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Introduction to physics

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Presentation on theme: "Introduction to physics"β€” Presentation transcript:

1 Introduction to physics

2 Lecture 21 Gyro and Statics
Motion of a gyro Statics Virtual work

3 Moving a spinning wheel

4 A top

5 Gyroscopic precession
The precession of a gyroscope shows up in many β€œcommon” situations.

6 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.

7 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

8 Lever 𝐹 𝑙 1 πΉβˆ’ π‘š 1 π‘”βˆ’ π‘š 2 𝑔=0 π‘š 1 𝑔 𝑙 1 βˆ’ π‘š 2 𝑔 𝑙 2 =0 π‘š 2 𝑔 π‘š 1 𝑔

9

10 View point of energy Energy conservation 𝐸=𝑇+𝑉=π‘π‘œπ‘›π‘ π‘‘π‘Žπ‘›π‘‘
No kinetic energy 𝑇=0 When energy is 𝐸 1 or 𝐸 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)

11 Stable equilibrium

12 Unstable equilibrium

13 Shape of hanging bridge

14 Protein Structure Prediction

15

16 Mechanism of Confinement
A elastic ring on a cone a h Mechanism of Confinement

17 Mechanism of Confinement
Virtual displacement οΌˆθ™šδ½η§»οΌ‰: displacement under constraint within the variation of time dt=0 Real displacement Virtual workοΌˆθ™šεŠŸοΌ‰: Ideal constraintοΌˆη†ζƒ³ηΊ¦ζŸοΌ‰: Virtual displacement Mechanism of Confinement

18 Constraint forces 𝐹 𝑐𝑖 and other forces 𝐹 𝑖
Total virtual work π›Ώπ‘Š= Ξ£ 𝑖 ( 𝐹 𝑖 + 𝐹 𝑐𝑖 ) βˆ™π›Ώ π‘Ÿ 𝑖 Ideal constraint Ξ£ 𝑖 𝐹 𝑐𝑖 βˆ™π›Ώ π‘Ÿ 𝑖 =0 Static equilibrium Ξ£ 𝑖 𝐹 𝑖 + 𝐹 𝑐𝑖 =0β†’ Ξ£ 𝑖 𝐹 𝑖 βˆ™π›Ώ π‘Ÿ 𝑖 =0

19 Mechanism of Confinement
l1 l2 q1 q2 m1g m2g Mechanism of Confinement


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