13 This process’s load deflection curve is sawtooth like in your video Mechanical properties related to a unique variation of Euler’s Contain Column studies. It shows how materials (representing fields) naturally respond to induced stresses in a “quantized“ manor. This process, unlike harmonic oscillators can lead to formation of stable structures. The quantized responses closely models the behaviors known as the Quantum Wave Function as described in modern physics. The effect has been used to make light weight structures and shock mitigating/recoiled reduction systems. The model shows the known requirement of exponential load increase and the here-to-for unknown collapse of resistance during transition, leading to the very fast jump to the next energy levels. This is shown by the saw-tooth graph’s bifurcation during the quantum jump. In materials the process continues till the load passes the ultimate tensile strength. Fields are not bounded by these conditions. th-cam.com/video/wrBsqiE0vG4/w-d-xo.htmlsi=waT8lY2iX-wJdjO3 0:08
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13
This process’s load deflection curve is sawtooth like in your video
Mechanical properties related to a unique variation of Euler’s Contain Column studies.
It shows how materials (representing fields) naturally respond to induced stresses in a “quantized“ manor.
This process, unlike harmonic oscillators can lead to formation of stable structures.
The quantized responses closely models the behaviors known as the Quantum Wave Function as described in modern physics.
The effect has been used to make light weight structures and shock mitigating/recoiled reduction systems.
The model shows the known requirement of exponential load increase and the here-to-for unknown collapse of resistance during transition, leading to the very fast jump to the next energy levels.
This is shown by the saw-tooth graph’s bifurcation during the quantum jump.
In materials the process continues till the load passes the ultimate tensile strength. Fields are not bounded by these conditions.
th-cam.com/video/wrBsqiE0vG4/w-d-xo.htmlsi=waT8lY2iX-wJdjO3
0:08
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