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In the approximation that the Earth is a sphere of uniform density, it can be shown that the gravitational force it exerts on a mass m inside the Earth at a distance r from the center is mg(r/R), where R is the radius of the Earth. (Note that at the surface, the force is indeed mg, and at the center it is zero). Suppose that there were a hole drilled along a diameter straight through the Earth, and the air were pumped out of the hole. If an object is released from one end of the hole, how long will it take to reach the other side of the Earth? Include a numerical result.

Short Answer

Expert verified

The object travel from the center of the earth is weightless and expression is T=2Regand the numerical value is5068s.

Step by step solution

01

Identification of given data

Given data can be listed below,

  • Mass of Earth,Me

  • The radius of Earth, Re

  • Mass inside Earth, m

  • Distance from the earth,r

  • Acceleration due to the gravity,g

Period of oscillation, T

02

Expression of acceleration due to the gravity

Acceleration due to the gravity of the earth is given by

g=GMeRe2=9.8m/s2

When we go toward the center. The person experiences weightless at the center of the earth, then the effective gravity given by

geff=GMrr2

Where Mris mass varying with the radius of the earth.

ÒÏMr=Ï€R×43Re3

Where ÒÏis the density of the earth.

ÒÏ=Me43Ï€Re3

Now effective gravity is

geff=GMer3r2Re3=grRe

The gravity force of the spherical shell is given as

F=-mgrRe=-kr

This is the same as the hook’s law for a spring-mass system

03

The angular frequency and time period of the spring-mass system

Expression for angular frequency and time period of the spring-mass system is

Ó¬=kmT=2mk

The period of oscillation is

T=2mRemg=2Ï€Reg

The radius of the earth, Re=6.378×106mand g=9.8m/sput in the above equation

T=26.378×108m9.8m/s=5068s=84.5min

Hence, the object travels toward the center of the earth and is weightless, and passes through the center.

T=2Reg

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An object of mass m is attached by two stretched springs (stiffnessKs and relaxed lengthL0 ) to rigid walls, as shown in figure 4.60. The springs are initially stretched by an amount (L-L0). When the object is displaced to the right and released, it oscillates horizontally. Starting from the momentum principle, find a function of the displacement xof the object and the timet describes the oscillatory motion.

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