Potential energy equilibrium positions

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SUMMARY

The discussion focuses on finding equilibrium positions for a particle with potential energy defined by the equation U(x) = x + sin((2 rad/m) x) within the range of 0 to π meters. The first derivative of U(x) was calculated as 1 + 2 cos(2x), which was set to zero to find equilibrium points. The solutions include x = π/3 rad and x = 2π/3 rad, with the latter being identified as another valid solution due to the periodic nature of the cosine function. Stability analysis using the second derivative, -4 sin(2x), indicates that x = π/3 rad corresponds to an unstable equilibrium, as the second derivative is negative.

PREREQUISITES
  • Understanding of calculus, specifically derivatives and their applications in physics.
  • Familiarity with potential energy concepts in classical mechanics.
  • Knowledge of trigonometric functions and their properties, particularly cosine.
  • Ability to solve equations involving trigonometric identities.
NEXT STEPS
  • Study the periodic properties of trigonometric functions, focusing on cosine and its inverse.
  • Learn about stability analysis in potential energy systems using second derivatives.
  • Explore the concept of equilibrium in classical mechanics, including stable and unstable types.
  • Practice solving similar problems involving potential energy functions and their derivatives.
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Students studying physics, particularly those focusing on mechanics and potential energy, as well as educators looking for examples of equilibrium analysis in particle systems.

frostking
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Homework Statement


A particle has potential energy

U(x) = x + sin ((2 rad/m) x)

over the range of x greater or equal to 0 meters and less than or equal to pi meters
Where are the equilibrium positions in this range and for each is it a point of stable or unstable equilibrium?

Homework Equations


derv of u(x) set = to 0 and then the second derv of u(x)


The Attempt at a Solution




I solved derv of u(x) = 1 + 2 cos(2x) then set = to 0

so 2 cos(2x) = -1 divide by 2 and cos(2x) = -1/2
2x = arch cos of (-1/2) = 2pi/3 rad

x = 1 pi/3 rad

I get this part but the answer says that x can = 2pi/3 rad as well and I do not understand why.

To determine if equilibrium is unstable or stable I took the second derv and at x = pi/3 and second derv of - 4 sin(2x) I got less than 0 so a maximum and therefore unstable equilibrium

Can someone please help me understand why I should have known to consider 2pi /3? Thanks for your efforts, Frostking
 
Physics news on Phys.org
There are an infinite number of solutions to \cos(2x) = -1/2. You just found one - there's another solution which will give you 2\pi/3 as the final answer.
 
Thanks, yes I should have realized I needed to check for other values less than or equal to pi!
 

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