How do we justify the generality of the wave equation?

Click For Summary
SUMMARY

The wave equation, expressed as ∂²y/∂x² = (1/v²) ⋅ ∂²y/∂t², is derived from Newton's second law (f=ma) applied to an oscillating string under the small angle approximation (sinα=α). This derivation assumes the string is nearly horizontal and applies primarily to waves of small amplitude relative to wavelength. Despite this limitation, the wave equation is considered a general result applicable to various wave phenomena, as it effectively models many physical situations, particularly in linear media. Understanding the constraints of linearity is crucial for determining the applicability of the wave equation across different media.

PREREQUISITES
  • Understanding of Newton's second law (f=ma)
  • Familiarity with wave mechanics and wave equations
  • Knowledge of linear approximations in physics
  • Basic concepts of tension and density in physical systems
NEXT STEPS
  • Study the derivation of the wave equation in more detail, focusing on the small angle approximation.
  • Explore the limitations of the wave equation in non-linear media.
  • Investigate the applications of the wave equation in electromagnetism (EM field).
  • Read P.G. Tait's proof regarding wave propagation on strings without calculus.
USEFUL FOR

Students and professionals in physics, particularly those studying wave mechanics, linear systems, and their applications in various physical phenomena.

Sturk200
Messages
168
Reaction score
17
We derived the wave equation by applying f=ma to an element of an oscillating string, yielding

2y/∂x2 = 1/v2 ⋅ ∂2y/∂t2.

In order to get this result it was necessary to assume that the string in question was nearly horizontal, so that the angle formed by the tension vector and the horizontal axis satisfied the small angle approximation sinα=α. It follows that the equation applies only to waves of very small amplitude relative to wavelength.

However, it is claimed, by my textbook for instance, that this equation is a general result that describes all wave phenomena. How can the derivation be generalized to waves with larger amplitudes if it requires the assumption that the string is nearly horizontal?
 
Physics news on Phys.org
At the end of the day, it just happen that the wave equation has solutions that model extremely well a host of physical phenomena (those phenomenon that we call "wave-like" :-) ) no matter how or what "inspired" us to find it (to find the wave equations).

Just like Poisson Equation is extremely useful to Gravitation and Electrostatics.

Sometimes we discover these equations by means of studying basic examples, sometimes deriving them from other assumptions,...

But at the end of the day, what is important is that they work, they are useful (they represent correctly certain features of certain physical phenomena).
 
The sinα=α approximation is essentially a linearity assumption. Which really means, the formula you arrive at will hold for all media that are linear. Which is a constraint that a lot of media fulfill (e.g. EM field). It's really just that physical strings stop being linear at some point. So, the wave equation is very general indeed, but you have to know at which point it is no longer applicable.
 
  • Like
Likes Sturk200

Similar threads

  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 7 ·
Replies
7
Views
3K
  • · Replies 0 ·
Replies
0
Views
5K
  • · Replies 1 ·
Replies
1
Views
2K
Replies
13
Views
2K
Replies
32
Views
5K
  • · Replies 2 ·
Replies
2
Views
3K
  • · Replies 0 ·
Replies
0
Views
1K
Replies
1
Views
2K