How to find the L1 (First Langrangian Point) between the Earth and the Moon?

  • Thread starter Thread starter ootz0rz
  • Start date Start date
  • Tags Tags
    Earth Moon Point
AI Thread Summary
To find the L1 point between the Earth and the Moon, the gravitational forces from both celestial bodies must be equal. Given the masses of the Earth (5.98x10^24 kg) and the Moon (7.35x10^22 kg), the distance between them is 3.84x10^5 km. By setting the gravitational forces equal, a ratio can be derived, leading to the conclusion that the distance from the Earth to the L1 point is approximately 3.456x10^5 km. The calculations confirm that the method used to arrive at this solution is valid.
ootz0rz
Messages
3
Reaction score
0
Hi everyone :) I'm new to the forums, need some help with a homework question I just can't seem to be able to get...

The question as described in my book is as follows:

The mass of the moon is 7.35x10^22 kg. At some point between Earth and the Moon, the force of Earth's gravitational attraction on an object is canceled by the Moon's force of gravitational attraction. If the distance between the Earth and the moon (center to center) is 3.84x10^5 km, calculate where this will occur, relative to the Earth.

Earlier in the book, I am given the mass of the Earth as 5.98x10^24 kg and I am supposed to use that.

What I've got so far (not sure if any of this is correct at all... :frown:):

F_g = \frac{GMm}{r^2}

Where...
G = 6.67x10^{-11} \frac{Nm^2}{kg^2}
M = The larger mass
m = the smaller mass
r = radius

Problem is, we are not given an object being at the L1 point (which I will refer to as X), so it can't be used for that. It can be used however to find the force of gravity from Earth that is acting on the moon at that radius. But anyways, I needed a way to remove the m variable, so I replaced Fg with an equivalent equation:

\frac{mv^2}{r} = \frac{GMm}{r^2}

m and one r cancels out and we get

\frac{GM}{r} = v^2

this however introduces a new unknown variable into, v - being the velocity
However, v can be expressed as

v = \frac{2 \pi r}{T}
therefore v^2 \Rightarrow v^2 = \frac{4 \pi^2 r^2}{T^2}

T is the period it takes to complete one revolution, yet another fun unknown...

at this point we have
\frac{GM}{r} = \frac{4 \pi^2 r^2}{T^2}

Then if we bring r^2 to the left side...

\frac{GM}{r^3} = \frac{4 \pi^2}{T^2}

I could further juggle the equation so it would solve for r...however...I'm not sure what to do with the T variable

That's about as far as I was able to get :/ Any help would be greatly appreciated.
Thank you :)
 
Last edited:
Physics news on Phys.org
ootz0rz said:
The mass of the moon is 7.35x10^22 kg. At some point between Earth and the Moon, the force of Earth's gravitational attraction on an object is canceled by the Moon's force of gravitational attraction. If the distance between the Earth and the moon (center to center) is 3.84x10^5 km, calculate where this will occur, relative to the Earth.

Earlier in the book, I am given the mass of the Earth as 5.98x10^24 kg and I am supposed to use that...
Welcome to PF!

You just have to find the point at which the force of gravity on an object from the moon is equal and opposite to the force of gravity on the earth. Take the distance between the Earth and moon as d. So r_e = d - r_m

AM
 
I just tried doing this another way, as follows (and was able to successfully solve for "r" using this method). Can someone please look it over? :)

We assume an object is at the L1 point (the point where the gravitational fields of the two objects cancels out). We will call this object X

r is the radius between the Earth and the Moon
We will call r_1 the point from the center of the Earth to x and r_2 the point from x to the center of the moon
Therefore
(1)r = r_1 + r_2

Using this assumption of the object X we get..

F_g = \frac{G m_1 x}{r^2_1} where m_1 is the mass of the earth, and x is the mass of object X
F_g = \frac{G m_2 x}{r^2_2} where m_2 is the mass of the moon, and x is the mass of object X

Since we know that, at the point where the object X is situated, the gravitiational pull from both the Earth and the Moon will be equal, we can equate the above two equations getting the following:
(2)\frac{G m_1 x}{r_1^2} = \frac{G m_2 x}{r_2^2}

Now, we obtain a ratio between m_1 and m_2 so we can express m_1 in terms of m_2

\frac{m_1}{m_2} = 81 (Note: I rounded to 81 just to make typing it up here easier...)
Therefore, m_1 = 81m_2

Now, going back to equation (2), G and x will cancel out and we replace r_1 with r-r_2 (from equation (1)) leaving us with:
\frac{81m_2}{(r-r_2)^2} = \frac{m_2}{r_2^2}

m_2 will cancel out:
\frac{81}{(r - r_2)^2} = \frac{1}{r_2^2}

81 = \frac{(r - r_2)^2}{r_2^2}

i take the square root of both sides, and put the denominator on the left side
9 r_2 = r - r_2

10 r_2 = r

r_2 = r / 10

r_2 = 3.84*10^{4}

Since r_1 = r - r_2

r_1 = 3.84*10^{5} - 3.84*10^{4}

r_1 = 3.456*10^{5}

my actual answer is a little bit different since i rounded differently for posting on here...but i'd like to know if the method is correct?
Thanks again in advance.
 
Last edited:
Andrew Mason said:
Welcome to PF!
Thank you :)
Andrew Mason said:
You just have to find the point at which the force of gravity on an object from the moon is equal and opposite to the force of gravity on the earth. Take the distance between the Earth and moon as d. So r_e = d - r_m
I thought of doing something similar, and my results are posted above. I was writing the post up as you replied :)
 
Thread 'Collision of a bullet on a rod-string system: query'
In this question, I have a question. I am NOT trying to solve it, but it is just a conceptual question. Consider the point on the rod, which connects the string and the rod. My question: just before and after the collision, is ANGULAR momentum CONSERVED about this point? Lets call the point which connects the string and rod as P. Why am I asking this? : it is clear from the scenario that the point of concern, which connects the string and the rod, moves in a circular path due to the string...
Back
Top