Solving a Second-Order Wave Equation

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Discussion Overview

The discussion revolves around the nature of the second-order wave equation, specifically its form and the reasons for its second-order partial differential equation (PDE) status. Participants explore both mathematical and physical justifications for this characteristic, including the implications of initial conditions and the relationship between acceleration and force in wave propagation.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant notes that the wave equation is a second-order PDE because it requires knowledge of both initial position and initial speed to determine the system's time evolution.
  • Another participant questions whether time reversibility plays a role in the necessity of a second-order PDE.
  • One participant provides a mathematical perspective, explaining that second-order differential equations allow for complex roots and sinusoidal solutions, which cannot arise from first-order equations.
  • Another participant emphasizes that various waveforms can satisfy the wave equation, but their representation involves Fourier analysis, linking back to trigonometric functions.
  • A participant asserts that the second-order nature of the wave equation is due to its relation to acceleration and net tension forces, rather than time reversibility.
  • One participant describes a derivation of the wave equation from a system of coupled oscillators, suggesting that the second derivative nature arises from the movement equations of these oscillators.

Areas of Agreement / Disagreement

Participants express a range of views regarding the reasons for the wave equation's second-order status, with some agreeing on mathematical justifications while others explore physical interpretations. No consensus is reached on the role of time reversibility or the necessity of the second-order form in physical systems.

Contextual Notes

Some participants highlight that while the wave equation is second-order, there are first-order PDEs that describe other physical systems, indicating that the choice of order may depend on the specific characteristics of the system being modeled.

KFC
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Hi there,
I am solving a second-order wave equation of the following form:

##v^2\dfrac{\partial^2 y}{\partial x^2} = \dfrac{\partial^2y}{\partial t^2}##

where ##t## is time; ##y## is the wave function. I learn the wave function by assuming the system is linear and has a linear solution. The book tells to try a solution of sinusoidal wave so I get the following solution

##
y = A\sin(kx - \omega t)
##

M question is why the wave equation has to be a second-order PDE but not a first-order PDE. I saw some explanation online, it is stated that for a physical system, we need to know both initial position and initial speed so to learn the time evolution of the system. This makes sense to me. However, besides this points, is it anything to do with the time reversibility to explain why we need a second-order PDE instead?
 
Last edited:
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KFC said:
##v^2\dfrac{\partial^2 y}{\partial t^2} = \dfrac{\partial^2y}{\partial t^2}##

##
y = A\sin(kx - \omega t)
##
Would like to point out that as is, the equation can only makes sense if v= +/-1, and the solution wouldn't work. It should be:
##v^2\dfrac{\partial^2 y}{\partial x^2} = \dfrac{\partial^2y}{\partial t^2}##
 
DarkBabylon said:
Would like to point out that as is, the equation can only makes sense if v= +/-1, and the solution wouldn't work. It should be:
##v^2\dfrac{\partial^2 y}{\partial x^2} = \dfrac{\partial^2y}{\partial t^2}##

Yes, it is a typo there. I just get it fixed. Thanks for that.
 
As for why it HAS to be a second order PDE:
In ordinary differential equations you have first order and second order. It is safe to assume that the solution would always be in the form of:
y(x)=A*exp(α*x)
The first order would return that α is what multiplies the derivative.
The second order however becomes something that I personally find comfort with as it is a middle school level maths from here until further notice:
2+bα+c=0
For the homogeneous solution, where {a,b,c} are parameters. That is a quadratic equation so we can solve it using this following formula:
α1,2=[-b±sqrt(b2-4ac)]/(2a)
Notice we have a square root. This would return us several kinds of roots:
One repeated root where the solution is:
y(x)=A*exp(αx)+Bx*exp(αx)
Two different real roots where the solution is:
y(x)=A*exp(α1*x)+B*exp(α2*x)
Or two complimentary complex roots where the solution is:
y(x)=A*exp((λ+μi)x)+B*exp((λ-μi)x)
where λ is the solution for -b/(2a) and μ is the solution for sqrt(b2-4ac)/(2a).
However these are complex numbers. Through some formulation and Euler's formula you can then end up with this:
y(x)=A*exp(λx)*cos(μx)+B*exp(λx)*sin(μx)
or if you don't like two trigonometric functions for whatever reason:
y(x)=C*exp(λx)*cos(μx+φ)
where φ is the phase, C is the amplitude, A is a parameter and B is also a parameter, all dependent on the initial conditions. i is the imaginary unit.
The sinusoidal solution can't appear for first order differential because α is a real number, if and only if the multiplier of the derivative is a real number. If the multiplier of the derivative is a complex number then α must also be complex however the solution will return a function that belongs to the complex plane.
As for why in this particular equation it must be sinusoidal I trust you can, with this information, arrive at the answer yourself.

I would like to also point out it is not just a sinusoidal function solution solves this. Any wave form can solve this equation, be it square, triangle, saw-tooth etc. but you must use their Fourier representation to do that, which incidentally involves the trigonometric functions sine and cosine and if you work with complex numbers, exponent (must have an imaginary unit in the exponent) as well.
 
Last edited:
Can't edit on the phone.
Where I said:
is the solution for sqrt(b2-4ac)/(2a)."
It should be μi, excuse me for the inaccuracy.
 
DarkBabylon said:
Can't edit on the phone.
Where I said:
is the solution for sqrt(b2-4ac)/(2a)."
It should be μi, excuse me for the inaccuracy.
Thanks a lot for your explanation. I agree the reason to have a second order PDE for the wave equation in terms of mathematics. But what I want to know more is why physically it should be 2nd order and if it is any thing to do with the time reversibility. In physical system, there is 1st order PDE to describe some system as well. I just don't understand why wave equation is not 1st order or 3rd order or even 4rd order but just 2nd order in terms of physics.
 
The order has nothing to do with time reversibility. (The heat equation is also 2nd order.)

The 2nd order comes about because the wave equation is relating the acceleration (2nd derivative of position with respect to time) of a piece of string to the net tension force exerted on it (essentially the 2nd derivative of position with respect to space).
 
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You should look up a derivation of the wave equation then it would make more sense, essentially what they do is they take a system of N coupled oscillators where they connect all oscillators in a line such that they are all evenly spaced (assume that the line's length is L, then the distance between each couple is L/N), they write the movement equations for the system and then take the limit of N going to infinity, the result of that limit is the wave equation, so basically the second derivative nature of the wave equation is a result of the movement equations for the coupled oscillators.
 
Thanks all above. Yes, by looking at the force, it makes sense to have 2nd order PDE.
 

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