| New Reply |
Gravitation potential energy |
Share Thread |
| Jan5-13, 01:30 PM | #1 |
|
|
Gravitation potential energy
Hello,
Can anybody please explain me: While going through gravitation potential energy, I came across: F=G.m1.m2/r^2 From there it follows: g=-GM/r^2.r How does it follow? Specially the -G case? -- Shounak |
| Jan5-13, 02:00 PM | #2 |
|
|
They're defining the "gravitational field" to be:
[tex]\mathbf{g}=-\frac{GM}{r^3}\mathbf{r}[/tex]. Basically this means that if you take the gravitational field at a point, [itex]\mathbf{g}(\mathbf{r})[/itex], and you multiply it by the mass [itex]m[/itex] of an object at that point, you get the force on that object: [tex]\mathbf{F}=m\mathbf{g}[/tex] The reason there's a "-" sign in the definition of the field is because the vector [itex]\mathbf{r}[/itex] points out from the "gravitating" mass. Since the gravitational field effectively tells you the acceleration that small, free particles experience, the [itex]\mathbf{g}[/itex] needs to point in the opposite direction of [itex]\mathbf{r}[/itex] (because gravity is attractive). |
| Jan5-13, 02:25 PM | #3 |
|
|
It explains:
"We know that the further you get from an object, the higher your GPE relative to it. (As something must have done more work against gravity to get you there). Thus when you are infinitely far away, you have as high a GPE relative to it as possible. We choose (arbitrarily) to make the value of GPE of all bodies at infinity zero. Then since this is the highest value of GPE, all real values of GPE (closer than infinity) must be negative. Therefore the minus sign in the equation is NOT optional; it must always be included and all values of potential energy in a gravitational field are negative. (This is not the case when we come on to electric fields, because they can be repulsive too)." I want to understand "all real values of GPE (closer than infinity) must be negative." What does that mean? You have mentioned that the vector r points out from the gravitating mass. If I draw a diagram, a point m, the lines will be pointing out from the point......That means the vectors is not drawing inwards rather outwards, hence negative right? Is there any difference between POTENTIAL ENERGY AND GRAVITATIONAL POTENTIAL ENERGY? Thanks, -- Shounak |
| Jan5-13, 02:43 PM | #4 |
|
|
Gravitation potential energy
Hi Shounak!
![]() (and potential energy is minus the work done by a conservative force) gravitational potential is potential energy per mass (just as electric potential is potential energy per charge) we measure it relative to a test mass at infinity, whose PE we define to be zero since nothing can be at infinity (or further away!), that means that all real values of gravitational potential energy must be less than zero for electric potential energy, we use a (positive) test charge at infinity … so for any real positive charge, the electric potential energy will also be less than zero, but for any real negative charge, the electric potential energy will always be greater than zero ![]()
|
| Jan5-13, 02:53 PM | #5 |
|
|
Ok, I got it now. It is just as we want to avoid infinite, it is better even to get -ve values. If we consider all the non zero values it would be extremely difficult for us to compute. Am I right?
What I am trying is just to draw a vector with points pointing outwards and hence -G. |
| Jan5-13, 03:12 PM | #6 |
|
|
Hi Shounak!
![]() we're not trying to avoid infinity it's just that we want a convenient formula if we chose radius R as our "zero" level of potential energy, then the magnitude of the potential energy at a general distance r would be GM(1/R - 1/r) that's a rather cumbersome formula*, so we prefer to put R = ∞, which makes it GM(1/∞ - 1/r), = GM(0 - 1/r), = -GM/r ![]() * of course, if we're happy with an approximation … which we usually are … then we can use R, eg as the radius of the EarthDerivation of mgh: [tex]\Delta (PE)\ =\ \Delta(-mMG/r)[/tex] [tex]=\ \frac{-mMG}{r_{earth}\,+\,H\,+\,h}\ -\ \frac{-mMG}{r_{earth}\,+\,H}[/tex] which is approximately: [tex]\frac{-mMG(H\,-H\,-\,h)}{r_{earth}^2}\ =\ \frac{mMGh}{r_{earth}^2}\ =\ mgh[/tex]
|
| Jan5-13, 03:29 PM | #7 |
|
|
Thank you very much. It cleared me all up. Just 2 more questions:
Wikipedia writes: "The singularity at r=0 in the formula for gravitational potential energy means that the only other apparently reasonable alternative choice of convention, with U=0 for r=0, would result in potential energy being positive, but infinitely large for all nonzero values of r, and would make calculations involving sums or differences of potential energies beyond what is possible with the real number system. Since physicists abhor infinities in their calculations, and r is always non-zero in practice, the choice of U=0 at infinity is by far the more preferable choice, even if the idea of negative energy in a gravity well appears to be peculiar at first." Hence I was asking about avoiding infinity. Secondly, if you can please explain H and h. Thanks. |
| Jan5-13, 03:37 PM | #8 |
|
|
![]() h is the extra height above that. ![]() (so if you move a height h above H, the PE is +mgh) |
| Jan5-13, 03:40 PM | #9 |
|
|
One more thing:
U=-m(G.M1/r1+G.M2/r2) Are you putting GM(1/R - 1/r) in here or somewhere else? |
| Jan5-13, 03:44 PM | #10 |
|
|
It also says:
"the choice of U=0 at infinity is by far the more preferable choice, even if the idea of negative energy in a gravity well appears to be peculiar at first" |
| Jan5-13, 03:50 PM | #11 |
|
|
what is it supposed to be? ![]() it's adding that some people find negative energy peculiar … well, that's obviously correct, because you do!! |
| Jan5-13, 03:57 PM | #12 |
|
|
What I am trying to say is:
GM(1/R - 1/r) how to put in which equation? |
| Jan6-13, 04:20 AM | #13 |
|
|
R is the (fixed) distance which you arbitrarily choose as your "zero" level for potential energy
|
| Jan7-13, 02:47 PM | #14 |
|
|
To sum up:
If r is non-zero, then there cannot be infinity, hence r is always non zero. If U i.e. GPE =0 at infinity then anything less than zero is always negative, hence it is negative. Right? |
| Jan7-13, 05:33 PM | #15 |
|
|
![]() |
| Jan7-13, 10:52 PM | #16 |
|
|
Ok, thank you very much for clearing all the doubts and answering the questions.
I am on it. Thanks once again. |
| New Reply |
Similar discussions for: Gravitation potential energy
|
||||
| Thread | Forum | Replies | ||
| Gravitation potential energy question help | Introductory Physics Homework | 7 | ||
| Gravitation and potential energy | Introductory Physics Homework | 3 | ||
| gravitation potential energy without hieght | Introductory Physics Homework | 5 | ||
| Gravitation (Potential Energy) | Introductory Physics Homework | 4 | ||
| Gravitation Potential Energy Help | Introductory Physics Homework | 8 | ||