Moment of inertia and rotational kinetic energy

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SUMMARY

The discussion focuses on the concept of moment of inertia and its relationship to rotational kinetic energy. Moment of inertia (I) is defined as I = ∫ dm r², which relates torque (τ) to angular acceleration (α) through the equation τ = Iα, analogous to Newton's second law (F = ma). The kinetic energy associated with rotation is expressed as KE = 1/2 Iω², paralleling the linear kinetic energy formula. Understanding these relationships is crucial for analyzing rotational dynamics in physics.

PREREQUISITES
  • Understanding of basic physics concepts such as torque and angular acceleration.
  • Familiarity with Newton's laws of motion, particularly F = ma.
  • Knowledge of calculus, specifically integration for deriving moment of inertia.
  • Basic understanding of rotational motion and kinetic energy equations.
NEXT STEPS
  • Study the derivation of moment of inertia for various geometries and shapes.
  • Explore the application of rotational dynamics in real-world scenarios, such as in machinery.
  • Learn about the conservation of angular momentum and its implications in rotational systems.
  • Investigate advanced topics in rotational kinetic energy, including energy transfer in rotating systems.
USEFUL FOR

Students of physics, mechanical engineers, and anyone interested in understanding the principles of rotational motion and energy in physical systems.

CrazyNeutrino
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I can't seem to understand moment of inertia. What does it mean and how is it derived ?
How does it relate to rotational kinetic energy.
 
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Hi CrazyNeutrino! :smile:

From the PF Library on moment of inertia

Moment of Inertia … relates rotational force (torque) to rotational acceleration in the same way that mass relates ordinary (linear) force to ordinary acceleration.​

ie τ = Iα just like F = ma

(and KE = 1/2 Iω2 just like 1/2 mv2)

it is derived from I = ∫ dm r2
 
Why dm r^2?
 
CrazyNeutrino said:
Why dm r^2?

because for a point mass m at distance r from the axis, subjected to a force F,

the torque is τ = Fr, and the angular acceleration is α = a/r

τ = Iα means Fr = Ia/r

but F = ma (good ol' Newton's second law)

so mar = Ia/r

so I = mr2

(and moment of inertia of the whole = sum of moments of inertia of the parts, giving us ∫ dm r2)
 

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