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Duhamel's Principle


Duhamel's principle states that the solution of an inhomogeneous linear evolution equation is a superposition of solutions of the corresponding homogeneous equation. If S(t) is the solution operator for u_t=Lu and u(0)=u_0, then the solution of u_t=Lu+f(t) is formally

 u(t)=S(t)u_0+int_0^tS(t-s)f(s)ds.

The integrand propagates the forcing introduced at time s through the remaining time t-s.

For an ordinary differential equation or a linear time-invariant system, this representation becomes the Duhamel integral. For the inhomogeneous wave equation, it expresses the solution as an integral of solutions generated by instantaneous source data.


See also

Duhamel Integral, Fundamental Solution, Variation of Parameters, Wave Equation

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References

Evans, L. C. Partial Differential Equations, 2nd ed. Providence, RI: American Mathematical Society, 2010.

Cite this as:

Weisstein, Eric W. "Duhamel's Principle." From MathWorld--A Wolfram Resource. https://mathworld.wolfram.com/DuhamelsPrinciple.html

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