PM [08] Phonon Processes in Circular Motion

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PHONON IN CIRCULAR MOTION


Phonons in Circular Motion

According to the Eskade theory, all motions of material particles are caused by phonons.

Circular motions are of no exception although their processes are more complicated than those of linear motions.

So let us examine in detail to see what kind of role the phonons play in circular motion.

The staging of the analysis is in step with the previous discussion in which we talked about the cyclical nature of the centripetal and centrifugal forces.


𝑣

1. A free particle

The phonons are carrying the particle towards the top of the paper at a constant speed 𝑣 in a vacuum.

P


𝑣

2. Caught by a string

The particle is suddenly being caught by a string fixed at A.

A

P

No tension

Fixed Contact established at this point


𝑣

3. The formation of the centrifugal force

This effort trying to make the string longer constitutes a new force – this is the origin of the centrifugal force 𝐹⊤.

𝐹⊤

A P

Part of the phonons turns around and sets up a centrifugal force

𝐹⊤


𝑣

4. Tension formed in string

The string now is under tension and the stress is transmitted to the point at A. Because the anchor point is fixed, it absorbed the incoming force 𝐹⊤.

A

𝐹⊤

𝐹⊤ being transmitted to A

Tension

𝐹⊤


5 Production of centripetal force 𝐹⊥

In turn point A produces a reaction to counteract the incoming force 𝐹⊤. This produces a centripetal force 𝐹⊥ equal in magnitude to 𝐹⊤.

𝑣

A

𝐹⊤


Tension

𝐹⊥A

𝐹⊥


6 𝐹⊥ moves to P

𝐹⊥ travels to the particle at P.

𝑣

A

𝐹⊤ being transmitted to P

𝐹⊥

Centripetal phonon enters particle at A

𝐹⊥


𝑣

7. Action by centripetal force

The centripetal force 𝐹⊥ causes particle P to turn.

A

𝐹⊥

Centripetal phonon causes particle to turn


8 Dynamic equilibrium

The process then starts all over again and the entire series of repetitions ends up in a circle.

𝑣

A


𝐹⊥𝐹⊤ 𝐹⊤𝐹⊥


ENERGY OF CIRCULAR MOTION

To be carried on in:

Science

PM [08] Phonon Processes in Circular Motion