Why no higher derivative in physics?

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SUMMARY

The discussion centers on the rarity of higher derivatives beyond the second order in physics equations, particularly in the context of differential equations like wave equations and the Riemann curvature tensor in General Relativity. While terms such as jerk, jounce, crackle, and pop exist, they are seldom utilized in practical physics applications. The consensus indicates that most physical phenomena can be effectively described using second derivatives, with higher derivatives being less common due to their complexity and the principle of locality, which emphasizes local interactions over distant ones.

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  • Understanding of differential equations, particularly second-order partial differential equations (PDEs).
  • Familiarity with concepts of derivatives in physics, including jerk and acceleration.
  • Knowledge of General Relativity and the role of the Riemann curvature tensor.
  • Basic grasp of Taylor series and their application in approximating functions.
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  • #31
Ksitov said:
Dear all,

I'm asking why there is no higher derivative than two in physics ? I never encountered a third (time or space) derivative in physics.

Have you some litterature about this?

Thank you.

Regards.

I would say the short answer is that the all phenomena can be represented as a perturbation upon a differential equation having constant coefficients. The solutions of such a differential equation map out to functions that are the exponential functions (i.e., of the natural logarithm base, e) of the input variable scaled by the values that are the root of the polynomial equation that corresponds to the original differential equation such that the order of the differential is the power of the polynomial term (this is standard material covered by a course in differential equations). Now, for a polynomial with real coefficients, the roots must either be real values or pairs of complex conjugate values, and those pairs when multiplied together yield a quadratic factor; hence whatever is modeled mathematically can be resolved down to a function in which is no more than quadratic in nature, and hence, all that is needed to describe it is the use of at most the 2nd differential.
 
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  • #32
The Blasius equation relates to boundary layer flow on along a semi-infinite plate

2f''' + f''f = 0
 

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