Classical longitudinal wave on taut String

Click For Summary
SUMMARY

The discussion centers on solving Barton Zwiebach's question 4.2 from "Introduction to String Theory," which addresses the behavior of longitudinal waves on a taut string with uniform mass density (μ₀) and equilibrium tension (T₀). The user derived the tension as a function of length, T(L) = t₀ ln(L/a) + T₀, and attempted to apply Newton's second law to find the governing equation for small longitudinal oscillations. However, complications arose due to the variation of tension across the string, indicating a need for a more refined approach to analyze longitudinal wave propagation.

PREREQUISITES
  • Understanding of classical mechanics, specifically Newton's laws.
  • Familiarity with wave mechanics and the properties of longitudinal waves.
  • Knowledge of tension in strings and its dependence on length changes.
  • Basic grasp of calculus, particularly in relation to differential equations.
NEXT STEPS
  • Study the derivation of wave equations for longitudinal waves in strings.
  • Explore the concept of tension variation in elastic materials.
  • Learn about the application of Newton's second law in wave mechanics.
  • Investigate the mathematical treatment of oscillations in stretched strings.
USEFUL FOR

Students and professionals in physics, particularly those focusing on wave mechanics, string theory, and classical mechanics. This discussion is beneficial for anyone looking to deepen their understanding of longitudinal wave behavior in elastic media.

Gianni2k
Messages
17
Reaction score
0
Hi guys, this is Barton Zwiebach's Introduction to String theory question 4.2 on the longitudinal wave on a taut string. The problem is purely classical and I seem to obtain a solution which seems far too complicated for me. If anyone has the answers it would be great, if not just your help would be amazing. For people that don't have the book this is how the question goes.

"Consider a string with uniform mass density mu_0 stretched between x = 0 and x = a. Let the equilibrium tension be T_0. Longitudinal waves are possible if the string tension varies at it stretches or compresses. For a piece of this string with equilibrium length L, a small change in its length deltaL is accompaigned by a change in the tension deltaT where:

1/t_0 = (1/L)(deltaL/detaT)

where t_0 is a tension coefficient with units of tension. Find the equation governing small longitudinal oscillations of the string. Give the velocity of the waves."

many thanks.
 
Physics news on Phys.org
Just so you know what I did is calculate the general form of T(L):

T(L) = t_0 ln(L/a) + T_0

Then find the force on an infinitesimal stretch of the string then finally equate this to the acceleration via Newton's second law. The method is consistent for tangential waves but I have problems with longitudinal ones where the tension varies across the string.
 

Similar threads

  • · Replies 1 ·
Replies
1
Views
2K
Replies
13
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K
Replies
8
Views
2K
Replies
1
Views
2K
Replies
31
Views
4K
  • · Replies 6 ·
Replies
6
Views
2K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 6 ·
Replies
6
Views
2K
  • · Replies 26 ·
Replies
26
Views
8K