24.3 Exercises
Exercise 24.1 Through direct computation, verify the following calculations:
- When f(t)=1√4πDt, then f′(t)=−2πD(4πDt)−3/2
- When g(t)=−x24Dt, then g′(t)=x24Dt2
- Verify that (−12t+x24Dt2)=(x2−2Dt(2Dt)2)
Exercise 24.3 For this problem you will investigate p(x,t) (Equation @ref(eq:diffusion-equation}) with D=12.
- Evaluate ∫1−1p(x,10)dx. Write a one sentence description what this quantity represents.
- Using desmos or some other numerical integrator, complete the following table:
Equation | Result |
---|---|
∫1−1p(x,10)dx= | |
∫1−1p(x,5)dx= | |
∫1−1p(x,2.5)dx= | |
∫1−1p(x,1)dx= | |
∫1−1p(x,0.1)dx= | |
∫1−1p(x,0.01)dx= | |
∫1−1p(x,0.001)dx= |
- Based on the evidence from your table, what would you say is the value of lim?
- Now make graphs of p(x,t) at each of the values of t in your table. What would you say is occuring in the graph as \displaystyle \lim_{t \rightarrow 0^{+}} p(x,t)? Does anything surprise you? (The results you computed here lead to the foundation of what is called the Dirac delta function.)
Exercise 24.4 Consider the function \displaystyle p(x,t) = \frac{1}{\sqrt{4 \pi D t}} e^{-x^{2}/(4 D t)}. Let x=1.
- Explain in your own words what the graph p(1,t) represents as a function of t.
- Graph several profiles of p(1,t) when D = 1, 2, and 0.1. How does the value of D affect the profile?
Exercise 24.5 Consider the function \displaystyle p(x,t) = \frac{1}{\sqrt{\pi t}} e^{-x^{2}/t}:
- Using your differentiation skills compute the partial derivatives p_{t}, p_{x}, and p_{xx}.
- Verify p(x,t) is consistent with the diffusion equation \displaystyle p_{t}=\frac{1}{4} p_{xx}.
Exercise 24.6 For the one-dimensional random walk we discussed where there was an equal chance of moving to the left or the right. Here is a variation on this problem.
Let’s assume there is a chance v that it moves to the left (position x - \Delta x), and therefore a chance is 1-v that the particle remains at position x. The basic equation that describes the particle’s position at position x and time t + \Delta t is:
\begin{equation} p(x,t + \Delta t) = (1-v) \cdot p(x,t) + v \cdot p(x- \Delta x,t) \end{equation}
Apply the techniques of local linearization in x and t to show that this random walk to derive the following partial differential equation, called the advection equation:
\begin{equation} p_{t} = - \left( v \cdot \frac{ \Delta x}{\Delta t} \right) \cdot p_{x} \end{equation}
Note: you only need to expand this equation to first order