SU-MATH53 MAR112024
Last edited: August 8, 2025heat equation on the entire line
\begin{equation} \pdv{u}{t} = \frac{1}{2} \pdv[2]{u}{x} \end{equation}
We can try to find a:
\begin{equation} U(0,x) = f(x) \end{equation}
if we write:
\begin{equation} \hat{U}(t,\lambda) = \int e^{-i x \lambda} U(t,x) \dd{x} \end{equation}
which means we can write, with initial condtions:
\begin{equation} \hat{U} (t, \lambda) = \hat{f}(\lambda) e^{- t \frac{\lambda^{2}}{2}} \end{equation}
We want to reach a close form:
\begin{equation} U (t, x) = \frac{1}{\sqrt{2\pi} t} \int_{-\infty}^{\infty} f(y) e^{-\frac{(x-y)^{2}}{2t}} \dd{y} \end{equation}
SU-MATH53 Midterm Sheet
Last edited: August 8, 2025This is the staging file for the midterm sheet, which I don’t usually publicise.
SU-MATH53 Practice 1 Problem 4
Last edited: August 8, 2025We have:
\begin{equation} \pdv[2]{u}{x} + \pdv[2]{u}{y} = 0 \end{equation}
Ignoring the boundary conditions when \(u(0,y)\), we know that we have Dirichlet boundaries in \(y\). This gives:
\begin{equation} u(x,0) = u(x,\pi) = 0 \end{equation}
Assuming our solution takes on the shape of \(u=X(x)Y(y)\), we obtain:
\begin{equation} X’’(x)Y(y) + Y’’(y)X(x) = 0 \end{equation}
by plugging in derivatives of that assumption; meaning:
\begin{equation} X’’(x)Y(y) = -Y’’(y)X(x) \end{equation}
This gives rise to:
\begin{align} \frac{X’’(x)}{X(x)} = -\frac{Y’’(y)}{Y(y)} = c \end{align}
SU-MATH53 Problem Session
Last edited: August 8, 2025L-Periodic Functions
So, we have:
\begin{equation} f(x+L) = f(x) \end{equation}
The integral is equivalent for any:
\begin{equation} \int_{a}^{a+L} f(x) \end{equation}
for any \(a\).
Heat Equation Recipe
- are we on a finite interval? then, decompose into product-type solution \(A(t)B(x)\) and solve.
- are we not? Fourier transform on the space variable and solve.
What if \(\lambda \in \mathbb{C} \backslash \mathbb{R}\)
Shush.
Why can we guess \(A(t)B(x)\)
Because we were able to find solutions. Believe that the solution set spans.
SU-PHIL2 APR032025
Last edited: August 8, 2025Recap: descritive morality, true morality
Principle of Beneficience
“you should help people when you are in need.”
=> evidence to show descritive morality
Moral Theory
Moral Theory is an implementation of modern morality.
- identify the “real” rules/principles
- explain why the rules are the rules
- “Why should you be moral?”
- How does it fit in with the “rest of the world”: metaphysics and epistemology
- metaphysical
- physical question
- where does the rules come front?
- what does it depended on?
- epistemological questions
- how do we know these rules are the rules?
- metaphysical
argument (philosophy)
Here are some properties of argument.
