K.J.Healey
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The non generated one is just for :
G = 6.667428*10^-11 _m^3 _kg^-1 _s^-2
G = 6.667428*10^-11 _m^3 _kg^-1 _s^-2
The discussion revolves around a hypothetical scenario where a ball is dropped into a tunnel that goes through the center of the Earth. Participants explore the dynamics of the ball's motion, including its oscillation, travel time, and the effects of gravity as it moves through the tunnel.
Participants express differing views on the travel time of the ball and the applicability of various physical analogies. There is no clear consensus on the exact dynamics of the ball's motion or the implications of gravity's variation within the Earth.
Some calculations depend on assumptions about uniform density and neglecting air resistance. The discussion includes various mathematical approaches and analogies that may not fully account for the complexities of the scenario.
Since I don't use Mathematica I can't comment on your use of it, but your potential energy term is incorrect.K.J.Healey said:Heres how i did it in mathematica:
<br /> F= -G m M /r[t]{}^{\wedge}2<br />
<br /> -\frac{G m M}{r(t)^2}<br />
<br /> U=\text{Integrate}[F,r[t]]<br />
<br /> \frac{G m M}{r(t)}<br />
<br /> \rho = \text{ME}/((4/3)*\text{Pi}*\text{RE}{}^{\wedge}3)<br />
<br /> \frac{3 \text{ME}}{4 \pi \text{RE}^3}<br />
M=\rho *(4/3)*\text{Pi}*r[t]{}^{\wedge}3<br />
<br /> \frac{\text{ME} r(t)^3}{\text{RE}^3}<br />
T=(1/2)m (r'[t]){}^{\wedge}2<br />
<br /> \frac{1}{2} m r'(t)^2<br />
<br /> L=T-U<br />
<br /> \frac{1}{2} m r'(t)^2-\frac{G m \text{ME} r(t)^2}{\text{RE}^3}<br />