Higher-Dimension PDE
today: edges are kept at \( u = 0 \)
BCs:
- \( u(x, 0, t) = 0 \) (bottom)
- \( u(a, y, t) = 0 \) (right)
- \( u(x, b, t) = 0 \) (top)
- \( u(0, y, t) = 0 \) (left)
today: edges are kept at \( u = 0 \)
Same method: separation of variables
\( u(x, y, t) = X(x) Y(y) T(t) \)
rewrite heat eq: \( u_t = k (u_{xx} + u_{yy}) \)
\( X Y T' = k (X'' Y T + X Y'' T) \)
same separation constant
\( X'' + \lambda X = 0 \)
\( -\frac{Y''}{Y} + \frac{T'}{kT} = \text{constant} = -\lambda \)
\( \frac{Y''}{Y} = \frac{T'}{kT} + \lambda = \text{constant} = -\mu \)
(another constant)From that we get two more ODEs:
looks just like \( X \) equation
\( X'' + \lambda X = 0, \quad X(0) = X(a) = 0 \)
\( n = 1, 2, 3, \dots \)
\( Y'' + \mu Y = 0, \quad Y(0) = Y(b) = 0 \)
\( m = 1, 2, 3, \dots \)
for \( n = 1, 2, 3, \dots \)
\( m = 1, 2, 3, \dots \)
for each \( (m, n) \) pair, there is one solution
General solution: sum over \( n \) and \( m \)
IC:
\( u(x, y, 0) = f(x, y) \)
initial heat distribution
if \( x \) is fixed, it looks like
(\( x \) fixed)
The following visualization represents the temperature distribution \( u \) across a 2D domain at a specific time step \( t = 0.002 \). The vertical axis represents the temperature \( u \), while the horizontal axes represent spatial coordinates \( x \) and \( y \).
Note: The sharp drop-off at the edges indicates the boundary conditions where the temperature is held at zero.
This top-down heatmap view provides an alternative perspective of the temperature distribution \( u(x, y) \) at time \( t = 0.002 \). The color intensity corresponds to the temperature value.
Observation:
The heatmap confirms that the interior of the domain remains at the initial high temperature, while the thermal diffusion effect is concentrated near the boundaries at this very early time step.
The following visualization represents the spatial distribution of temperature \( u \) across a 2D domain at a specific time step \( t = 0.05 \).
Observation:
At \( t = 0.05 \), the temperature profile shows a clear diffusion pattern, with the highest values concentrated in the center of the domain and tapering off towards the boundaries.
This top-down heatmap view provides an alternative perspective of the temperature distribution \( u \) at \( t = 0.05 \), highlighting the symmetry of the diffusion process.
Key Details:
The visualization represents the temperature distribution \( u \) across a spatial domain defined by \( x \) and \( y \) coordinates at a specific time step \( t = 0.1 \).
This 2D heatmap provides a top-down view of the temperature field \( u(x, y) \) at \( t = 0.1 \).
The following visualization represents the temperature distribution \( u \) across a 2D domain defined by coordinates \( x \) and \( y \) at a specific time step \( t = 0.15 \).
This heatmap provides a top-down view of the temperature distribution \( u(x, y) \) at time \( t = 0.15 \), corresponding to the surface plot on the previous page.