The gravitating of a small mass towards a big mass

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SUMMARY

The discussion focuses on the gravitational interaction between a small mass (##m##) and a larger mass (##M##), specifically addressing the differential equation governing the motion of the smaller mass as it approaches the larger mass. The key equation derived is the gravitational potential energy expressed as ##\frac{GMm}{x} = \frac{1}{2}mv^2(x)##, leading to the velocity function ##v(x) = \sqrt{\frac{2GM}{x}}##. The participants emphasize the need to solve the differential equation ##\frac{d^2x}{dt^2}= \frac{GM}{x^2}## to determine the position and velocity as functions of time, and they highlight the importance of the initial distance from the larger mass to predict collision outcomes.

PREREQUISITES
  • Understanding of gravitational potential energy and kinetic energy concepts
  • Familiarity with differential equations and their solutions
  • Knowledge of the work-energy theorem in classical mechanics
  • Basic calculus skills, particularly in separation of variables and integration
NEXT STEPS
  • Study the method of solving second-order differential equations in classical mechanics
  • Learn about the work-energy theorem and its applications in gravitational systems
  • Explore the implications of gravitational potential energy in orbital mechanics
  • Investigate numerical methods for simulating gravitational interactions between masses
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Physics students, mechanical engineers, and anyone interested in classical mechanics and gravitational dynamics will benefit from this discussion.

brotherbobby
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Homework Statement
A large mass of ##10^8## kg is held in free space at a certain point. A small mass of 1 kg exists at a point 1000 km (##10^6\;\text{m}##) away from the larger mass at the start of motion. Answer the following questions :
(1) Write the velocity of the smaller mass as function(s) of its space coordinate and time, assuming the location of the larger mass to be at the origin, the motion taking place along a line and the start of motion to be at ##t=0##.
(2) What is the location of the smaller mass at a given time ##t##?
(3) When will the smaller mass collide with the bigger mass?
(4) With what velocity will the bigger mass collide with the smaller mass?
Relevant Equations
From Newton's gravitation formula, the acceleration due to gravity ##g=\frac{d^2x}{dt^2}= \frac{GM}{x^2}##, where ##x## is the distance of separation between the masses ##M## and ##m## at a given instant.
Gravity.png
Diagram :
I draw a picture of the problem situation and paste it to the right.

Attempt : Let me assume that the position of the smaller mass ##m## at a given instant of time ##t## is ##x(t)##.

(1) Gravitational potential energy ##\frac{GMm}{x} = \frac{1}{2}mv^2(x)##, where ##v(x)## is the velocity of the mass at that position. This simplifies to ##\boxed{v(x) = \sqrt{\frac{2GM}{x}}}##.
However, I do not know how to find the velocity as a function of the time ##t##, or ##v(t)##.
More crucially, I do not know how to solve the differential equation given in the Relevant Equations above : ##\frac{d^2x}{dt^2}= \frac{GM}{x^2}##. If I could, it would yield ##\frac{dx}{dt} = v(t)## and ##x(t)##, thereby answering questions 1 and 2 above.
Solving the differential equation would also lead to finding when will the masses collide and with what velocity, which would answers questions (3) and (4) above.

Request : A help or hint would be very welcome.
 
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For solving the differential equation, note that you have $$v(x) = \sqrt{\frac{2GM}{x}}=\frac{dx}{dt}.$$ Can you separate variables and integrate?

I am bothered by the fact that the radius of the larger sphere is not given. How will one know where the smaller mass is when it collides? Check your source to see if you missed it. If the radius is not given, assume that it is ##R## and proceed.

On edit
Actually it should be $$\frac{dx}{dt} = -\sqrt{\frac{2GM}{x}}$$ because the distance ##x## decreases as time increases.
 
Last edited:
brotherbobby said:
(1) Gravitational potential energy ##\frac{GMm}{x} = \frac{1}{2}mv^2(x)##, where ##v(x)## is the velocity of the mass at that position.
GPE is not ##\frac{GMm}{x}## (you forgot something) and there is no law that says GPE equals KE (or -KE). What does it say?
 
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Can you prove this?
If the object with mass ##m \ll M## is dropped at rest at the distance ##x_1## from the centre of the object with mass ##M##, then
## \dfrac{mv^2}{2} - \dfrac{GMm}{x} = -\dfrac{GMm}{x_1}## where ##x \leq x_1## and ##v## is the velocity at position ##x##.
Hint: work-energy theorem.
 

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