Transverse Displacement of Stretched String: Derivation of Poisson Eq.

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SUMMARY

The derivation of the Poisson Equation model for transverse displacement of a stretched string is established through the application of Newton's second law. The equation is represented as \(\nabla^{2}\psi(x) = \frac{F(x)}{T}\), where \(\psi(x)\) denotes the transverse displacement, \(F(x)\) is the externally applied transverse force, and \(T\) is the constant tension in the string. The derivation assumes small angles with the horizontal, allowing the approximation \(\sin(\theta) \approx \theta\). A visual representation of the forces acting on the string is essential for clarity in this derivation.

PREREQUISITES
  • Understanding of Newton's second law of motion
  • Familiarity with the concept of tension in strings
  • Basic knowledge of differential equations
  • Ability to visualize forces acting on a physical system
NEXT STEPS
  • Study the derivation of wave equations in stretched strings
  • Learn about boundary conditions in differential equations
  • Explore the application of the Laplace operator in physics
  • Investigate the effects of varying tension on string displacement
USEFUL FOR

Physicists, mechanical engineers, and students studying wave mechanics or string theory will benefit from this discussion, particularly those interested in the mathematical modeling of physical systems involving tension and displacement.

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Please how would one derive the Poisson Equation model,

\nabla^{2}\psi(x) = \frac{F(x)}{T},

for Transverse displacement \psi(x) of a stretched string under constant non-zero tension T and an externally applied transverse force F(x) . Assuming small angle with the horizontal (i.e sin(\theta)\approx\theta) ?

Thanks
 
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Start by by drawing a picture and labeling all the forces acting on the string. Then apply Newton's second law.
 

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