DashCampbell
/
MATH201
forked from Sasserisop/MATH201
1
0
Fork 0
Code Pull Requests Activity

added lec 35 and fixed some audio stuff

This commit is contained in:
Sasserisop 2023-12-06 23:40:58 -07:00
parent c3d7ab95f6
commit 541827e168
6 changed files with 1313 additions and 4 deletions
Show Stats Download Patch File Download Diff File Expand all files Collapse all files

2
content/Fourier Series (lec 28-29).md
View File

@ -174,7 +174,7 @@ then:
$$\bar{f}(x)=\frac{2}{\pi}+\frac{2}{\pi}\sum_{k=1}^\infty\left( \frac{1}{2k+1}-\frac{1}{2k-1} \right)\cos(2k\pi x)$$ $$\bar{f}(x)=\frac{2}{\pi}+\frac{2}{\pi}\sum_{k=1}^\infty\left( \frac{1}{2k+1}-\frac{1}{2k-1} \right)\cos(2k\pi x)$$
Even with 10 terms, we get a pretty good approximation: Even with 10 terms, we get a pretty good approximation:
![fouriercosineofsin.png](drawings/fouriercosineofsin.png) ![fouriercosineofsin.png](drawings/fouriercosineofsin.png)
Here's a little script I wrote to generate an audible waveform of this Fourier series! Here's a little script that generates an audible waveform of this Fourier series!
<html> <html>
<head> <head>

49
content/Wave equations (lec 35).md Normal file
View File

@ -0,0 +1,49 @@
#start of lec 35
last problem of the course which we will finish today.
$\frac{ \partial^2 u }{ \partial t^2 }=\frac{ \partial^2 u }{ \partial x^2 }+tx, 0\leq x\leq \pi$ $t>0$
thats a driven wave equation. tx is the source term.
$u(0,t)=u(\pi,t)=0 \quad t>0$
$u(x,0)=\sin(x) \quad 0\leq x\leq \pi$
$\frac{ \partial u }{ \partial t }(x,0)=5\sin(2x)-3\sin(5x)\quad 0\leq x\leq \pi$
if any of the boundary conditions are non zero, then we have to split(?) into X and T.
in this case there's a $\sin(x)$ term so its a nonhomogenous equation (?)
when $tx$ wasn't there in last problem we had the solution:
$u(t,x)=\sum_{n=1}^\infty \underbrace{ (a_{n}\cos(nt)+b_{n}\sin(nt)) }_{ u_{n}(t) }\sin(nt)$ notice $L=\pi$
if we expand $tx$:
$tx=\sum_{n=1}^\infty h_{n}\sin(nx)$ (this is called a formal expansion, the two arent exactly equal due to the discontinuouity in tx.)
$h_{n}=\frac{2}{\pi}\int _{0} ^\pi tx\sin(nx)\, dx$
![draw](drawings/2023-12-06-13.14.28.excalidraw.png)
continuous between 0 and pi but on the edge ponts, the foureir sin series will converge to the midpoint of the two edge points.
$h_{n}=\frac{2t}{\pi}\int _{0}^\pi x\sin(nx)\, dx=- \frac{2t}{\pi n}\left( x\cos(nx)|_{0}^\pi-\int _{0}^\pi \cancel{ \cos(nx) }\, dx \right)$
$h_{n(t)}=\frac{2t}{n}(-1)^{n+1}$
$h(x,t)=tx=\sum_{n=1}^\infty h_{n}\sin(nx)=\sum_{n=1}^\infty \frac{2t}{n}(-1)^{n+1}\sin(nx)$
$\frac{ \partial^2 u }{ \partial t^2 }=\sum_{n=1}^\infty u_{n}''(t)\sin(nx)$
$\frac{ \partial^2 u }{ \partial x^2 }=\sum_{n=1}^\infty -u_{n}(t)n^2\sin(nx)$
$\sum_{n=1}^\infty \underbrace{ \left( u_{n}''+n^2u_{n}+\frac{2t}{n}(-1)^n \right) }_{ =0 }\sin(nx)=0$
$u''_{n}+n^2u_{n}=\frac{2}{n}(-1)^{n+1}t, \quad n=1,2,\dots$
use #mouc (or laplace, but that'll take much longer.)
characteristic eq:
$r^2+n^2=0$
$r_{1,2}=\pm in$
$u_{n}^h(t)=a_{n}\cos(nt)+b_{n}\sin(nt)$
$u_{n}^p(t)=At+B$
$B=0$ because there's no constant term on the RHS
$A=\frac{2(-1)^{n+1}}{n^3}$
$u_{n}(t)=a_{n}\cos(nt)+b_{n}\sin(nt)+\frac{2(-1)^{n+1}}{n^3}t$
$u(x,t)=\sum_{n=1}^\infty(a_{n}\cos(nt)+b_{n}\sin(nt)+\frac{2(-1)^{n+1}}{n^3}t)\sin(nx)$
This is the last problem I'll be solving in my career. This is the last time he's teaching math 201 :( or any course for that matter.
$u(x,0)=\sum_{n=1}^\infty a_{n}\sin(nx)=\sin(x)$
$a_{1}=1, \quad a_{k}=0, \quad k=2,3,\dots$
*audio recording started*
$\frac{ \partial u }{ \partial t }(x,0)=\sum_{n=1}^\infty\left( b_{n}n+\frac{2(-1)^{n+1}}{n^3} \right)\sin(nx)=5\sin(2x)-3\sin(5x)$
coefficients =0 if $n\ne_{2},5$
$\implies b_{n}=\frac{2}{n^4}(-1)^n, \quad n\ne_{2},5$
$b_{2}=\frac{5}{2}+\frac{2(-1)^2}{2^4}$
$b_{5}=-\frac{3}{5}+\frac{2(-1)^5}{5^4}$
$u(x,t)=\cos(t)\sin(x)+\frac{5}{2}\sin(2t)\sin(2x)-\frac{3}{5}\sin(5t)\sin(5x)+2\sum_{n=1}^\infty \frac{(-1)^{n+1}}{n^3}\left( t-\frac{\sin(nt)}{n} \right)\sin(nx)$
finished the solution
#end of lec 35
man I got teary eyed from this lecture.

2
content/_index.md
View File

@ -26,6 +26,8 @@ I have written these notes for myself, I thought it would be cool to share them.
[Separation of variables & Eigen value problems (lec 26-28)](separation-of-variables-eigen-value-problems-lec-26-28.html) [Separation of variables & Eigen value problems (lec 26-28)](separation-of-variables-eigen-value-problems-lec-26-28.html)
[Fourier series (lec 28-29)](fourier-series-lec-28-29.html) [Fourier series (lec 28-29)](fourier-series-lec-28-29.html)
[Partial differential equations (lec 30-34)](partial-differential-equations-lec-30-34.html) (raw notes, not reviewed or revised yet.) [Partial differential equations (lec 30-34)](partial-differential-equations-lec-30-34.html) (raw notes, not reviewed or revised yet.)
[Wave equations (lec 35)](wave-equations-lec-35.html) (raw notes, not reviewed or revised yet.)
</br> </br>
[How to solve any DE, a flow chart](Solve-any-DE.png) (Last updated Oct 1st, needs revision. But it gives a nice overview.) [How to solve any DE, a flow chart](Solve-any-DE.png) (Last updated Oct 1st, needs revision. But it gives a nice overview.)
[Big LT table (.png)](drawings/bigLTtable.png) [Big LT table (.png)](drawings/bigLTtable.png)

1258
content/drawings/2023-12-06-13.14.28.excalidraw.md Normal file
View File

File diff suppressed because it is too large Load Diff

BIN
content/drawings/2023-12-06-13.14.28.excalidraw.png Normal file
View File

Binary file not shown.
Side by Side

After

Width:  |  Height:  |  Size: 32 KiB

6
static/playaudio.js
View File

@ -22,7 +22,7 @@ var cspec = document.getElementById('spectrum'),
sliderFreq.oninput = function() { sliderFreq.oninput = function() {
textFreq.innerHTML=this.value; textFreq.innerHTML=this.value;
osc.frequency.value=this.value; osc.frequency.value=this.value/2;
} }
// Update the current slider value (each time you drag the slider handle) // Update the current slider value (each time you drag the slider handle)
slider.oninput = function() { slider.oninput = function() {
@ -43,7 +43,7 @@ slider.oninput = function() {
real[2*i] = (2/Math.PI) *( 1/(2*i+1)-1/(2*i-1) ); real[2*i] = (2/Math.PI) *( 1/(2*i+1)-1/(2*i-1) );
} }
osc.frequency.value = textFreq.innerHTML; osc.frequency.value = textFreq.innerHTML/2;
//var imag= new Float32Array([0,0,0,0,0]); // sine //var imag= new Float32Array([0,0,0,0,0]); // sine
//var real = new Float32Array(imag.length); // cos //var real = new Float32Array(imag.length); // cos
var customWave = context.createPeriodicWave(real, imag); // cos,sine var customWave = context.createPeriodicWave(real, imag); // cos,sine
@ -181,7 +181,7 @@ function playSound(h){
//var real = new Float32Array(imag.length); // cos //var real = new Float32Array(imag.length); // cos
var customWave = context.createPeriodicWave(real, imag); // cos,sine var customWave = context.createPeriodicWave(real, imag); // cos,sine
osc.setPeriodicWave(customWave); osc.setPeriodicWave(customWave);
osc.frequency.value = textFreq.innerHTML; osc.frequency.value = textFreq.innerHTML/2;
osc.connect(masterGain); osc.connect(masterGain);
osc.start(); osc.start();
isPlaying = true; isPlaying = true;