Let me be very clear: math is all about practice, and there are no shortcuts. So, please refer to B. S. Grewal's book for theory and practice questions. Here, I can only provide video links to help you understand the topic.🙂

Method of Separation of Variables

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SEPERATION OF VARIABLES

Let second order PDE is given.

And uu be a function of two independent variables xx & tt.

We assume that all required solution is separable and of form

u(x,t)=X(x)T(t)..... (1)u(x, t) = X(x) \cdot T(t) \quad \text{..... (1)}

Using this equation (1) we reduce the PDE in form of

f(X,X,X,.....)=g(T,T,T,.....)..... (2)f(X, X', X'', ..... ) = g(T, T', T'', .....) \quad \text{..... (2)}

Which is separable in XX & TT.

From equation (2)

f(X,X,.....)=k..... (3)f(X, X', .....) = k \quad \text{..... (3)}

g(T,T,.....)=k..... (4)g(T, T', .....) = k \quad \text{..... (4)}

Equation (3) & (4) are ODE and can be solved by known methods.

Solution of One-Dimensional Wave and Heat Equation

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One-Dimensional Wave Equation

Equation: 2ut2=C22ux2\frac{\partial^2 u}{\partial t^2} = C^2 \frac{\partial^2 u}{\partial x^2}

  • CC Wave speed, a constant that represents how fast the wave propagates through the medium.
  • xx Spatial coordinate, representing the position along the one-dimensional medium.
  • tt Time variable.

Boundary Conditions:

  1. u(0,t)=0u(0, t) = 0 (Dirichlet boundary condition)
  2. u(L,t)=0u(L, t) = 0 (Dirichlet boundary condition)

Initial Conditions:

  1. u(x,0)=f(x)u(x, 0) = f(x) (initial displacement)
  2. ut(x,0)=g(x)\frac{\partial u}{\partial t}(x, 0) = g(x) (initial velocity)

One-Dimensional Heat Equation

Equation: ut=C22ux2\frac{\partial u}{\partial t} = C^2 \frac{\partial^2 u}{\partial x^2}

  • CC Thermal diffusivity, a constant that indicates how quickly heat diffuses through the medium.
  • xx Spatial coordinate, representing the position along the one-dimensional medium.
  • tt Time variable.

Boundary Conditions:

  1. u(0,t)=0u(0, t) = 0 (Dirichlet boundary condition)
  2. u(L,t)=0u(L, t) = 0 (Dirichlet boundary condition)

Initial Condition:

  1. u(x,0)=f(x)u(x, 0) = f(x) (initial temperature distribution)

These conditions define the behavior of the solutions in a specified domain over time.

Boundary and Initial Conditions

  • LL: Length of the domain for both equations.
  • f(x)f(x): Initial displacement (for the wave equation) or initial temperature distribution (for the heat equation) as a function of position xx.
  • g(x)g(x): Initial velocity as a function of position xx (only relevant for the wave equation).

Two-Dimensional Laplace's Equation

The two-dimensional Laplace's equation is given by:

2ux2+2uy2=0\frac{\partial^2 u}{\partial x^2} + \frac{\partial^2 u}{\partial y^2} = 0

  • u(x,y)u(x, y): A scalar potential function, which can represent various physical quantities such as electric potential, fluid velocity potential, or temperature.
  • xx: The spatial coordinate in one direction (e.g., horizontal).
  • yy: The spatial coordinate in the perpendicular direction (e.g., vertical).
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