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Understanding centripetal force

 
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Sep16-11, 05:23 AM   #18
 
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Understanding centripetal force


Quote by jsmith613 View Post
Q:If the earth rotated faster on its axis would would happen to your weight (as measured by a scale)


Answer
Here, the centripetal force increases due to an increase in speed.
As we said before, mv2/r = mg - R
This is correct.

My weight = the reaction force so R = mv^2/r + mg therefore weight increases
This is not correct.

Take the correct equation and solve for R.
Sep16-11, 05:28 AM   #19
 
Quote by Doc Al View Post
This is correct.


This is not correct.

Take the correct equation and solve for R.
sorry
R = mg - mv^2/r
Sep16-11, 05:48 AM   #20
 
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Quote by jsmith613 View Post
sorry
R = mg - mv^2/r
Good. Now how would you answer the question?
Sep16-11, 06:38 AM   #21
 
as speed increases, Reaction force decreases so apparent weight decreases
Sep16-11, 06:39 AM   #22
 
This matches the answer
could we now go through Q2 (with the change of "space habitat" to "satellite")
Sep16-11, 07:50 AM   #23
 
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Quote by jsmith613 View Post
as speed increases, Reaction force decreases so apparent weight decreases
Good.
Quote by jsmith613 View Post
could we now go through Q2 (with the change of "space habitat" to "satellite")
Please state the problem you are asked to solve.
Sep16-11, 08:11 AM   #24
 
Q:As the rotational speed of a satellite increases what happens to the apparent weight of the people inside

The force, mg, of the space station acts towards the earth

F = ma
F = mv2/r
BUT v = omega (w) * r
SO

F = m*w2*r

F = (GMm)/r2

(GMm)/r2 = m*w2*r

If w (omega) increases then Force increases
this seems wrong because GMm/r2 should always be constant and therefore not affected by speed :S

this is where i get stuck
Sep16-11, 08:14 AM   #25
 
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Quote by jsmith613 View Post
Q:As the rotational speed of a satellite increases what happens to the apparent weight of the people inside
I assume they mean orbital speed, not that the satellite is rotating about it's center of mass.

Note that the satellite is in free fall as it orbits. So what's the apparent weight of the people inside? No calculation needed.
Sep16-11, 08:16 AM   #26
 
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Quote by jsmith613 View Post
http://www.youtube.com/watch?v=1CD8Q...eature=related

could someone please explain what is the forces are here (especially Fn)
I don't like the presenters explanation very much. I look at the problem this way:

When the bucket is overhead, the water will tend to accelerate down with acceleration g, just as it would if there was no bucket there at all.

In order to not have the water coming out of the bucket, you must accelerate the bucket down at g or higher.

You could pull the bucket down with great acceleration, but it will soon hit the ground.

If you rotate the bucket fast enough, the bucket will have acceleration [centripetal acceleration towards the centre] given by V2 / R. Provided that is at least equal to g, we have the bucket accelerating down with a sufficiently large acceleration for the water not to fall out of the bucket.
Sep16-11, 10:10 AM   #27
 
Quote by Doc Al View Post
I assume they mean orbital speed, not that the satellite is rotating about it's center of mass.

Note that the satellite is in free fall as it orbits. So what's the apparent weight of the people inside? No calculation needed.
I copied the question exactly from a website. The website has the answer as an increase.
The only force acting on the satellite is mg (towards the earth) and we would use the F = GmM/r^2 to find this force (I presume)

I don't see why no calculation is needed for your interpretation of the Q
Sep16-11, 10:15 AM   #28
 
Quote by PeterO View Post
I don't like the presenters explanation very much. I look at the problem this way:

When the bucket is overhead, the water will tend to accelerate down with acceleration g, just as it would if there was no bucket there at all.

In order to not have the water coming out of the bucket, you must accelerate the bucket down at g or higher.

You could pull the bucket down with great acceleration, but it will soon hit the ground.

If you rotate the bucket fast enough, the bucket will have acceleration [centripetal acceleration towards the centre] given by V2 / R. Provided that is at least equal to g, we have the bucket accelerating down with a sufficiently large acceleration for the water not to fall out of the bucket.
i would presume the logic is
if the bucket accelerates fast than the water downwards then the bucket will move before the water has a chance to get out.
My next question is why won't the bucket and the water accelerate at the same speed downward as they are effectively one object
Sep16-11, 10:23 AM   #29
 
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Quote by jsmith613 View Post
I copied the question exactly from a website. The website has the answer as an increase.
So they are talking about the rotation of the satellite about its center of mass, not its orbiting around the earth.
The only force acting on the satellite is mg (towards the earth) and we would use the F = GmM/r^2 to find this force (I presume)
What you need to consider is the force exerted by the rotating satellite (a space 'habitat') on the passenger. That's his apparent weight. The force of the earth on the satellite is not relevant to this question.

Imagine the 'satellite' as a rotating cylinder and a person is standing on the inner surface of that cylinder. As the rotational speed increases, what happens to the force with which he is pressed against the 'floor'?

FYI: 'mg' is only valid near the earth's surface.

I don't see why no calculation is needed for your interpretation of the Q
Think of astronauts in the space shuttle once they are in orbit. What's their apparent weight?
Sep16-11, 11:25 AM   #30
 
Quote by Doc Al View Post
What you need to consider is the force exerted by the rotating satellite (a space 'habitat') on the passenger. That's his apparent weight. The force of the earth on the satellite is not relevant to this question.


Imagine the 'satellite' as a rotating cylinder and a person is standing on the inner surface of that cylinder. As the rotational speed increases, what happens to the force with which he is pressed against the 'floor'?

FYI: 'mg' is only valid near the earth's surface.
ok so with a free body diagram,
mg = down
Reaction force = towards centre
he is accelerating towards the centre of the satellite (i presume this is up)
F = ma
ma = R - mg
mv^2/r = R - mg
mg = R + mv^2/r

so as the satellite rotates faster, his weight increases :)

I am confused though as to why on earth the effect of a faster rotation is completley different than on a satellite

Quote by Doc Al View Post
Think of astronauts in the space shuttle once they are in orbit. What's their apparent weight?
well weight = mass * acceleration
I would presume their weight is dependant on how fast the rocket is accelerating
Once in orbit, they must have a net acceleration towards the earth (v^2/r) so the guys weight = mass * (v^2/r)
Sep16-11, 12:03 PM   #31
 
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Quote by jsmith613 View Post
ok so with a free body diagram,
mg = down
Reaction force = towards centre
he is accelerating towards the centre of the satellite (i presume this is up)
F = ma
ma = R - mg
mv^2/r = R - mg
mg = R + mv^2/r

so as the satellite rotates faster, his weight increases :)
The only force on the person that you need to consider is the 'reaction force' from the 'floor' of the satellite.

I am confused though as to why on earth the effect of a faster rotation is completley different than on a satellite
On the earth you are standing on the outside of the rotating body; in the satellite, you're standing on the inside. (Look up 'artificial gravity'.)

well weight = mass * acceleration
I would presume their weight is dependant on how fast the rocket is accelerating
Once in orbit, they must have a net acceleration towards the earth (v^2/r) so the guys weight = mass * (v^2/r)
So I guess you've never see pictures of the astronauts in orbit floating around in their ship?
Sep17-11, 02:03 PM   #32
 
of course, but they must weight something
Although, if your weight is given by the reaction force then floating astronouts have no weight
Sep17-11, 02:30 PM   #33
 
Quote by Doc Al View Post
The only force on the person that you need to consider is the 'reaction force' from the 'floor' of the satellite.
so was my answer wrong?

(please also see last post for the previous question)
Sep18-11, 12:47 AM   #34
 
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Quote by jsmith613 View Post
My next question is why won't the bucket and the water accelerate at the same speed downward as they are effectively one object
I don't like the way you used speed [I underlined it]!!!!
They do accelerate at the same rate [speed is not a term that relates well to acceleration]. The fact is that acceleration is greater than g, so the only way the water can accelerate at a rate greater than g, is if something applies an extra force to it [gravity is not enough] The thing that applies the extra force is the bucket - but that can only happen if the water remains in contact with the bucket - it doesn't come out.
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