, v
is the speed of descent in still air, and A is the
area. Therefore the drag force is least on the circular
parachute so it reaches the ground first. (A proviso is that
the values of the drag coefficient depend on a quantity
called the Reynolds number which depends on the velocity.
However, the values given are for low Reynolds numbers which
are suitable for parachutes.)
paper on special relativity, On the
Electrodynamics of Moving Bodies , states two main
problems in electromagnetic theory at the end of the 19th
century:
The first
paragraph states, essentially, that Maxwell's equations
will not have the same form in a frame of reference
moving with constant velocity relative to a frame where
they are the laws governing electromagnetism if you
transform them using Galilean transformations.*
The
beginning of the second paragraph acknowledges "…the unsuccessful attempts to discover
any motion of the earth relatively to the 'light medium' [luminiferous æther,
e.g. the
Michaelson-Morley experiment]…"
Einstein had a
strongly-held philosophical belief that, for something to be a
true law of physics, it must be the same in all reference frames—regardless
of where you are or how you are moving, the laws of physics for
you are the same as for anybody else in the universe; this is
the principle of relativity . Since he believed
Maxwell's equations to be laws of physics, he concluded that
Galilean relativity was not correct and this led to his
postulate that the speed of light was independent of the motion
of the source or the observer. To my own mind, I believe that
the constancy of the speed of light is not a necessary
postulate, rather a
consequence of the principle of relativity applied to
Maxwell's equations.
*A Galilean transformation is, for
example, observing a car moving 60 mph east relative to the
ground to be moving 100 mph east if you are in a car moving 40
mph west relative to the ground.
M moving with velocity V MV after the
collision or any time during the collision. What will not be
conserved is the kinetic energy MV 2 .
recent answer , you mention the Cosmic Microwave Background and say that it "provides a frame of reference for the whole universe".
It was my understanding that one of the underpinnings of the basic theory of relativity is that there CANNOT be such a universal frame of reference (UFOR). I assume you're not claiming Relativity has been disproven (well, shown to be a special case of something else), so can you explain the difference between the frame of reference meant for relativity and the CMB as you described it?
v v
0 F) of fall would result in the
outside being burnt and the inside being raw. It might be
fun to do a couple of very rough calculations just to get an
order of magnitude feeling for what you are interested in.
I will approximate the turkey to have the properties of
water, in particular that its specific heat is C =4.186
J/gram⋅0 C; so the energy which will raise
the temperature of a M =6000 gm turkey is E=MC ΔT =6000x4.186x56=1.41x106
J. (700 F→1700 F is 210 C→770 C,
hence ΔT =560 C.)
The change in potential energy in falling from a height
h is V=Mgh =6x9.8h= 59h , so if the turkey falls
with constant velocity the potential energy lost goes into
heat. If the heat is 1.41x106 J, the height is
h =1.41x106 /59=24,000 m. The atmospheric
pressure at this altitude is only about 3% what it is at sea
level; so it is clear that, if your turkey is given any
velocity at this altitude, it will not continue moving with
constant velocity. (Whereas, if the pressure were
atmospheric and you gave the turkey a speed equal to the
terminal velocity it would continue moving with that speed
as it fell.) If you dropped it from very far away
(essentially infinitely far), it would arrive at the upper
atmosphere going nearly the escape velocity, 11,200 m/s. At
this speed, which is faster than the reentry speed of the
shuttle which needed special ceramic tiles to shield against
burning up, the turkey would be burned to a crisp, probably
would not reach ground before totally burnt. Although there
would be some speed of entry to the atmosphere where the
turkey would absorb 1.41x106
J, it would almost certainly not be "perfectly cooked".
light isotope of helium, He (one neutron, two protons), and also a gamma
ray. Two of these 3 He now fuse, throwing off two
protons in the process and one alpha particle (4 He,
two protons and two neutrons). The two thrown-off protons
are now free to continue the process, so this chain, called
the proton-proton cycle, is self-sustaining until the star
runs out of hydrogen which ends the life of the star.
For more earth-bound hydrogen fusion, like fusion reactors
or hydrogen bombs, single-step reactions are sought. The
most frequently used is the deuterium-tritium reaction,
involving the fusion of one deuteron and one triton (3 H,
one proton and two neutrons) shown in the other figure.
Most certainly not! The expression for the time t
elapsed in the gravitational field of a nonrotating
spherically symmetric mass M is t=t 0 / √(1- δ )
where δ= 2GM /(Rc 2 )=2aR /c 2 ;
here, R is the distance from the center, t 0
is the time elapsed when R =∞, G
is the universal gravitational constant, M is the
mass of the sphere, and c is the speed of light,
and a is the local acceleration due to gravity. If a=g
and R =6.4x106 m (earth radius), it
is easy to calculate that δ= 1.39x10-9 .
Now, t g t ½g =[√(1- ½δ )]/[√(1- δ )];
using the binomial expansion
(1 +δ )x ≈1+xδ+ …
if δ<< 1, we finally get t ½g ≈tg (1+¼δ )=tg (1+3.5x10-10 ),
quite a bit different from t ½g =2tg !
old
answer and the links it contains. I do not know what
"accelerate wildly" means in this context but, since you
mentioned "bumped", mechanical bumping probably caused
unexpected behavior of the radiometer.
groundrule for "single, concise, well-focused questions". I can tell you that what is learned in elementary physics courses that airplanes get lift from the Bernouli effect of lower pressure due to higher velocity of air on the top of a wing is a relatively small part of how an airplane is able to fly. As you seem to refer to in your question, the main thing is that air leaves the wing with a downward component
of its velocity; this means that the wing exerted a force down on that air which means, via Newton's third law, that the air exerted a force up on the airplane. To quote Wolfgang Langewiesche, author of
Stick and Rudder ,
the private pilot's bible on the art of flying, "The main fact of all heavier-than-air flight is this:
the wing keeps the airplane up by pushing the air down ."
e.g. , another galaxy or the
center of our local cluster of galaxies. However, the
discovery of the cosmic microwave background (CMB) has now
given us a reference frame which seems to define the
reference frame of the whole universe. Very careful
measurements and data analyses from the satellite COBE have
shown that our galaxy moves with a speed of about 580 km/s
relative to the CMB.
So, what can we do to answer your question which is,
essentially, how far does the earth move in 57 yr=1.8x109
s? (Your 5 minute question is essentially impossible to
answer since it depends on the time of year. Over years the
orbital motion averages out to zero.) Relative to the center
of the galaxy, the distance is D =220x1.8x109
km= 4x1011 km=0.013 pc. The center of the galaxy
in that time will move 580x1.8x109 km=1012
km=0.032 pc. But I do not know the relative directions of
these two velocities, the sum of which would be the average
velocity of the solar system over these 57 years; this speed
would be anything between 360 and 800 km/s. However, in my
researching this question I found that the speed of sun
relative to the CMB is about 370 km/s, so the final answer
is that the earth moved about 370x1.8x1011 =6.7x1011
km=0.022 pc. It is interesting to me that, at this time, the
sun and the center of the galaxy are moving in nearly
opposite directions (370 km/s compared to 360 km/s); since
the time for the sun to go all the way around the galaxy is
about 225 million years, in about 110 million years our
speed relative to the CMB will be about 800 km/s.
Keep in mind that I am not an
astronomer/astrophysicist/cosmologist! I have gathered these
data as best I can.
2 )=1.93368x10-5
PSI=1.31579x10-6 atm.
As the conversation progressed, we considered the implications and began to wonder if it was possible to shield against cosmic radiation? To the best of my knowledge, I explained that no substance I know of can block cosmic radiation and that the Earth's magnetic field would have little effect either. The only effects I know of are when they impact atoms in the atmosphere or the earth. If I understand this, if it doesn't hit something fairly dense, it just keeps going, understandable given the space between atoms.
I have read about the gravitational lensing effects on light by massive objects like neutron stars and galaxies that bend light around them. I have also read about the possibility of warping space as a method space travel by changing the shape of space in front of and behind a craft so that it "falls" in a particular direction.
While we were discussing these effects, he looked at me and said something to the effect, "Maybe we could bend space and make them go around?". To me, this was a pretty profound leap in my book. So I decided to ask physicist if he could be right.
Please forgive the length of this post before asking our question. I wanted to provide sufficient context before asking. So, here it is. Is it possible to make cosmic rays go around something, either by gravitational or microwave warping of space?
B.T.W. I really really enjoy your web site. It is awesome!
But, I can speak to your main question and comment on some
of your statements.
Cosmic
radiation refers to a broad range of radiations but
mostly protons and light nuclei; but also it could refer to
neutrinos, electrons, positrons, antiprotons, gamma rays,
x-rays, and others. What is not the case, though, is that "no
substance…block cosmic radiation"; just about any
cosmic radiation can be blocked by a dense solid or liquid.
Neutrinos are the exception and most pass all the way
through the earth without any interactions. You may know
many neutrino experiments are performed in deep abandoned
mines to block out all other radiation. The atmosphere also
is very effective since a single energetic proton will
strike an atom and many other particles, all with less
energy than the original proton, will form a "shower" of
particles. And magnetic fields are not very effective
deflecting the very highest energy charged particles but are
known to be an effective shield for lower energy particles.
Finally, let's address
the question of warping of space as a way to deflect the
rays. The only way to warp space that I know of is to have
an enormous mass nearby. The earth already warps the space
around it which would cause a particle passing close by, but
not on a collision course with earth, to be deflected a tiny
bit (viz. gravity). But putting a star sized object near
enough the earth to "shield" us would obviously be a
catastrophic thing to do! The whole solar system would be
disrupted. I have no idea what "microwave warping of space"
means.
I commend your son for his hypothesizing and you for your
tutoring and encouragement of his curiosity.
and electric fields
earlier answer to understand the answer
here. The graph here is from that earlier answer and shows
(in red) v /c as a function of a 0 t /c
where a 0 is the acceleration measured in
the frame of the object which is accelerating and t
is the time since the object was at rest. Reading off the
graph, you can see that v /c =0.9 when
a 0 t /c= 2. Now, t =30
days=2.6x106 s, so a 0 t /c=a0 (2.6x106 /3x108 )=8.64x10-3 a 0 =2;
solving, a 0 =232 m/s2 =23.6 Gs. I would not
suggest having anybody aboard this object!
m is walking up a
hill with incline θ with a constant
speed of v . His potential energy is E=mgy
where y is his height above the bottom of the hill
and g= 9.8 m/s2 is the acceleration due
to gravity. The rate at which his energy is changing is dE /dt=P =mg (dy /dt )=mgvy =mgv sinθ ;
so this rate (called power) depends only on the vertical,
not the horizontal component of his velocity. Now, you have
made things difficult for me because you have not specified
the angle, but rather the inclination which is actually the
tangent of the angle (rise/run) times 100%. I will call this
inclination the grade G =100tanθ. For
example, let's take a man with mass 100 kg walking with a
speed of 2 m/s up the 10% and 20% inclines you specify. The
angles would be θ 10% = tan-1 (10/100)=5.710
and θ 20% = tan-1 (20/100)=11.310 .
So the power values are P 10% = 100x9.8x2xsin(5.71)=195.0
Watts and P 20% = 100x9.8x2xsin(11.31)= 384.4
Watts. The ratio of these two is 1.97, close to, but not
equal to, 2.0; for small angles the sine and tangent are
approximately linear functions but as the angle (hence
inclination or grade) increases this is no longer a good
approximation. The graph shows the power for grades up to
200% (about 63.40 ); as you can see, the power
increases approximately linearly only up to about a grade of
about 30% which is about 170 .
When I say "trajectory"
I refer to the path from collision point to the ground. The
horizontal distance gone from the point of collision to the
point of landing depends on the angle at which the cat
started; if launched at 450 relative to the
horizontal he will go much farther than if launched at 200 .
Again, unless you witnessed the accident, there is no way to
know the angle.
2 )=0.31;
so if you went to a star 1 light year from earth, it would
only take you 0.31/0.95=0.33 years to get there but the
earth-bound clock would say it took you 1/0.95=1.05 years.
earlier
answer . In the case where v /c =0.95, the graph shows
how the angle at which you see something depends on where it
would be if you were at rest; for example, a star actually
at θ =1200 (300
behind you) would be seen as being about θ' ≈300
in front of you!
R =2GM /c 2 ,
would be about 1 cm. R is the radius within which
nothing can escape. So, if you could get the earth down to
that size, it would then collapse the rest of the way to a
black hole, I presume.
m approaches the end of a thin uniform rod of mass
M and length 2L with velocity v L from where m
exerts the force. Linear momentum and angular momentum are
both conserved but, as we shall see, energy is not
conserved. After the collision the center of mass has a
velocity u ; conserving linear momentum, (M+m )u=mv
or u=v [m /(M+m )]. Before the
collision m brings in an angular momentum mvL .
After the collision, the rod plus mass has angular momentum
(I +mL 2 )ω
where I=M (2L )2 /12=ML 2 /3
is the moment of inertia of a thin rod about its center of
mass. Conserving angular momentum I find ω [m +(M /3)]L 2 =mvL
or
ω=mv /{[m+ (M /3)]L }.
Just for fun I put in some numbers to illustrate what would
happen in a specific situation: m =1 kg, M =3
kg, L =1 m, v =4 m/s. With these I find:
u =1 m/s, ω =2 radians/s=19.1 rpm. You can
also calculate the energy before and after the collision:
E before = ½mv 2 =8
J, E after =½(M+m )u 2 +½([m +(M /3)]L 2 ω 2 =6
J. So, energy was not conserved in this collision, 2 Joules
were lost.
x=mL /(M+m )
toward where m is stuck. It is this center
of mass which moves forward with speed u , and u
is still v [m /(M+m )]. The rotation
is about this center of mass but now the moment of
inertia is different; the net (rod plus mass) moment of
inertia is ML 2 /3+Mx 2 +m (L-x )2 ,
so the corrected value of the angular velocity is
ω=mvL /[ML 2 /3+Mx 2 +m (L-x )2 ].
In the example I did, x =1/4 m, so ω= 16/7 radians/s=21.8 rpm and E after =46/7=6.57
J (1.43 J lost).
earlier answer and the earlier answers referred to in
that answer. The graph here shows the results derived or
cited in that earlier answer. The three graphs all show what
is observed of your motion as seen by the twin on earth. The
red curve is your velocity v relative to c
as seen by the earth-bound twin, v /c =(gt c )/√[1+(gt c 2 ];
the blue curve is your acceleration a g , a /g =[1+(gt c 2 -3/2 ;
the black curve is your position expressed (approximately)
in light years, gx /c 2 =√[1+(gt /c )2 ]-1.
Now, since I have set this up as seen from earth, let me
specify the time you travel as the time of your trip out as
observed from earth: earth-bound twin observes you to arrive
at you destination in two years. Then, as you can read off
the graph, gx /c 2 =√[1+(2)2 ]-1=1.24
ly; the return trip will be the same length of time, so the
earth-bound twin's clock will have advanced 4 years. Light
would take 2.48 yr to travel that distance, so your clock
will have advanced a time somewhere between 2.48 and 4
years. Your maximum speed would have been about v /c =(2)/√[1+(2)2 ]=0.89.
We can get a rough estimate of your clock reading by
approximating your average relative speed as 0.89/2=0.445;
so you would have seen, on average, the distance contracted
by √[1-(0.445)2 ]=0.9 and your time would
have been 0.9x4=3.6 years.
g appears to be
somewhat smaller than it really is, but the amount is very
tiny. This effect depends on your latitude and is zero at
the poles and greatest at the equator. Also because of this
effect, the acceleration is not directly toward the center
of the earth except at the poles and equator.
earlier answer
illuminating.
Kibble balance which is used. Also see
Wikipedia for more detail
I stated that it was incorrect based on the fact that
"made up of" usually means putting two or more things together (aka addition). Net radiated energy is the difference between emitted energy and absorbed energy. I have yet to see my exam paper but I believe that the mark I lost was due to this question on basis that “made up of” means that it is a result of a mathematical relation between the two values and not necessarily addition (in this case subtraction). What is the correct answer in this case and why?
angular
speed of the object in the smaller orbit is twice that
of the object in the larger orbit even though their linear
speeds are the same. You cannot do this with planets or
moons, though, because the speed of a satellite in a
circular orbit depends on the radius.
essay about general relativity, curvature of
spacetime, gravity. Many nonscientists (and scientists as
well) are familiar with and accept as gospel that general
relativity demonstrates that the distortion of spacetime by
the presence of mass is what gravity is; the "cartoon" which
illustrates this is the "bowling ball on a trampoline
example in which a mass causes the distortion of the
two-dimensional space defined by the trampoline surface. The
implication is that gravity is just geometry. On the other
hand, many theorists are struggling to find a successful
theory of quantum gravity and to do that one must treat
gravity as a force. The take-away from this essay, though,
is that curved spacetime is not a unique representation of
what the mathematics which are the framework of the very
successful theory of general relativity mean. The author,
Rodney Brooks, notes that "…you can view gravity as a force field that, like the other force fields in QFT
[quantum field theory], exists in three-dimensional space and evolves in time according to the field equations."
He also goes so far as to say "…shame on those who try to foist and force the four-dimensional concept onto the public as essential to the understanding of relativity theory."
a and a mass M . The forces on
the car are its own weight W W=Mg )
acting at the center of mass a distance d from the
real axle; the normal and frictional forces on the rear
wheels, N 1 and
f 1 ; and the normal and
frictional forces on the front wheels, N 2
and f 2 ; the radius of
the wheels is R and the distance between front and
rear axels is D . I will ignore the rotational
motion of the wheels, that is, I will approximate their
masses as zero. If the front wheels are not lifting up from
the ground, the sum of torques about the rear axel is (f 1 -f 2 )R +N 2 D -Mgd= 0;
Newton's first law for the horizontal and vertical
directions are (f 1 -f 2 )=Ma
and N 1 +N 2 Mg =0.
From these equations it is easy to show that N 2 =M (gd-aR )/D .
This is interesting because it shows that N 2 =0
if a=gd /R ; for larger accelerations, the
front wheels will lift off the ground. (Note that as N 2
approaches zero, f 2 also approaches
zero.) I have ignored the suspension of a real car, so this
lift will not be abrupt; it will happen gradually as the
front springs decompress and the rear springs compress; so
overall the nose goes up but the rear end goes down.
If
it is a front-wheel drive, the directions of the frictional
forces reverse. The corresponding torque equation (this time
about the front axle) is
(f 2 -f 1 )R-N 1 D+Mg (D-d )= 0;
Newton's first law for the horizontal and vertical
directions are (f 2 -f 1 )=Ma
and N 1 +N 2 Mg =0.
From these equations it is easy to show that N 1 =M (aR+g (D-d ))/D .
As a increases in magnitude, N 1
gets bigger and bigger until N 1 =Mg
which necessarily means that N 2 becomes
zero. It is easy to show that this happens when a=gd /R ,,
exactly the same result as for the rear wheel drive.
a ,
so most likely the wheels will slip well before N 2 =0
when f 2 must be zero. For very large
accelerations, like required for drag racers, rear-wheel
drive is imperative.
i.e. all
objects near the surface of the earth have an acceleration
of 9.8 m/s2 . The acceleration (which is what
describes the orbit) is F /m but the force
is MmG /r 2 , so the acceleration
is MG /r 2 .
t . Its
momentum drops from mv (where m is the
mass and v is the speed when it hits) to zero
because an impulse I was delivered to it by the
ground. The impulse may be written as I=F avg Δt .
where F avg is the average
force. Therefore you can find the average acceleration a avg
during the collision, but not the acceleration as a function
of time: a avg =F avg /m =I /(m Δt )=v /Δt.
So you cannot get detailed kinematics about the
collision without measuring how the speed decreases with
time.
here .
F= ¼A (u-v )2
where u is the speed of the wind, v is the
speed of the ball, and A is the cross sectional
area of the ball. Applying Newton's second law, ¼A (u-v )2 =ma =m dv /dt
. This differential equation may be shown to have the
solution t=cv /[u (u-v )] where
c =4m /A and t is the time it takes the
ball to reach the speed v if the wind speed is
u . I find that c =137 s2 /m. Note
that after a very long time the speed will be constant at
the wind speed; we are only interested in the time it takes
to get to 35.8 m/s (80 mph). I have plotted t for
three values of u , 70, 80, and 90 m/s.
Now comes the hard part. We are interested in finding the
value of u for which v will be 35.8 m/s when the ball has
gone a distance x =18.4 m. This means that we need
to write the equation for t as
t=c {dx /dt }/[u (u- {dx /dt })]
and solve that differential equation for t as a
function of x . That is actually doable, but the
solution is so messy that I looked for a simpler way to do it.
This took some trial and error, but I got a pretty good
estimate, I believe. Look at the black line in the graph; it
is not a straight line, but it is pretty close, so I am going
to approximate the acceleration as being constant over this
time interval of 1 s, a2 . Now, an object with constant acceleration
starting from rest goes a distance d = ½at 2
in a time t , so if u =90 m/s=201 mph the ball will have a
speed of 35.8 m/s when d =35.8/2=17.9 m=59 ft. As
far as I am concerned, I have adequately solved this problem—it
takes a wind of approximately 200 mph to accelerate a
baseball from rest to the speed of 80 mph in a distance of
about 60 ft.
groundrules state
that I will not answer questions of this sort. Your first
question is equivalent to the question "why can nothing with
mass travel as fast or faster than light?" which is included
in the FAQ page.
