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Introduction to physics
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Lecture 21 Gyro and Statics
Motion of a gyro Statics Virtual work
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Moving a spinning wheel
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A top
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Gyroscopic precession
The precession of a gyroscope shows up in many βcommonβ situations.
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Actual motion of a Gyro, nutation
When we let go of a ryro, it first fall, and at the same time, process. It falls below the average procession line and then comes up again, and falls again in the vertical direction. The oscillation damps out eventually, one has in the end the pure procession.
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Static equilibrium of rigid body
Mechanism of Confinement Static equilibrium of rigid body Dynamical equations of rigid body Center of mass is at rest No rotation Mechanism of Confinement
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Lever πΉ π 1 πΉβ π 1 πβ π 2 π=0 π 1 π π 1 β π 2 π π 2 =0 π 2 π π 1 π
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View point of energy Energy conservation πΈ=π+π=ππππ π‘πππ‘
No kinetic energy π=0 When energy is πΈ 1 or πΈ 2 , the system is in the equilibrium state Condition of equilibrium is the potential energy is at local minimum (stable equilibrium) or maximum (unstable equilibrium)
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Stable equilibrium
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Unstable equilibrium
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Shape of hanging bridge
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Protein Structure Prediction
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Mechanism of Confinement
A elastic ring on a cone a h Mechanism of Confinement
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Mechanism of Confinement
Virtual displacement οΌθδ½η§»οΌ: displacement under constraint within the variation of time dt=0 Real displacement Virtual workοΌθεοΌ: Ideal constraintοΌηζ³ηΊ¦ζοΌ: Virtual displacement Mechanism of Confinement
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Constraint forces πΉ ππ and other forces πΉ π
Total virtual work πΏπ= Ξ£ π ( πΉ π + πΉ ππ ) βπΏ π π Ideal constraint Ξ£ π πΉ ππ βπΏ π π =0 Static equilibrium Ξ£ π πΉ π + πΉ ππ =0β Ξ£ π πΉ π βπΏ π π =0
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Mechanism of Confinement
l1 l2 q1 q2 m1g m2g Mechanism of Confinement
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