From 609afd96f4069c69945fedcdfa7787ae4f7de967 Mon Sep 17 00:00:00 2001 From: Holden Rohrer Date: Sat, 4 Apr 2020 02:21:04 -0400 Subject: attempted (but wrong) start of solution --- progreport/document.tex | 34 +--------------------------------- 1 file changed, 1 insertion(+), 33 deletions(-) (limited to 'progreport') diff --git a/progreport/document.tex b/progreport/document.tex index 7b34439..af7da22 100644 --- a/progreport/document.tex +++ b/progreport/document.tex @@ -2,39 +2,7 @@ \input ../format \titlesub{Part 2: Progress Report}{Topic: Mystery Circuit} -\section{Project Topic} - -Our group will be working on the \link{Mystery Circuit Modelling -Scenario from SIMIODE}{https://simiode.org/resources/3187/download/4-23% --S-MysteryCircuit-StudentVersion.pdf}. This applies Kirchhoff's Voltage -and Current Laws to the given circuit, which describe, respectively, -that the sum of all voltages in a closed loop is zero and the sum of all -currents at a node is zero. The circuit we're examining is an RLC -(resistor, inductor, capacitor) circuit, with zeroed initial conditions. -The specific circuit has two linked loops of resistors and capacitors, -in which ``gain,'' the ratio between chosen voltage differentials in the -circuit can be modeled mathematically. Because there are two connected -loops, there are three different currents. There is the current coming -off of the battery $x(t)$, the current split at the middle node becoming -$y(t)$ and $z(t)$. We are examining ${E(t)\over z(t)\rload}$ as the -``gain'' in the system. The first part uses $\omega = 100$ and the -entire problem uses $E(t) = \sin(\omega t)$. - -\section{Progress} - -From Kirchhoff's Voltage law over the first (xy) loop, -$$E(t) = \sin(\omega t) = x(t)R_1 + {1\over C_1}\int y(t)dt.$$ -Kirchhoff's Voltage law also applies to the second (yz) loop: -$${1\over C_1}\int y(t)dt = {1\over C_2}\int z(t)dt + z(t)\rload.$$ -Differentiating and rearranging gives: -$$x'(t) = -{y(t) \over R_1C_1} + {\omega\cos(\omega t) \over R_1},$$ -$$z'(t) = {y(t) \over C_1\rload} - {z(t) \over C_2\rload}$$ - -Kirchhoff's current law tells us that $y(t) + z(t) = x(t)$, so -$$y'(t) = x'(t) - z'(t) = -{y(t)\over R_1C_1} + -{\omega\cos(\omega t) \over R_1} - {y(t)\over C_1\rload} -+ {z(t) \over C_2\rload},$$ -giving a system of differential equations to solve. +\input ../com \section{Further Exploration} -- cgit