Gravitational potential energy near the earth

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Discussion Overview

The discussion revolves around gravitational potential energy near the Earth, specifically the formula U = mgh and its implications when considering movement upwards and downwards. Participants explore the definitions, calculations, and potential inconsistencies in the application of the formula in different scenarios.

Discussion Character

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

Main Points Raised

  • Some participants express confusion regarding the application of the gravitational potential energy formula U = mgh when moving upwards versus downwards, questioning the consistency of results.
  • One participant notes that using U(x) = -W(x0 to x) leads to different potential energy values depending on the direction of movement, suggesting a contradiction in the results.
  • Another participant emphasizes the importance of keeping track of signs in the calculations, indicating that missing a minus sign can lead to incorrect interpretations of potential energy changes.
  • Several participants discuss the relationship between work done by gravity and the work done by an external force, highlighting the nuances of positive and negative work in different scenarios.
  • There is mention of a professor's statement regarding the nature of work done by gravity, prompting further inquiry into how this aligns with the participants' understanding of potential energy changes.

Areas of Agreement / Disagreement

Participants generally agree on the importance of sign conventions in calculations, but there remains uncertainty and disagreement regarding the reconciliation of different approaches to calculating gravitational potential energy. No consensus is reached on the implications of these calculations.

Contextual Notes

Participants highlight potential limitations in their reasoning, such as the dependence on chosen reference points and the need for clarity in defining initial and final positions during calculations.

Who May Find This Useful

This discussion may be useful for students and educators in physics, particularly those grappling with the concepts of gravitational potential energy and the mathematical treatment of work and energy in different contexts.

demonelite123
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I am a bit confused about gravitational potential energy near the earth, namely the formula given by mgh.

I know that potential energy is defined as U(x) = -W(x0 to x) where x0 is our chosen reference point. Let's take the Earth's surface as the zero point and let's travel upwards to a point x. Since mg is pointing down and my displacement is pointing up, the dot product is negative so W(x0 to x) = -mgx. Therefore, U(x) = -(-mgh) = mgh.

however, let's say i want to travel downwards instead. then since mg is pointing down and my displacement is also pointing down, the dot product is positive this time so W(x0 to x) = mgx (x is negative). but then U(x) = -(mgx) = -mgx. If i say travel downwards from x = -2 to x = -4, i get U(-4) - U(-2) = mg(4) - mg(2) > 0, which doesn't make sense since if i am going downwards, shouldn't my change in potential energy be negative?
 
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Do you have a higher PE on the ground or higher up?
 
Using the formula U(x) = -mgx derived from taking the work going from the zero point (ground) to a point below the surface, it seems that points above the surface have negative potential.

what i don't understand is why both approaches don't give me the same U(x). for U(x) = mgx, i traveled upwards so i can only use positive values of x (above the surface). If i want to use negative values of x, I travel downwards but i come up with U(x) = -mgx which seems to contradict with the function i got from traveling upwards since taking points above the surface, one gives me a positive PE and the other gives me a negative PE.

is there a way to reconcile them?
 
demonelite123 said:
I am a bit confused about gravitational potential energy near the earth, namely the formula given by mgh.

I know that potential energy is defined as U(x) = -W(x0 to x) where x0 is our chosen reference point. Let's take the Earth's surface as the zero point and let's travel upwards to a point x. Since mg is pointing down and my displacement is pointing up, the dot product is negative so W(x0 to x) = -mgx. Therefore, U(x) = -(-mgh) = mgh.

however, let's say i want to travel downwards instead. then since mg is pointing down and my displacement is also pointing down, the dot product is positive this time so W(x0 to x) = mgx (x is negative)

You lost a minus sign here.
 
U=-W, W=F.d

F=-(mg)j
d=(y-y0)j if we go "up" (final minus initial)
... since y0<y, d>0 - for later reference, put h=|d|
U= -(-mg)[+(y-y0)] = mgh

if you go "down" the d=(y0-y)j = - (y-y0)j
U=-(-mg)[-(y-y0)] = -mgh

Keeping track of the minus signs is, indeed, the trick to keeping things consistent.
 
demonelite123 said:
however, let's say i want to travel downwards instead. then since mg is pointing down and my displacement is also pointing down, the dot product is positive this time so W(x0 to x) = mgx (x is negative). but then U(x) = -(mgx) = -mgx.
As others have already explained, you are essentially double counting the minus sign.

ΔU = -(F)*(Δx) = -(-mg)*(Δx) = (mg)*(Δx)

When Δx is positive, ΔU is positive; when Δx is negative, ΔU is negative.
 
@demonelite: this sound good to you?
 
Simon Bridge said:
@demonelite: this sound good to you?

sorry about my late response. I'm still a bit confused. for the case "going up" i agree that F = (-mg)j and d = (y - y0)j since as you said it was final point (y) - initial point (y0).

but for the "going down" case, F = (-mg)j but how come d = (y0 - y)j? isn't final point - initial point still y - y0?

thanks for all the replies so far everyone.
 
demonelite123 said:
sorry about my late response. I'm still a bit confused. for the case "going up" i agree that F = (-mg)j and d = (y - y0)j since as you said it was final point (y) - initial point (y0).

but for the "going down" case, F = (-mg)j but how come d = (y0 - y)j? isn't final point - initial point still y - y0?

In the "going down" case the object is going "from" y "to" y0, so final point - initial point is y0 - y which is negative.
 
  • #10
Thank you jtbell :)
@deminelite123 - since y > y0, in order to go down you have to start at y.
 
  • #11
Simon Bridge said:
Thank you jtbell :)
@deminelite123 - since y > y0, in order to go down you have to start at y.

ah ok. what you said earlier makes sense now. thanks!
 
  • #12
Like everyone said, you missed a minus sign. :)
 
  • #13
ah ok. what you said earlier makes sense now. thanks!
No worries, happens to the best of us.

In general, it is a good discipline to have the same labels refer to the same things. In this case: locations - when you were going down, you forgot to account for your y0>y so that y-y0 < 0. Try it with a diagram.
 
  • #14
Wait a second... The professor at MIT said that when I do positive work, gravity does negative work and when I do negative work, gravity does positive work. How does this make sense. When I do negative work from A to B then gravity is also doing negative work right? since it is -mg?
 
  • #15
Keep track of the directions ...

If you lower a mass at constant speed, then you are exerting a force in the opposite direction to the displacement, and gravity is acting in the same direction as displacement.

In your example, A must be higher than B so the displacement from A to B is negative.
 
  • #16
Thanks a lot
 
  • #17
Thanks!
 
  • #18
No worries.
Tracking the minus signs can be tricky - especially if things are slowing down as well as changing direction.
 

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