Gravitation and planetes: exercise

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Homework Help Overview

The discussion revolves around a physics problem involving two planets, A and B, where an astronaut throws a ball vertically upward on each planet and measures the maximum height reached. The problem requires calculating the ratio of the planets' radii and densities, as well as the rotation period of planet B based on gravitational effects.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants explore the relationship between gravitational potential energy and height to derive ratios of radii and densities. There is discussion about the correctness of these ratios, especially considering the assumption of equal masses for the planets. Questions arise regarding the role of density in these calculations and how to approach the third part of the problem involving centripetal acceleration.

Discussion Status

Some participants have provided tentative solutions for the first two parts of the problem, while others question the assumptions made, particularly regarding the densities of the planets. There is ongoing exploration of how to approach the third part, with suggestions to consider the effects of rotation on gravitational acceleration.

Contextual Notes

Participants note that the masses of the two planets are equal, which is a crucial assumption for the calculations. There is also a discussion about the implications of centripetal acceleration on gravitational measurements at different points on the same planet.

RHK
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This is my first topic. I'm sorry for my english: that is not my language.
On the planet A, sferically symmetric and with no atmosphere, an astronaut on one pole throws in vertical upwards, a little ball giving to it a certain velocity: this ball reaches the maximum height of 25 cm.
The same thing is done on another planet, B, equal in mass to the planet A, and then the ball reaches the maximum height of 4 m.
Requests:
(i) to calculate the planetes radii ratio
(ii) to calculate the planetes densities ratio, with the hypothesis that the planets are uniform.

Successively, the astronaut make the same experiment on the B planet, this time on the equator, verifying that the ball reaches the height of 8 m.

(iii) calculate the rotation period of the planet, supposing that the mass of the planet is 10^27 g and its radius is 5000 km.

Temptative of solution:
(i) We know that E=mgh, so h=E/mg. Writing down the same equation for the two planetes, the following ratio is obtained: (hA/hB)=(R_A/R_B)^2 = 1/16

(ii) The density rho is writable as rho=M/V, where V=(4pi)/R^3, than (rhoA/rhoB)=(R_B/R_A)^3=64

Is this right? And then, how can i proceed for the third point?
Thanks a lot.
 
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the following ratio is obtained: (hA/hB)=(R_A/R_B)^2 = 1/16
......

chech the working in obtaining the above. I do not think it is correct if the densities of the two planets are not the same.
 
Thread moved to homework forums.
 
grzz said:
the following ratio is obtained: (hA/hB)=(R_A/R_B)^2 = 1/16
......

chech the working in obtaining the above. I do not think it is correct if the densities of the two planets are not the same.

What do you mean? How can density enter to play?
Thanks
 
RHK said:
What do you mean? How can density enter to play?
Thanks
If you show how you got the ratio of the heights then I can try to find if the method is correct.
 
This is my temptative for the first point:

E_A=m*g_A*h_A, so: h_A=E_A / m*g_A

E_B=m*g_B*h_A, so: h_B=E_B / m*g_B

Then it's possible to write: h_A / h_B = g_A / g_B

where g=(G M)/R^2 and so: (hA/hB)=(R_A/R_B)^2 = 1/16
What do you think about?
 
Note that M is the mass of the planet. but there are TWO planets and you have to distinguish between them - planet A and planet B.
 
I'm sorry: in the exercise text above the two planets masses are equal.
I've fixed the text.
 
Then I think that i and ii are correct.
As regards iii note that the rotation of the planet causes the acc due to gravity to reduce from that at the pole.
Use F = ma where a is the centripetal acc of a point on the equator towards centre of planet.
 
  • #10
Yes, i also thought at that.
But i can not start the problem: F=ma for the centripetal acceleration, where a=R*w^2 and w is related to the period. But i can not proceed...
 
  • #11
Is not the centripetal acc the reason that the acc due to gravity reduced by half from that at the pole?
 
  • #12
grzz said:
Is not the centripetal acc the reason that the acc due to gravity reduced by half from that at the pole?

Yes, of course it is.
But i don't get the point: I have to build another system with two equation, one for the pole and another one for the equator?
 
  • #13
Is it right to suppose a new system, with other two heights (a system for the same planet, with different heights at the pole and the equator)?
In this case i think that at the equator the acceleration is g+a_c isn't it?
 
  • #14
RHK said:
i think that at the equator the acceleration is g+a_c isn't it?

Since g[itex]_{equator}[/itex] = (1/2)g[itex]_{pole}[/itex]
then g[itex]_{pole}[/itex]= 2R[itex]\omega[/itex][itex]^{2}[/itex]
 
  • #15
I don't understand just a thing: the acceleration at the equator is ONLY the centripetal one? Why?
 
  • #16
g[itex]_{equatir}[/itex] = GM/(R[itex]^{2}[/itex]) - R[itex]\omega[/itex][itex]^{2}[/itex]
 
  • #17
That's ok :)
Thanks a lot
 

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