Relationship between potential energy and force

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SUMMARY

The relationship between potential energy and force is defined by the equation F = -dU/dx, indicating that force is the negative gradient of potential energy. In scenarios where potential energy U(x) is explicitly dependent on position x, the force F will also vary with x. The discussion highlights that the expression dW = -dU is only valid under specific conditions, such as when the second derivative of potential energy with respect to position is zero. For example, in a harmonic oscillator, the potential energy is given by U(x) = (1/2)kx², leading to a specific force calculation.

PREREQUISITES
  • Understanding of potential energy and force concepts
  • Familiarity with calculus, specifically differentiation
  • Knowledge of harmonic oscillators and their equations
  • Ability to interpret differential equations
NEXT STEPS
  • Study the derivation of force from potential energy in various systems
  • Learn about the implications of the second derivative of potential energy
  • Explore the dynamics of harmonic oscillators in detail
  • Investigate the applications of potential energy in real-world physics problems
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Students of physics, particularly those studying mechanics, engineers working with dynamic systems, and anyone interested in the mathematical relationships between force and potential energy.

Aaron Wong
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Hi,
I wonder which steps of my following deduce are wrong
dU=-dW
dU=mg dh
dW=Fdx
thus, mgdh=-Fdx (dx=dh)
then, F=-mg which is a constant in most of situation
However, F does change in some situation.

I am confused about this.
 
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Sticking to 1D, if you have potential energy distribution U(x) so U is explicitly dependent of the position x ... then:
F = -dU/dx ... so you see F will depend on x if dU/dx depends on x.

Constraining motion to the x axis, the work done by force F is given by:
W = Fx so dW/dx = x.dF/dx + F (by the product rule) so dW = x.dF + F.dx and substituting above gives:
dW = x.dF - dU which gives a 2nd order DE in U.
Thus dW = -dU everywhere only in the situation where d2U/dx2 = 0 ...
ie. The expression you started with is a 1st order approximation only (expand U(x) as a power series and see.)

Notice that F=mg means that dU/dx = -mg and d2U/dx2 = 0 so the relation is exact, and you will see that dU/dx does not depend on x (see first sentence above).

Try for a harmonic oscillator ... ##U(x)=\frac{1}{2}kx^2 \implies F=?## ... here I have chosen U(x):U(0)=0 for you.
 
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