Transverse Wave in a String Reflection and Transmission

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SUMMARY

The discussion focuses on the reflection and transmission of transverse waves in a string with a density/length of ρ and tension T, interacting with an elastic spring of stiffness k at x=0. The boundary conditions (BCs) established are y(0-,t) = y(0+,t) and the relationship between incident, reflected, and transmitted waves is given by fi(-ct) + gr(ct) = ft(-ct). The participant seeks clarification on the appropriate boundary condition at the spring, suggesting Ty' = ky at x = 0 as a potential option for further analysis.

PREREQUISITES
  • Understanding of wave mechanics, specifically transverse waves.
  • Familiarity with boundary conditions in wave equations.
  • Knowledge of elastic properties of materials, particularly spring constants.
  • Basic principles of tension and density in strings.
NEXT STEPS
  • Research the application of boundary conditions in wave mechanics.
  • Study the derivation of wave equations for strings with discontinuities.
  • Learn about the principles of reflection and transmission in elastic media.
  • Explore the mathematical modeling of spring-mass systems in wave propagation.
USEFUL FOR

Students and professionals in physics, particularly those specializing in wave mechanics, mechanical engineering, and materials science, will benefit from this discussion.

artongue
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A string with a density/length of rho and tension T has an elastic spring with stiffness k at x=0. There is a step pulse (fi = H(t)) incident on this discontinuity. Determine the reflected and transmitted waves.

Im not sure what boundary condition to use at the location of the spring. All I have now is:

BCs: (y(x,t) is deflection, fi(x-ct) is incident wave, gr(x+ct) is reflected, ft(x-ct) is transmitted)

y(0-,t) = y(0+,t) ----> fi(-ct) + gr(ct) = ft(-ct)

Not sure what other BC to use. Maybe Ty' = ky at x = 0? Where do I go from there?
 
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