Period of a Simple Pendulum with Varying Masses and Gravitational Forces

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SUMMARY

The discussion focuses on deriving an alternative expression for the period T of a simple pendulum, considering varying inertial mass (m_{i}) and gravitational mass (m_{g}). The standard formula T=2π√(l/g) is modified by substituting g with the expression g = GM_{g}m_{g}/(R²m_{i}), where G represents the gravitational constant, R is the Earth's radius, and M_{g} is the Earth's mass. This approach effectively incorporates the effects of mass variations on the pendulum's period.

PREREQUISITES
  • Understanding of gravitational forces and Newton's law of universal gravitation
  • Familiarity with the concept of inertial mass versus gravitational mass
  • Basic knowledge of pendulum mechanics and oscillatory motion
  • Mathematical proficiency in manipulating algebraic expressions and square roots
NEXT STEPS
  • Explore the implications of varying mass on pendulum dynamics in "Advanced Mechanics" textbooks
  • Study the derivation of gravitational force equations, particularly in "Classical Mechanics" by David Morin
  • Investigate the effects of Earth's radius and mass on gravitational acceleration in "Astrophysics" resources
  • Learn about the applications of pendulum motion in real-world scenarios, such as timekeeping and seismology
USEFUL FOR

Students studying physics, particularly those focusing on mechanics, as well as educators looking for examples of gravitational effects on pendulum motion.

rbwang1225
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Homework Statement


The usual formula for the period T of a simple pendulum of length l is T=2[itex]\pi[/itex][itex]\sqrt{\frac{l}{g}}[/itex] where g is the acceleration due to gravity. Denoting rhe inertial mass of the pendulum bob by m[itex]_{i}[/itex] and its gravitational mass by m[itex]_{g}[/itex], derive an alternative expression for T in terms of these masses, the radius R of the Earth and its mass M[itex]_{g}[/itex].


Homework Equations





The Attempt at a Solution



I just replaced g as [itex]\frac{GM_{g} {m_{g}}}{R^{2}m_{i}}[/itex].
I don't know if this is what the author wants.
 
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That looks correct to me.
 

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