Change of Variables and Chain Rule

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SUMMARY

The discussion centers on solving the transport partial differential equation (PDE) given by \(\frac{\partial u}{\partial t}+c\frac{\partial u}{\partial x} = 0\) using a change of variables and the chain rule. The change of variables is defined as \(\xi = x - ct\), leading to the relationship \(u(t,x) = v(t, \xi)\). The user successfully applies the chain rule to derive \(\frac{\partial u}{\partial t} = \frac{\partial v}{\partial t} - c\frac{\partial u}{\partial x}\) and seeks to prove that \(\frac{\partial u}{\partial x} = \frac{\partial v}{\partial \xi}\). The conclusion indicates that the solution simplifies to \(u(x,t) = f(x-ct)\), where \(f\) is an arbitrary function of \(\xi\).

PREREQUISITES
  • Understanding of partial differential equations (PDEs)
  • Familiarity with the chain rule in calculus
  • Knowledge of change of variables in mathematical analysis
  • Basic concepts of function derivatives
NEXT STEPS
  • Study the method of characteristics for solving PDEs
  • Learn about the implications of the anti-partial derivative in PDEs
  • Explore the concept of arbitrary functions in solutions of differential equations
  • Investigate the applications of transport equations in physics and engineering
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Students and professionals in mathematics, physics, and engineering who are working with partial differential equations, particularly those interested in transport phenomena and variable transformations.

Stalker_VT
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Homework Statement


I am trying to solve the transport PDE using a change of variables and the chain rule, and my problem seems to be with the chain rule. The PDE is:

\frac{\partial u}{\partial t}+c\frac{\partial u}{\partial x} = 0 ......(1)

The change of variables (change of reference frame) is:

\xi = x - ct......(2)

From this we know that

u(t,x) = v(t, x - ct) = v(t, \xi)......(3)

The Attempt at a Solution



Taking the total derivative of both sides of (3)

\frac{d}{dt} [u(t,x) = v(t,\xi)]

using chain rule yields

\frac{\partial u}{\partial t} = \frac{\partial v}{\partial t} - c\frac{\partial u}{\partial x}......(4)

I think the next step is to PROVE that

\frac{\partial u}{\partial x} = \frac{\partial v}{\partial \xi}.....(5)

and then substitute (4) into (5) to get

\frac{\partial v}{\partial t} = 0

but i am not sure how to do this...Any help Greatly Appreciated

Thanks!
 
Last edited:
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Stalker_VT said:
and then substitute (4) into (5) to get

\frac{\partial v}{\partial t} = 0

but i am not sure how to do this...Any help Greatly Appreciated

Thanks!

If I understand correctly, I think you are basically done. You have $$
\frac{\partial v(t,\xi)}{\partial t}=0$$Take the anti-partial derivative of this with respect to t. Here your constant of integration is an arbitrary function of the other variable:$$
v(t,\xi) = f(\xi) = f(x-ct)$$so you have$$
u(x,t)=v(t,\xi)=f(\xi)=f(x-ct)$$Unless, of course, you already understood that and I misunderstand what your question is.
 

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