d’Alembert’s formula

E158707

d’Alembert’s formula is a classical solution method for the one-dimensional wave equation that expresses the displacement of a vibrating string in terms of its initial shape and velocity.

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Predicate Object
instanceOf analytical solution method
mathematical formula
partial differential equation solution
applicableWhen no boundary conditions or infinite domain
appliesTo one-dimensional wave equation
vibrating string
assumes constant wave speed
infinite string
linear wave equation
captures finite speed of disturbance propagation
characteristicMethod uses propagation along characteristics x±ct = const
contrastWith energy method for wave equations
numerical methods for the wave equation
domain real-valued functions of two variables
expresses displacement of a vibrating string
field applied mathematics
mathematical physics
partial differential equations
generalizes to piecewise smooth initial data
historicalPeriod 18th century
mathematicalType closed-form solution
namedAfter Jean d’Alembert
surface form: Jean le Rond d’Alembert
property preserves finite propagation speed
represents superposition of left- and right-traveling waves
relatedTo Fourier series methods for the wave equation
Green’s function for the one-dimensional wave equation
method of characteristics
relates solution to initial data
requires twice differentiable solution in x and t
solutionForm u(x,t) = F(x-ct) + G(x+ct)
u(x,t) = \tfrac12[f(x-ct)+f(x+ct)] + \tfrac1{2c} \int_{x-ct}^{x+ct} g(s)\,ds
solves u_{tt} = c^2 u_{xx}
usedFor Cauchy problem for the 1D wave equation
usedIn acoustics
theory of vibrating strings
wave propagation theory
uses initial displacement
initial velocity

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Jean d’Alembert knownFor d’Alembert’s formula