In Problems 5 through 8, assume that the differential equation of a simple pendulum of length L is L0" + g0 = 0, where g = GM/R2 is the gravitational acceleration at the location of the pendulum (at distance R from the center of the earth; M denotes the mass of the earth). 5. Two pendulums are of lengths L1 and L2 and–when lo- cated at the respective distances R1 and R2 from the cen- ter of the earth-have periods p1 and p2. Show that P1 R1LI P2 R2/L2

Advanced Engineering Mathematics
10th Edition
ISBN:9780470458365
Author:Erwin Kreyszig
Publisher:Erwin Kreyszig
Chapter2: Second-order Linear Odes
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Differential Equations

In Problems 5 through 8, assume that the differential equation of a simple pendulum of length \( L \) is \( L\theta'' + g\theta = 0 \), where \( g = GM/R^2 \) is the gravitational acceleration at the location of the pendulum (at distance \( R \) from the center of the earth; \( M \) denotes the mass of the earth).

5. Two pendulums are of lengths \( L_1 \) and \( L_2 \) and—when located at the respective distances \( R_1 \) and \( R_2 \) from the center of the earth—have periods \( p_1 \) and \( p_2 \). Show that

\[
\frac{p_1}{p_2} = \frac{R_1 \sqrt{L_1}}{R_2 \sqrt{L_2}}.
\]
Transcribed Image Text:In Problems 5 through 8, assume that the differential equation of a simple pendulum of length \( L \) is \( L\theta'' + g\theta = 0 \), where \( g = GM/R^2 \) is the gravitational acceleration at the location of the pendulum (at distance \( R \) from the center of the earth; \( M \) denotes the mass of the earth). 5. Two pendulums are of lengths \( L_1 \) and \( L_2 \) and—when located at the respective distances \( R_1 \) and \( R_2 \) from the center of the earth—have periods \( p_1 \) and \( p_2 \). Show that \[ \frac{p_1}{p_2} = \frac{R_1 \sqrt{L_1}}{R_2 \sqrt{L_2}}. \]
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