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Barley

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First: A particle dropped into a hole drilled straight through the center of the earth. Neglecting rotational effects, show that the particles motion is simple harmonic if you assume Earth has uniform density. Show that the particle of oscillation is about 84 minutes.

Problem does not say if the hole is through the equator, or from pole to pole, does this matter. Now, I had the idea to show that the particle has the acceleration of a(t) = -omega^2x(t). Meaning that somehow I've got to show that the acceleration of the particle is proportional to the displacement of the particle but opposite in sign, and the quantities are related by the square of the angular frequency.

In the case described by the problem, is the acceleration through the center of the Earth the same as the accelration near the surface of the Earth ? What happens to g force in the middle--it must be zero right? And how do I figure the angular frequency the particle ?

2nd problem: The orbital revolution about the Earth is about 23.7 days and is in the same direction as the as the Earth's rotation every 24 hours. Use this information to show high tides occur everwhere on Earth every 12 h and 26 minutes.

Looked in an astronomy book and found that the tidal force has a 1/r^3 dependence. My text goes a little further and derives the Tidal force as a vector with Fx and Fy allowing you to determine tidal force at an point on the earth. But, I don't see how this information helps with the problem stated above. I'm given 2 periods of orbital revolution.

Clues, I need clues.

Thanks