INGENIA

EMG-06

Series RLC impedance

Z = √(R² + (ωL − 1/(ωC))²).

Reading speed
AC circuitsSteinmetz

Governing equation

Z=R2+(ωL−1ωC)2Z=\sqrt{R^2+\left(\omega L-\dfrac{1}{\omega C}\right)^2}

f∈[1,2000]f \in \left[1, 2000\right]

where

R
Resistance (Ω)
L
Inductance (mH)
C
Capacitance (µF)
f
Frequency (Hz)
Z
Impedance (Ω)
\varphi
Phase (°)

The figure, part by part

Each numbered marker wears the color of its card. Hover a card to light the marker. Tap a marker to jump to that card. The slider walks a red point along the curve; Animate drawing traces it like a pen.

EMG-06 · circuit
00:0 / 00:08
①

Governing law — red

Z=R2+(ωL−1ωC)2Z=\sqrt{R^2+\left(\omega L-\dfrac{1}{\omega C}\right)^2}

f∈[1,2000]f \in \left[1, 2000\right]

f=1f = 1Z=3978.7Z = 3978.7

②

Domain of the variable — blue

fmin⁡=1,fmax⁡=2000f_{\min} = 1,\quad f_{\max} = 2000

f∈[1,2000]f \in \left[1, 2000\right]

f=1f = 1f=1f = 1

③

Response curve — green

Z=R2+(ωL−1ωC)2Z=\sqrt{R^2+\left(\omega L-\dfrac{1}{\omega C}\right)^2}

f∈[1,2000]f \in \left[1, 2000\right]

f=1f = 1Z=3978.7Z = 3978.7

④

Rate of change — amber

dZdf\frac{\mathrm{d}Z}{\mathrm{d}f}

f∈[1,2000]f \in \left[1, 2000\right]

f=13.57f = 13.57Z′=−152.3Z^{\prime} = -152.3

Lecture brief

Historical brief

Coulomb, Gauss, Ampère, Faraday and Maxwell (1861–65) unified charge, current and light. The lab computes fields, induction, Poynting flux and the electromagnetic wave in SI. This sheet (EMG-06 — Series RLC impedance) is the form associated with Steinmetz. Working symbols: RR, LL, CC, ff →\rightarrow ZZ, φ\varphi. Phasor addition of resistance and the two reactances yields the magnitude of series impedance, minimum at resonance.

Purpose

Purpose: compute ZZ, φ\varphi from RR, LL, CC, ff in Electromagnetism via Z=R2+(ωL−1ωC)2Z=\sqrt{R^2+\left(\omega L-\dfrac{1}{\omega C}\right)^2} Z = √(R² + (ωL − 1/(ωC))²). Use it when a real electromagnetism question must be answered in SI before a code check.

Live realistic example

In symbols

Live case. Given R=10.000 ΩR = 10.000\,\mathrm{Ω}, L=25.000 mHL = 25.000\,\mathrm{mH}, C=40.000 μFC = 40.000\,\mathrm{\mu F}, f=50.000 Hzf = 50.000\,\mathrm{Hz}, the governing relation Z=R2+(ωL−1ωC)2Z=\sqrt{R^2+\left(\omega L-\dfrac{1}{\omega C}\right)^2} yields Z=72.417 ΩZ = 72.417\,\mathrm{Ω}, φ=−82.063 ∘\varphi = -82.063\,\mathrm{^{\circ}}. Linear lumped R, L, C driven by a sinusoid. Move a slider: the numbers are this situation, not a canned story.

Calculator

Inputs

Outputs

  • Impedance Z72.417 Ω
  • Phase \varphi-82.063 °
Reading speed

Watch on YouTube

Free library

Full library

Free PDF / open book

YouTube channels

EMG-06 · circuit
00:0 / 00:08

Narration of this film

Linear lumped R, L, C driven by a sinusoid.

Phasor addition of resistance and the two reactances yields the magnitude of series impedance, minimum at resonance.

Reading speed

Watch on YouTube