Calculating Distance from Center of Earth to Point with 0.50g Acceleration

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To calculate the distance from the Earth's center to a point where gravity is 0.50g, the relevant gravitational force equation is G * (M/r^2) = 0.5g, where M is the mass of the Earth. The mass affecting gravity at that point is only the mass below it, which can be expressed in terms of Earth's average density. The approach involves solving for r using the derived relationship between gravitational pull and the mass below the object. The discussion emphasizes that Kepler's laws are not applicable to this problem, as they pertain to orbital mechanics rather than gravitational force calculations. Understanding these principles allows for the correct determination of the desired distance.
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Problem:
Calculate the distance from the center of the Earth to a point below the surface where the acceleration due to gravity is 0.50g, where g is the acceleration due to gravity at the Earth's surface.
I am really stuck on this. I tried using T^2 = 4pi^2 / GMe *r^3
but it didnt work it could be because M is supposed to be the mass of the sun but I decided it should be the mass of the earth! But it wasnt, it didnt work. I just can't seem to find a way to relate Keplers Laws to this problem. Are there other equations I could use?
Thanks in advance!
 
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Universal gravitational law :
\frac{Gm_{1}m_{2}}{r^2}=m_{2}g
m1 is the mass of the eart from its center up to the point. g is the gravitational acceleration at that point. m2 is the mass of an object you place at that point.
to find m1, you have to know the density of earth.
 
envscigrl said:
Problem:
Calculate the distance from the center of the Earth to a point below the surface where the acceleration due to gravity is 0.50g, where g is the acceleration due to gravity at the Earth's surface.
I am really stuck on this. I tried using T^2 = 4pi^2 / GMe *r^3
but it didnt work it could be because M is supposed to be the mass of the sun but I decided it should be the mass of the earth! But it wasnt, it didnt work. I just can't seem to find a way to relate Keplers Laws to this problem. Are there other equations I could use?
Thanks in advance!


You used kepler's law. It makes no mention of force. It would work for a body in orbit of the earth, T being the period of the orbit. But that is not the question, so that equation is completely irrelevant. use the equationg given by leong. consider:

<br /> g=G*\frac{M}{r^2}<br />

so

<br /> 0.5g = G*\frac{M}{r_{new}^2}<br />

and solve for r_{new}.

Note: M is the mass of the earth.
 
envscigrl said:
Problem:
Calculate the distance from the center of the Earth to a point below the surface where the acceleration due to gravity is 0.50g, where g is the acceleration due to gravity at the Earth's surface.
I am really stuck on this. I tried using T^2 = 4pi^2 / GMe *r^3
but it didnt work it could be because M is supposed to be the mass of the sun but I decided it should be the mass of the earth! But it wasnt, it didnt work. I just can't seem to find a way to relate Keplers Laws to this problem. Are there other equations I could use?
Thanks in advance!

I don't know why you would use that formula- that's for time and radius of an orbit!

In general, gravitational force is \frac{Gm_{e}m_{2}}{r^2} where me is the mass of the earth, m2 is the mass of the "test object". If r= R, the radius of the earth, then \frac{Gm_{2}m_{2}}{R^2}=m_2 g[/tex] so that \frac{Gm_e}{R^2}= g as Leong said. <br /> <br /> HOWEVER, only the mass BELOW the level of the object affects the gravitational pull. With m<sub>e</sub> as the total mass of the Earth and R the radius of the earth, and &amp;rho; the (average) density of the earth, m_e= \frac{4}{3}\piR^3 \rho so \rho= \frac{3m_e}{4\piR^3}. The mass of the Earth <b>below</b> radius r is \rho\frac{4}{3}\pi r^3= m_e\frac{r^3}{R^3}= m_e\(\frac{r}{R}\)^3.<br /> <br /> The gravitational pull on an object of mass m<sub>1</sub> at distance r from the center of the Earth is \frac{m_em_1\(\frac{r}{R}\)^3}{r^2}= \frac{m_em_1r}{R^3} and we want that equal to (1/2)gm.<br /> <br /> We must have \frac{m_er}{R^3}= \frac{g}{2}=/frac{m_e}{R^2} . Solve that for r (which is remarkably simple!).
 
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