A giant snowboard, represented by a rigid and slender rod with mass m and length L, slides on the undersized cylindrical half-pipe of radius r without friction at its ends A and B. The motion of the snowboard within the half-pipe occurs only within the vertical plane shown. Using the generalized coordinate 0, derive the equations of motion for this system using Lagrange's Equations. Note: The moment of inertia of a slender rod about its center of mass I=1/12*m*L2

Elements Of Electromagnetics
7th Edition
ISBN:9780190698614
Author:Sadiku, Matthew N. O.
Publisher:Sadiku, Matthew N. O.
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A giant snowboard, represented by a rigid and slender rod with mass m
and length L, slides on the undersized cylindrical half-pipe of radius r
without friction at its ends A and B. The motion of the snowboard within the
half-pipe occurs only within the vertical plane shown. Using the generalized
coordinate 0, derive the equations of motion for this system using
Lagrange's Equations.
Note: The moment of inertia of a slender rod about its center of mass
IG=1/12*m*L2
A
C
Transcribed Image Text:A giant snowboard, represented by a rigid and slender rod with mass m and length L, slides on the undersized cylindrical half-pipe of radius r without friction at its ends A and B. The motion of the snowboard within the half-pipe occurs only within the vertical plane shown. Using the generalized coordinate 0, derive the equations of motion for this system using Lagrange's Equations. Note: The moment of inertia of a slender rod about its center of mass IG=1/12*m*L2 A C
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