00:01
We have to solve the initial boundary value problem and it is given as t of x, t is equal to alpha t double x of x, t where x is greater than 0 and t is greater than 0.
00:18
Then t of x, 0 it is equal to 0 whenever x is greater than 0.
00:24
Then minus k t of x, 0, t is equal to phi of 0 and limit extending to infinity, t of x, t is equal to 0 when t is greater than 0.
00:41
This was given to us and this can be written as this was t1.
00:47
So, here we can write it as del t by del x, this del t by del small t, this will be equal to alpha into del 2 of t by del x square where x is greater than 0 and t is greater than 0.
01:06
With the initial condition t of x, 0 it is equal to 0 where x is greater than 0 and these are the boundary conditions which we are provided here.
01:18
This is nothing but a partial differential equation.
01:21
This is a pde that is partial differential equation.
01:26
This is a heat equation with the source term given by alpha and the given boundaries and initial conditions.
01:34
Solving this kind of problem typically involves using the separation of variables.
01:39
Here we use the separation of variables and fourier series technique.
01:45
So, here step first is the separation of variables.
01:48
We will assume that t of x, t can be represented as a product of functions of x and t.
01:54
So, it is xx into t of t.
01:58
Substitute this into the partial differential equation.
02:02
So, x of x into t dash of t will be equal to alpha into x double dash of x and multiplied by t over t.
02:13
Then dividing both sides by this alpha and x of x and t of t, we get here t dash of t divided by alpha t of t is equal to x double dash of x divided by x of x.
02:33
This is equal to minus lambda where lambda is a separation constant.
02:38
Now, we will solve for the time part.
02:42
So, we will move into the step number 2 that is the time part.
02:47
The equation for t over t is a simple first order ordinary differential equation.
02:54
Therefore, t dash of t divided by alpha t of t, this is equal to minus lambda means this is equal to this term and integrating both sides with respect to t, we get over integration 1 by alpha log of that is natural log of t over t.
03:16
This is equal to minus lambda t plus c1 as a constant.
03:22
Now, we will solve for this t over t.
03:24
This t over t is equal to this alpha will multiply on that side that is alpha multiplied by minus lambda t, this minus lambda t plus c1...