Relativity and terminal velocity

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Discussion Overview

The discussion revolves around the concepts of gravity, terminal velocity, and the behavior of objects in a vacuum, particularly in relation to relativity and escape velocity. Participants explore hypothetical scenarios involving an evacuated tube, the acceleration of objects towards a planet, and the implications of black holes on these concepts.

Discussion Character

  • Exploratory
  • Debate/contested
  • Technical explanation

Main Points Raised

  • Some participants propose that an object in a long evacuated tube would continuously accelerate under gravity and thus have no terminal velocity, but it cannot exceed the speed of light.
  • Others argue that if the tube were infinitely long, the object could never reach the speed of light, suggesting that it would take an infinite amount of time to do so.
  • One participant suggests that an object released from infinity would impact a planet at its escape velocity, referencing the definition of escape velocity as the speed required to reach infinity.
  • Another participant agrees with the escape velocity argument but later expresses uncertainty about needing an infinitely long tube to define energy per kilogram at a point in space.
  • Questions are raised about whether a sufficiently massive object could accelerate another object to the speed of light, particularly in the context of black holes and their escape velocities.
  • A mathematical expression for terminal velocity is provided, indicating that it remains less than the speed of light for non-black hole objects, and that no stationary observer exists at or within a black hole's event horizon.

Areas of Agreement / Disagreement

Participants express multiple competing views regarding the behavior of objects under gravity, the nature of escape velocity, and the implications of black holes. The discussion remains unresolved with no consensus on several points.

Contextual Notes

Some limitations include assumptions about the nature of the evacuated tube, the definition of escape velocity, and the conditions under which terminal velocity is calculated. The discussion also touches on the complexities of black hole physics and the implications of relativistic speeds.

mrcotton
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Hi
If I had an object and a very long evacuated tube. Presumably the object with only the force of gravity acting on it would continuously accelerate and hence would have no terminal velocity.
However we know that it cannot go faster than light.
If my long tube is say pointing towards the centre of the Earth, how long would it have to be for an object to accelerate up to this speed.

If an object were to be released at infinity in a universe with only one planet would it reach the planet with a velocity equal to the escape velocity or would it have reached the speed of light.Any

thoughts to help my thoughts greatly appreciated
D
 
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mrcotton said:
Hi
If I had an object and a very long evacuated tube. Presumably the object with only the force of gravity acting on it would continuously accelerate and hence would have no terminal velocity.
However we know that it cannot go faster than light.
That's true but it also cannot reach the speed of light.

mrcotton said:
If my long tube is say pointing towards the centre of the Earth, how long would it have to be for an object to accelerate up to this speed.
Since it can never reach the speed of light, how about infinitely long?

mrcotton said:
If an object were to be released at infinity in a universe with only one planet would it reach the planet with a velocity equal to the escape velocity or would it have reached the speed of light.
If it's at infinity, then it will take forever to get to earth.

mrcotton said:
Any thoughts to help my thoughts greatly appreciated
D
I hope you didn't think my suggestion that the tube be infinitely long was serious. The fact of the matter is that it is impossible.
 
mrcotton said:
If an object were to be released at infinity in a universe with only one planet would it reach the planet with a velocity equal to the escape velocity or would it have reached the speed of light.

It would impact the planet with a speed equal to the planet's escape velocity. The way to see this is to imagine the situation in reverse: the object is launched upward from the planet's surface and eventually comes to rest "at infinity." The escape velocity is defined as the launch speed required for this to happen.
 
The_Duck said:
It would impact the planet with a speed equal to the planet's escape velocity. The way to see this is to imagine the situation in reverse: the object is launched upward from the planet's surface and eventually comes to rest "at infinity." The escape velocity is defined as the launch speed required for this to happen.
I like your answer better. Disregard mine.
 
Hi George, and The_Duck, thanks for responding.
There is no need to disregard an answer they all make me think.
I was under the impreeion we needed a long tube infinetly long to bring a unit mass from infinity to define the joules per kilogram at that point in space.

So the velocity an object would reach a planet at is its escape velocity.
If we had an object with enough mass can we have a large enough force to accelerate an object up to the speed of light.

Would a black hole with an escape velocity of the speed of light attract an object from infinity to arrive at the speed of light?

Black holes have varying masses and if I remember correctly that the escape velocity is dependent on the amount of mass contained within a specific volume.

Thanks again, all responses help me in my own thinking processes

D
 
The terminal velocity for a test particle initially at rest at infinity, and free falling radially towards a non rotating spherical massive object, is given by:

##v = c \sqrt{\frac{2GM}{rc^2}}##

where v is the velocity of the particle measured by an stationary observer at r. If the massive body is not a black hole and the observer is at the surface of the body, then ##r>2GM/c^2## and the terminal velocity must always be less than c when the object impacts the surface. If the object is a black hole there can be no stationary observer at ##r<=2GM/c^2## so the terminal velocity still never exceeds c.
 

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