Why is the Harmonic Oscillator so common in physics?

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SUMMARY

The harmonic oscillator is prevalent in physics due to the quadratic approximation of potential energy around a minimum point, as derived from Taylor series expansion. When expanding a smooth function, the first derivative at a minimum is zero, leading to a quadratic function that describes simple harmonic motion (SHM). This principle was applied in a recent research problem where a resistive force was modeled as F=-kx, aligning perfectly with observed data. Understanding this relationship is crucial for analyzing systems exhibiting harmonic behavior.

PREREQUISITES
  • Understanding of Taylor series expansion in calculus
  • Knowledge of potential energy functions in physics
  • Familiarity with simple harmonic motion (SHM) concepts
  • Basic principles of optimization theory
NEXT STEPS
  • Study Taylor series and its applications in physics
  • Explore potential energy functions and their characteristics
  • Research simple harmonic motion (SHM) and its mathematical modeling
  • Investigate optimization theory in multi-variable calculus
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Physicists, researchers in mechanics, students studying calculus and physics, and anyone interested in the mathematical foundations of harmonic oscillators.

barnflakes
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I've heard before that it's because when you expand around a minimum point in the potential energy you get a quadratic function, but I can't recall where I read this. Can anyone point me in the right direction, or give their own explanation?

I only ask because I just solved a problem in my research by assuming that the resistive force to something is F=-kx which of course leads to harmonic oscillation - and this was completely unexpected - nobody knew that the resistive force should be, it just happens that it fits the data bang on.
 
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barnflakes said:
I've heard before that it's because when you expand around a minimum point in the potential energy you get a quadratic function, but I can't recall where I read this. Can anyone point me in the right direction, or give their own explanation?

When you expand any "smooth" function as a Taylor series about ##x = a## you have
##f(x) = f(a) + f'(a)(x-a) + f''(a)(x-a)^2/2## plus higher powers of ##(x-a)##

At a minimum (or maximum) the first derivative ##f'(a) = 0## so ##f(x)## is approximately a quadratic.

Any book on optimisation theory or multi-variable calculus should give the corresponding results for functions of more than one variable.
 
To expand a little on what AlephZero wrote...
If the potential approximates f(a) + f''(a)x2 then the restorative force, the derivative of the potential, is linear. At an energy minimum, the coefficient is negative, producing SHM.
 
That's really helpful guys, cheers.
 

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