Escape Velocity and Centripetal/Centrifugal Acceleration

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Discussion Overview

The discussion revolves around the concept of escape velocity and its relationship with centripetal and centrifugal acceleration, particularly in the context of a hypothetical scenario involving a train traveling in a tunnel around the Earth. Participants explore the implications of traveling at escape velocity and the resulting forces experienced by passengers.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant notes that at escape velocity (11.2 km/s), passengers in a train would experience 1G towards the ceiling, suggesting a unique perspective on gravitational effects.
  • Another participant questions the novelty of this observation, emphasizing the need for a force to maintain circular motion and challenging the interpretation of the forces involved.
  • A participant shares calculations for the moon, indicating that at escape velocity, the net upward acceleration equals 1 moon G, drawing parallels to the Earth scenario.
  • It is proposed that the principle applies universally to any mass, where traveling at escape velocity results in a net acceleration equal to gravitational acceleration in the opposite direction.
  • One participant mentions the relationship between orbital energy and escape energy, suggesting that doubling the energy corresponds to a specific increase in speed and centripetal acceleration.
  • A reference to the virial theorem is made, indicating a potential theoretical framework for understanding the relationship between escape velocity and gravitational forces.
  • Another participant reflects on practical considerations for launching a vehicle at escape velocity, noting challenges such as air friction upon emergence from an evacuated tube.

Areas of Agreement / Disagreement

Participants express a mix of interest and skepticism regarding the implications of escape velocity and its effects. While some find the calculations and observations intriguing, others challenge the interpretations and practicality of the scenarios discussed. No consensus is reached on the novelty or applicability of the ideas presented.

Contextual Notes

Participants acknowledge various assumptions related to the scenarios, such as the need for an evacuated environment to minimize friction and the conditions under which the calculations hold true. The discussion remains open-ended regarding the practical implementation of the concepts.

willoughby
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This is just a reality that I have stumbled upon that I'm sure was well-known, but I still found it interesting. I apologize if this is second-nature to physics experts.

I was responding to a post on a different thread that claimed you could make a tunnel around the Earth and if you sent a train or something around that tunnel at 11.2 km/s, the people inside would feel weightless. Of course, this isn't the case; they only need to be traveling at what the orbital velocity would be at the surface of the Earth. I corrected him, and also wanted to be able to tell him what would happen if the train WERE going 11.2 km/s, and I calculated it, and as it turns out, the people on that train would experience 1G, but toward the top of the train. I though maybe this was a coincidence, so I actually did the math and it turns out that it is EXACTLY 1G. Like I said, I'm sure this is well-known, but I though it was a cool fact. At escape velocity, you would experience exactly 1G toward the roof. It would feel as though you were still on Earth, but the ceiling of the train would become the floor. I further delved into the equations and came up with why this was the case.

The acceleration due to gravity is GM/r². Centripetal acceleration can be calculated as v²/r. Escape velocity is √(2GM/r), and if we plug in the escape velocity into the centripetal acceleration equation, we get 2GM/r². I found that to be very cool. Acceleration due to gravity is GM/r² while centripetal acceleration with a radial velocity equal to escape velocity would be 2GM/r². Gotta love physics.
 
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willoughby said:
It would feel as though you were still on Earth, but the ceiling of the train would become the floor. I further delved into the equations and came up with why this was the case.

somehow i could not feel the thrill of 'new physics'...or i missed it...normally if you rotate anything on Earth say a man sitting inside the rotating body will need a force to keep it on that path and the reaction of the top of the container will provide it , otherwise he will fly off tangentially. so whatever be the magnitude of the velocity ...the force needed will be mass times v^2 divided by r. thanks and pl explain what was amiss.
 
willoughby said:
I actually did the math and it turns out that it is EXACTLY 1G. Like I said, I'm sure this is well-known, but I though it was a cool fact.
I didn’t know it! Definitely interesting
 
Thought I would do the calculation for the moon and it appears to give the same answer...

The escape velocity of the moon is 2.38 km/s. The radius of the moon is 1737km.

a = v2/r = 23802 / 1737,000
= 3.26 m/s2

The actual acceleration due to gravity is 1.63 m/s2 so the net upward acceleration is 3.26 - 1.63 = 1.63m/s2 or 1 moon g upwards.
 
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Yes, it would work anywhere. Basically, if you were in some vehicle that was traveling in a circle with a radius equal to the distance from the center of any given mass at a radial velocity equal to the escape velocity from that mass at that height, the net acceleration would be equal to the gravitational acceleration - just in the opposite direction since the resulting radial acceleration is exactly equal to twice the gravitational acceleration from that same height.
 
One could derive it from the related fact that orbital energy for a circular orbit is half of escape energy. Double the energy and you've multiplied speed by ##\sqrt{2}##. Multiply speed by ##\sqrt{2}## and you've doubled centripetal acceleration.
 
It looks like a special case of the virial theorem.
 
I was just trying to imagine what the journey would feel like for passengers and then I considered other practicalities for space launching in this way. Assuming the tube that was being used could be evacuated, there would be no problem inside it but, as soon as the ship emerged at sea level, there would be significant friction losses at the high speed through air at 1At. But perhaps the time for that phase would not be too long(?).
So I think this may just be a thought experiment, at best. Mr Musk seems to have the best solution at the present time.
 

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