Time of a falling object when the force of gravity isn't constant

Click For Summary
The discussion revolves around calculating the time it takes for an object to fall towards a planet when gravitational force is not constant. Initial calculations show the object's speed at the planet's surface is approximately 10,000 m/s, with gravity varying from 10 m/s² at the surface to 2.5 m/s² at a distance of 2*10^14 meters from the center. Participants emphasize the need for a function of time, suggesting differential equations and integration to derive the relationship between velocity and distance. There are multiple attempts to clarify the gravitational equations and integrate them to find time, but some participants express uncertainty about their calculus skills. The conversation highlights the complexity of integrating variable gravitational fields and the necessity of higher-level math for accurate solutions.
  • #31
SammyS said:
Really ?

(dv/dt) (dr/dr) = (dr/dt) (dv/dr) ?

The Calculus gods have just gone nuts !

The link. Not this site.Sorry my english isn't that good.
 
Physics news on Phys.org
  • #32
Shahar said:
The link. Not this site.Sorry my english isn't that good.
@Shahar,
I was replying to Post # 28 by rcgldr .
 
  • Like
Likes Shahar
  • #33
Shahar said:
The answer in the site isn't very helpful.
You can substitute u = sqrt(r / (r0-r))
 
Last edited:
  • #34
I prefer the substitution r = r0sin2θ

Chet
 
  • #35
rcgldr said:
a = dv/dt = (dv/dt) (dr/dr) = (dr/dt) (dv/dr) = v dv/dr
SammyS said:
Really ?
Chain rule, wiki link:
http://en.wikipedia.org/wiki/Chain_rule

I fixed what I now call method 1 and method 2 in my previous post.
 
Last edited:
  • #36
rcgldr said:
rcgldr said:
a = dv/dt = (dv/dt) (dr/dr) = (dr/dt) (dv/dr)

Chain rule, wiki link:

http://en.wikipedia.org/wiki/Chain_rule

This is used when acceleration is a function of distance (instead of time), acceleration = a(r) = - G M / r^2.
I'm familiar with the chain rule.

It's the abuse of the notation in that set of steps that I was objecting to, in particular the (dv/dt)(dr/dr) in
dv/dt = (dv/dt) (dr/dr) = (dr/dt) (dv/dr) .​

dv/dt is not a fraction. It represents a derivative in Leibniz's notation . It is very handy for implementing the chain rule.

You don't simply take ##\displaystyle\ \frac{dv}{dt}\,,\ ## then multiply numerator & denominator by ##\ dr\ ## like so, ##\displaystyle\ \frac{dv}{dt}\frac{dr}{dr}\ ## and then swap locations of dr & dt or dv to get ##\displaystyle\ \frac{dv}{dr}\cdot\frac{dr}{dt}\ ##.

If v is a function of r, and in turn, if r can be expressed as a function of t, then ##\displaystyle\ \frac{dv}{dt}=v'(r)\cdot r'(t)=\frac{dv}{dr}\cdot\frac{dr}{dt}\ ##.
 
  • #37
rcgldr said:
Maybe if I had paid attention to the thread title ... (brain fade on my part). In that case, can you delete all of the posts with the solutions? Or if you give me an OK, I can go back and empty out all my previous posts, leaving a comment about waiting for feedback. Perhaps the OP hasn't visited this thread since those posts were added.
Good suggestion. I will go back and delete and edit where appropriate. In the Country where the OP lives, it is a little before sunrise now, so maybe he hasn't seen any of the posts yet.

Chet
 
  • Like
Likes Shahar
  • #38
Update :I am tring to solve this using basoc calculus. So I'm tring to find the a(t) using a(x). Because v'(t)=a(t). I'm a bit stuck but I think I'm able to solve it.
 
  • #39
Converting a(x) to a(t) is difficult, and requires finding the time (and everything else) first. The correct approach is in the thread now, you just have to integrate it. If you don't know how to calculate integrals then I don't see a way to solve the problem.
 
  • #40
mfb said:
Converting a(x) to a(t) is difficult, and requires finding the time (and everything else) first. The correct approach is in the thread now, you just have to integrate it. If you don't know how to calculate integrals then I don't see a way to solve the problem.

II integrated a(x) and it gave me , well...IIts not the average velocity.
mfb said:
Converting a(x) to a(t) is diffi
mfb said:
Converting a(x) to a(t) is difficult, and requires finding the time (and everything else) first. The correct approach is in the thread now, you just have to integrate it. If you don't know how to calculate integrals then I don't see a way to solve the problem.

I integrated a(x) and v(x). The big problem is that I don't really understand differentials.
 
  • #41
Shahar said:
II integrated a(x) and it gave me , well...IIts not the average velocity.
I integrated a(x) and v(x). The big problem is that I don't really understand differentials.
If you don't understand differentials, how can you say that you have done an integration? Have you learned how to do integration in your courses yet? Have you learned about doing integrations by using algebraic or trigonometric substitution?

Chet
 
  • #42
Chestermiller said:
If you don't understand differentials, how can you say that you have done an integration? Have you learned how to do integration in your courses yet? Have you learned about doing integrations by using algebraic or trigonometric substitution?

Chet

Because I can't solve this problem without knowing how to integrate I learned integrations using algebraic substitution.
 
  • #43
What about doing it graphically? Is that allowed?

Chet
 
  • #44
Don't integrate v(x), integrate 1/v(x).
 
  • #45
Chestermiller said:
What about doing it graphically? Is that allowed?

Chet

My question is not homework. It's too advance to be 10th grade homework. In the original question they asked us to find a time range for the falling object .(1414<t<2828 seconds) .
I just wanted to find the precise time it takes to an object moving with changing gravitational acceloration to get from A to B.

mfb said:
Don't integrate v(x), integrate 1/v(x).

I tried that,
 
Last edited:
  • #46
This problem starts off with an equation for acceleration as a function of position. The sequence here is to generate an equation for velocity as a function of position, then time as a function of position, then invert this to an equation for position as a function of time, take the derivative to get velocity as a function of time, and another derivative to get acceleration as a function of time. However at some point in this process, you may not be able to continue, either due to an equation that can't be integrated, or an equation for time as a function of position that can't be inverted to an equation for position as a function of time.

If you wan't to get an idea of how this process works, try a simpler case like a(x) = -x (acceleration as a function of position), with an initial position of 0 and initial velocity of 1.
 
  • #47
rcgldr said:
This problem starts off with an equation for acceleration as a function of position. The sequence here is to generate an equation for velocity as a function of position, then time as a function of position, then invert this to an equation for position as a function of time, take the derivative to get velocity as a function of time, and another derivative to get acceleration as a function of time. However at some point in this process, you may not be able to continue, either due to an equation that can't be integrated, or an equation for time as a function of position that can't be inverted to an equation for position as a function of time.

If you wan't to get an idea of how this process works, try a simpler case like a(x) = -x (acceleration as a function of position), with an initial position of 0 and initial velocity of 1.

This is what I'm doing right now.
It will take some time.
 
  • #48
Shahar said:
My question is not homework. I just wanted to find the precise time it takes to an object moving with changing gravitational acceloration to get from A to B.
Well you already have the solution for time versus position in post #28 (the link to the math site), but in the form of a very complicated equation resulting from integration of velocity versus position. update - the rest of this post about substitutions was moved to post #50 to combine the important equations into a single post.
 
Last edited:
  • #49
rcgldr said:
This problem starts off with an equation for acceleration as a function of position. The sequence here is to generate an equation for velocity as a function of position, then time as a function of position, then invert this to an equation for position as a function of time, take the derivative to get velocity as a function of time, and another derivative to get acceleration as a function of time. However at some point in this process, you may not be able to continue, either due to an equation that can't be integrated, or an equation for time as a function of position that can't be inverted to an equation for position as a function of time.

If you wan't to get an idea of how this process works, try a simpler case like a(x) = -x (acceleration as a function of position), with an initial position of 0 and initial velocity of 1.
Yeah, its impossible to get v(t). I'm now just searching for x(t).
I know there are a lot of solutions here but I don't really understand them. I think I have to get to them myself to fully understand this.
 
  • #50
Shahar said:
I'm now just searching for x(t). I know there are a lot of solutions here but I don't really understand them. I think I have to get to them myself to fully understand this.
You need to get t(r) first, by integrating the equation you got in post #3, which I redid in post #28.
The left term, - sqrt(r0 / (2 G M)) is a constant, so the issue here is integrating the right term, sqrt(r / (r0 - r)) dr .
r0 is the initial position, in this case 10^14 meters.

$$-\sqrt{\frac{r_0}{2 \ G \ M}}\sqrt{\frac{r}{r_0 \ - \ r}} \ dr = dt$$
The substitutions suggested in posts #33 and #34 will result in a much simpler equation, but you'll have to convert position into the substituted values to order to calculate the time.

post #33 substitution (r0 is a constant):
$$ u = \sqrt{\frac{r}{r_0 \ - \ r}} $$
$$r = r_0 - \frac{r_0}{1 + u^2} $$
post #34 substitution (this one is simpler):
$$ r = r_0 \ sin^2(θ) $$
$$θ = {sin^{-1}\left ( \sqrt{\frac{r}{r_0}} \right )} $$
You need to determine what dr (derivative of r) is when using either substitution.

Use the post #34 substitution which is simpler than the post #33 substitution. The resulting integrals with either substitution are complicated enough that you'll probably want to look up the solution using a table of integrals (old timers may remember the CRC books with tables of integrals) or a website like WolframAlpha to solve, but those resulting integrals will be much simpler than the one from post #28.
 
Last edited:
  • #51
Hi Shahar,

Are you still out there, and are you still interested in pursuing the solution to this problem? Is anyone else out there interested in having rcgldr help them do this integration? rcgldr would like to complete the solution so that he does not have to save it in his computer files. If I don't hear back from someone on this by Monday, I'm going to release rcgldr to provide his analysis. Then I'm going to close this thread.

Chet
 
  • Like
Likes Shahar
  • #52
Chestermiller said:
Hi Shahar,

Are you still out there, and are you still interested in pursuing the solution to this problem? Is anyone else out there interested in having rcgldr help them do this integration? rcgldr would like to complete the solution so that he does not have to save it in his computer files. If I don't hear back from someone on this by Monday, I'm going to release rcgldr to provide his analysis. Then I'm going to close this thread.

Chet

I found a way to get the time.But because I have to learn more calculus I can't derive an X(t) function.
I'm learning calculus alone amd when I will understand how to solve a deferential equation Ill try to derive an X(t) function.
So I think rcgldr can release his analysis now.
 
  • #53
Shahar said:
I found a way to get the time.But because I have to learn more calculus I can't derive an X(t) function.
So I think rcgldr can release his analysis now.
Thanks. Personally, I don't see how you could get the time without automatically also getting X(t) as a byproduct, but that's just me.

OK, regldr. You're free to proceed.

Chet
 
  • #54
Chestermiller said:
Thanks. Personally, I don't see how you could get the time without automatically also getting X(t) as a byproduct, but that's just me.

OK, regldr. You're free to proceed.

Chet

I used averages(V , a) .
If I just combine all of the steps into one big expression, would it be an X(t) equation?
 
Last edited:
  • #55
Shahar said:
I used averages(V , a) .
If I just combine all of the steps into one big expression, would it be an X(t) equation?
Why don't you show us what you did and how you arrived at your final answer? Then we can compare it with what rcgldr got by integration.

Chet
 
  • #56
Using conversation of energy I found V(r) => Vfinal.
And I know the function a(r) = G × M / r2.
So when V0 = 0 ,∫ a(r) dr = (Vfinal * Δt)*(Δt/Vavg) = Vfinal * Vavg.
Δt = Δx/Vavg.
 
  • #57
Shahar said:
Using conversation of energy I found V(r) => Vfinal.
And I know the function a(r) = G × M / r2.
So when V0 = 0 ,∫ a(r) dr = (Vfinal * Δt)*(Δt/Vavg) = Vfinal * Vavg.
Δt = Δx/Vavg.
OK. What you basically did here was to use a very crude approximation to the average velocity, equal to half the final velocity. This would not give a very accurate result for Δt. Please tell us what your result for Δt was so that we can compare it with what rcgldr got by doing the integration exactly.

Chet
 
  • #58
Chestermiller said:
OK. What you basically did here was to use a very crude approximation to the average velocity, equal to half the final velocity. This would not give a very accurate result for Δt. Please tell us what your result for Δt was so that we can compare it with what rcgldr got by doing the integration exactly.

Chet

I got 2000 seconds, which is the only answer that is in the limit 1414 < t < 2828 seconds.
I found that the average accelerationis 5 m/s. a0 = 2.5 m/s2 and af = 10 m/s2.
I rejected this idea twice already but becuse it's the on;y one that gives an answer in the limit I tried it again.
The answer is a bit too small, isn't it?

EDIT: I can't find any material about differentials in physics. Most of the stuff on the internet is a bit too complex for me.
Do you know a simple explanation for differentials in physics?
 
Last edited:
  • #59
Shahar said:
I got 2000 seconds, which is the only answer that is in the limit 1414 < t < 2828 seconds.
I found that the average accelerationis 5 m/s. a0 = 2.5 m/s2 and af = 10 m/s2.
I rejected this idea twice already but becuse it's the on;y one that gives an answer in the limit I tried it again.
The answer is a bit too small, isn't it?

EDIT: I can't find any material about differentials in physics. Most of the stuff on the internet is a bit too complex for me.
Do you know a simple explanation for differentials in physics?
In post #45, you indicated that you had tried plotting 1/v as a function of r, and integrating graphically to get the area under the curve, but that didn't work. Can you elaborate on this? Can you furnish the plot? We would like to find out why it didn't work for you. (It should have).

Chet
 
  • #60
Chestermiller said:
In post #45, you indicated that you had tried plotting 1/v as a function of r, and integrating graphically to get the area under the curve, but that didn't work. Can you elaborate on this? Can you furnish the plot? We would like to find out why it didn't work for you. (It should have).

Chet

I integrated 1/v(r) dr (and v(r) )and I had an expression that I cna't understand what it means.
 

Similar threads

  • · Replies 3 ·
Replies
3
Views
5K
  • · Replies 9 ·
Replies
9
Views
2K
  • · Replies 8 ·
Replies
8
Views
2K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 7 ·
Replies
7
Views
2K
  • · Replies 7 ·
Replies
7
Views
2K
  • · Replies 16 ·
Replies
16
Views
2K
  • · Replies 10 ·
Replies
10
Views
2K
  • · Replies 6 ·
Replies
6
Views
1K
Replies
17
Views
2K