
Define the time constant for resistor–inductor circuits and derive the initial and final voltages and currents in an inductor, predicting exponential decay with time.
Learn the four equations that describe exponential voltage and current in inductors, including decays to zero or non-zero endpoints with initial, final, offset values, and the time constant tau.
Explore how the time constant controls voltage and current decay in rl circuits using v0 e^{-t/tau}, with drops to 37% after one, 14% after two, and 5% after three.
Explore how voltages and currents in RL circuits rise toward their final values, reaching 63% at one time constant, 86% at two, and 95% at three.
Calculate the time constant tau for resistor-inductor circuits by dividing inductance by the resistance the inductor sees, with practical examples.
An introductory inductor–resistor circuit demonstrates current decay from 3.5 amps, with a time constant of 45 ms (L/R), following i(t)=I0 e^{-t/τ}.
Explore a 680 μH inductor with 50 A initial current, fed through a 1 Ω resistor into a 2 Ω || 3 Ω parallel, yielding time constant and current distribution.
Explore how resistor-inductor circuits cause current to change gradually, governed by the time constant L/R, and predict voltage and current behavior.
Day 26 of Linear Circuits. Inductors are one of the three passive circuit components (along with resistors and capacitors). However, their operation and behavior is often shrouded in mystery. After seeing what inductors are and how they work in our previous lecture, today, we will see how we can always find the initial and final values for resistor-inductor circuits' currents and voltages AND specify their entire behavior by just one variable -- the time constant, TAU.
The material covers all of the lecture material from an twenty-sixth lecture in a traditional, sophomore-level linear circuits class.