Escape Velocity Question: Why is the final kinetic energy = 0?

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Discussion Overview

The discussion revolves around the concept of escape velocity, specifically addressing why the final kinetic energy of an object is considered to be zero when it reaches an infinite distance from a gravitational body. Participants explore the implications of this idea on the object's velocity and its interaction with gravity at large distances.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants express confusion about the final kinetic energy being zero, questioning if this implies the object has no velocity and would be affected by gravity again.
  • Others clarify that the final kinetic energy is zero only at infinity, suggesting that the object never actually reaches this point but continues to move away indefinitely.
  • One participant proposes that escape velocity serves as a threshold separating bound from unbound systems, indicating that if the initial kinetic energy exceeds a certain value, the object will not return to the gravitational body.
  • Some participants discuss the relationship between gravitational potential energy and kinetic energy, noting that as the object moves away, both energies approach zero, but the gravitational force also diminishes.
  • There are mentions of the limitations of escape velocity in practical scenarios, such as non-orbital journeys requiring higher speeds for timely travel to distant locations.
  • Mathematical formulations are presented to describe the conditions under which an object escapes gravitational influence, including discussions on the nature of potential energy in varying gravitational fields.
  • Some participants challenge the simplification of gravitational potential energy calculations, arguing that a more complex understanding is necessary for accurate descriptions in the context of escape velocity.

Areas of Agreement / Disagreement

Participants generally express differing views on the implications of final kinetic energy being zero and the conditions surrounding escape velocity. There is no consensus on the interpretation of these concepts, and multiple competing perspectives remain throughout the discussion.

Contextual Notes

Participants highlight the need for careful consideration of gravitational potential energy calculations, particularly in non-constant gravitational fields, and the complexities involved in understanding escape velocity in practical applications.

JoeyBob
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So Ekf-Eki+Epf-Epi=0. I understand that the final potential energy is 0 (distance away approaches infinity), but don't get why the final kinetic energy becomes 0. If the final kinetic energy was 0, wouldn't that mean the object no longer has any velocity and would start being effected by the gravity again, even if it was really far away from the planet?
 
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JoeyBob said:
If the final kinetic energy was 0, wouldn't that mean the object no longer has any velocity and would start being effected by the gravity again, even if it was really far away from the planet?
The final kinetic energy is zero only at infinity, which it never reaches. At any finite distance the object is moving away, so it will never return no matter how long you wait. With any lower initial velocity it would come to a stop at finite distance in finite time and then return. But with escape velocity it never quite stops.
 
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JoeyBob said:
If the final kinetic energy was 0, wouldn't that mean the object no longer has any velocity and would start being effected by the gravity again, even if it was really far away from the planet?
You are correct. When the kinetic energy drops to zero, the mass will fall back or orbit around the Earth. Gravity is a long range force that acts on masses even if they are in a galaxy far, far away.

You might think of the escape velocity as the threshold value that separates bound from unbound systems. If the initial kinetic energy of the mass is greater that ##\frac{1}{2}m v_{\text{esc}}^2##, then the mass will always have some kinetic energy left no matter how far it is from the Earth and the mass is considered no longer bound to the Earth. In another thread you have indicated that you are in a chemistry-related field. Think of the quantity ##\frac{1}{2}m v_{\text{esc}}^2## as the gravitational analogue of the ionization energy.
 
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JoeyBob said:
So Ekf-Eki+Epf-Epi=0. I understand that the final potential energy is 0 (distance away approaches infinity), but don't get why the final kinetic energy becomes 0.
Approaches and becomes are not synonyms.
 
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JoeyBob said:
Summary:: Why final kinetic energy = 0?

So Ekf-Eki+Epf-Epi=0. I understand that the final potential energy is 0 (distance away approaches infinity), but don't get why the final kinetic energy becomes 0. If the final kinetic energy was 0, wouldn't that mean the object no longer has any velocity and would start being effected by the gravity again, even if it was really far away from the planet?
What non-zero velocity "at infinity" does the object need in order not to fall back?
 
JoeyBob said:
Summary:: Why final kinetic energy = 0?

So Ekf-Eki+Epf-Epi=0. I understand that the final potential energy is 0 (distance away approaches infinity), but don't get why the final kinetic energy becomes 0. If the final kinetic energy was 0, wouldn't that mean the object no longer has any velocity and would start being effected by the gravity again, even if it was really far away from the planet?
As already pointed out the final PE and KE, approach 0 as the distance approaches infinity. But the gravitational force also approaches 0 as the distance approaches infinity ( in the way that 1/x^2 approaches 0 as x approaches infinity.)
So, if you are going to say that KE and PE become 0 at infinity, you'd also have to say that the gravitational force acting on the object becomes 0 also.
 
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Escape velocity is a good measure of the minimum rocket energy you need but it has its limitations because, for a non-orbital journey, you will mostly want to be going a lot faster than that - in order to get somewhere in a useful period of time. If you leave Earth with just a solar escape velocity, by the time you get to Neptune's orbit, you would be going pretty slowly (and it would take you a long time). Leaving the Solar System is always done using a slingshot orbit so you can't really compare the theoretical case of a rocket escaping from Earth with just its own fuel AND making it out of the Solar System too.
If you look at the orbital speeds of the planets, you find that Neptune's speed is about 1/6 of Earth's speed and that gives you an idea of the relative speeds of a simple projectile at those radii.
If you consider that gained Gravitational Potential Energy will be lost Kinetic Energy on the way out, going four times as far out as Neptune would involve halving the speed.
The speed of Voyager craft is about three times the orbital speed of Neptune and, as the graph in that link shows, it's hardly slowing down at all because it started off (with a little slingshot help) with a much higher speed than escape velocity from Earth orbit. They went past Neptune in the late 1980s iirc and are passing the heliopause now.
 
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Thanks guys, makes sense to me now.
 
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PeroK said:
What non-zero velocity "at infinity" does the object need in order not to fall back?
The answer is, of course, 0 ;-).

The solutions for the Kepler problem for ##E=0## are parabolae, i.e., unbound trajectories. For the zero angular-velocity case the bodies move radially away from each other approaching 0 velocity at infinite distance.

Proof: The solution of the radial equation of motion for ##L=0## and ##E=0##,
$$\frac{\mu}{2} \dot{r}^2-\frac{\alpha}{r}=0 \quad \text{with} \quad \alpha=\gamma m_1 m_2, \quad \mu=\frac{m_1 m_2}{m_1+m_2}$$
is (using Mathematica ;-))
$$r(t)=\left (r_0^{3/2} +\sqrt{\frac{9 \alpha}{2m}} t \right)^{2/3}.$$
 
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  • #10
vanhees71 said:
The answer is, of course, 0 ;-).
Yeah, but zero does not satisfy the condition to be non-zero. Maybe just approximately.
 
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  • #11
JoeyBob said:
I understand that the final potential energy is 0
Janus said:
As already pointed out the final PE and KE approach 0
In contrast to the OP, I get why KE is approaches zero at infinity, but why isn't PE equal to approaching ##mv_{init}^2/2## ? ##PE=mgd## is too simplistic, assuming ##g## as a constant.
sophiecentaur said:
If you consider that gained Gravitational Potential Energy will be lost Kinetic Energy
like that.
 
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  • #12
hmmm27 said:
In contrast to the OP, I get why KE is approaches zero at infinity, but why isn't PE equal to approaching ##mv_{init}^2/2## ?
The difference between the initial potential energy and the final potential energy approaches ##mv_{init}^2/2## (when ##v_{init}## is exactly equal to the escape velocity from the initial height) as the kinetic energy approaches zero. We have made the arbitrary but convenient (when grinding through the algebra) choice to set the potential energy at infinity to zero; thus the initial potential energy is negative.
##PE=mgd## is too simplistic, and assumes that ##g## as a constant
True, but this just means that to calculate the potential we have to integrate the non-constant force over the distance instead of simply multiplying a constant force by the distance. (Actually, that latter calculation is an integral too, it just so happens to immediately simplify down to a multiplication, which is why it's taught in intro classes where the students may not have already learned calculus)
 
  • #13
hmmm27 said:
PE=mgd is too simplistic, assuming g as a constant.
It not just "too simplistic"; it totally wrong in the context of Escape Velocity. Gravitational Potential (Energy per unit of mass) is:
E = MG/r
where M is the mass of the central attractor and G is the universal gravitational constant. You can only use g when you are very near a planet and where you can also treat the ground as flat etc. etc.. To understand orbits and trajectories in space you would never start with mgh.
 
  • #14
The total energy, of course, reads
$$E=\frac{m}{2} \vec{v}^2-\frac{\gamma m M}{r}.$$
 
  • #15
nasu said:
Yeah, but zero does not satisfy the condition to be non-zero. Maybe just approximately.
The question was what's the minimal total energy that the particle escapes when shot radially away (angular momentum 0). The answer to that question is exactly 0 (not only approximately). It's also easy to see by drawing the potential and some constant total energy lines in the same diagram. Then you'd not even need to solve the equation of motion to get this result. You just read it off from the diagram, considering that the physically allowed region is given by ##V(r) = E-T \leq E## since ##T=m v^2/2 \geq 0##.
 
  • #16
vanhees71 said:
The question was what's the minimal total energy that the particle escapes when shot radially away (angular momentum 0).
The question was:
PeroK said:
What non-zero velocity "at infinity" does the object need in order not to fall back?
 
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  • #17
Then an infinitesimal velocity is sufficient. If it's directed away from the other body both bodies just fly appart forever. If it's directed towards the other body the bodies crash together at some time ;-)).
 
  • #18
The mention about zero being just approximately non-zero was intended as a joke. Sorry.😀
 
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  • #19
kuruman said:
You are correct. When the kinetic energy drops to zero, the mass will fall back or orbit around the Earth. Gravity is a long range force that acts on masses even if they are in a galaxy far, far away.

You might think of the escape velocity as the threshold value that separates bound from unbound systems. If the initial kinetic energy of the mass is greater that ##\frac{1}{2}m v_{\text{esc}}^2##, then the mass will always have some kinetic energy left no matter how far it is from the Earth and the mass is considered no longer bound to the Earth. In another thread you have indicated that you are in a chemistry-related field. Think of the quantity ##\frac{1}{2}m v_{\text{esc}}^2## as the gravitational analogue of the ionization energy.
so actually we are considering satellite and Earth as a system but when satellite breaks the limit to infinty its no longer the part of the system?
 
  • #20
hxlfbloodpxince said:
so actually we are considering satellite and Earth as a system but when satellite breaks the limit to infinty its no longer the part of the system?
I would not use those words. We are free to draw system boundaries where we please. The distinction is between a pair of objects that continue separating further and further forever (an unbound system) and a pair of objects that never move more than a particular distance apart (a bound system).
 
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  • #21
hxlfbloodpxince said:
so actually we are considering satellite and Earth as a system but when satellite breaks the limit to infinty its no longer the part of the system?
To elaborate on @jbriggs444's reply: We can always consider an Earth and a satellite as a system. If the satellite orbits the Earth, it is a bound system in which the total energy of the system is negative. If the satellite "breaks the limit to infinity", it is not a bound system and the total energy of the system is greater than (or equal) to zero. In either case of energy accounting, the assumption is that the kinetic energy of the Earth is zero.

I think it is fair to say that Halley's comet forms a bound system with the Sun but not with the Earth. However, Earth, Sun and Halley's Comet, and the rest of the planets and asteroids too, form a bound system.
 
  • #22
vanhees71 said:
If it's directed towards the other body the bodies crash together at some time ;-)).
That is unless some small extra amount of energy is supplied to modify the trajectory into an elliptical orbit. You always need a second burst in a tangential direction at some stage.
 

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