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For sinusoidal AC, the series impedance magnitude is the quadratic combination of resistance and net reactance.
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Formula
Z, R, XL and XC in Ω; ω in rad/s; L in H; C in F
| Symbol | Meaning | Unit |
|---|---|---|
| Magnitude of complex series impedance | Ω | |
| Ohmic resistance | Ω | |
| Angular frequency 2πf | rad/s | |
| Inductance | H | |
| Capacitance | F |
Z=\sqrt{R^2+(\omega L-1/(\omega C))^2}For ideal series R, L and C, the complex impedance is R+j(ωL−1/ωC); the displayed expression is its magnitude. It applies in sinusoidal steady state with linear elements. At resonance, inductive and capacitive reactances cancel and Z=R. Component losses and parasitics can change real frequency response.
For ideal series R, L and C, the complex impedance is R+j(ωL−1/ωC); the displayed expression is its magnitude. It applies in sinusoidal steady state with linear elements. At resonance, inductive and capacitive reactances cancel and Z=R. Component losses and parasitics can change real frequency response.
For sinusoidal AC, the series impedance magnitude is the quadratic combination of resistance and net reactance.
Base equation for the target quantity
Preserve signs, boundary conditions and units when rearranging.
Work through the numerical example for “Impedance of a series RLC circuit” and check its unit and magnitude.
For R=30 Ω, f=50 Hz, L=0.10 H and C=100 μF, XL≈31.4 Ω and XC≈31.8 Ω, so Z≈30.0 Ω.
Substituting a related quantity that shares the same symbol.
Use variable definitions and check: Z, R, XL and XC in Ω; ω in rad/s; L in H; C in F.
Formula cluster
For sinusoidal AC, the series impedance magnitude is the quadratic combination of resistance and net reactance.
For R=30 Ω, f=50 Hz, L=0.10 H and C=100 μF, XL≈31.4 Ω and XC≈31.8 Ω, so Z≈30.0 Ω.
Calculate AC current, phase behavior and frequency response of series RLC networks.
Here is how to work through a typical Impedance of a series RLC circuit (Z = √[R² + (ωL − 1/(ωC))²]) task step by step:
Task
Work through the numerical example for “Impedance of a series RLC circuit” and check its unit and magnitude.
Solution path
For R=30 Ω, f=50 Hz, L=0.10 H and C=100 μF, XL≈31.4 Ω and XC≈31.8 Ω, so Z≈30.0 Ω.
Inductive reactance is XL=ωL and capacitive reactance is XC=1/(ωC). Both are measured in ohms, although they store energy temporarily rather than dissipating it like resistance. Use ω in rad/s and carefully convert millihenry and microfarad. The equation gives impedance magnitude only for ideal series components in sinusoidal steady state. Reactances depend on ω=2πf. To find phase, retain complex form R+j(XL−XC); magnitude alone loses whether the circuit is net inductive or capacitive. Finally check units, assumptions, measurement conditions and reference quantities against the problem before using the result.
At resonance, ωL=1/(ωC), so inductive and capacitive reactance cancel in series. Then Z=R and current is ideally in phase with source voltage. Resonant frequency is ω0=1/√(LC). Losses and parasitics can shift or broaden real resonance. The equation gives impedance magnitude only for ideal series components in sinusoidal steady state. Reactances depend on ω=2πf. To find phase, retain complex form R+j(XL−XC); magnitude alone loses whether the circuit is net inductive or capacitive. Finally check units, assumptions, measurement conditions and reference quantities against the problem before using the result.
No. Magnitude Z gives only the size of the voltage–current ratio. Phase follows from φ=arctan[(XL−XC)/R] with correct quadrant handling. Positive net reactance is inductive; negative is capacitive. Keep complex impedance for sign and phase analysis. The equation gives impedance magnitude only for ideal series components in sinusoidal steady state. Reactances depend on ω=2πf. To find phase, retain complex form R+j(XL−XC); magnitude alone loses whether the circuit is net inductive or capacitive. Finally check units, assumptions, measurement conditions and reference quantities against the problem before using the result.
Write the quantity and unit from the variable list next to every value: Z, R, XL and XC in Ω; ω in rad/s; L in H; C in F. Substitute only after converting to a consistent unit system, and state sign or reference direction explicitly. The example For R=30 Ω, f=50 Hz, L=0.10 H and C=100 μF, XL≈31.4 Ω and XC≈31.8 Ω, so Z≈30.0 Ω. is a calculation check: result, unit and order of magnitude must fit the described situation. Round after intermediate calculations so small contributions are not lost prematurely. The equation gives impedance magnitude only for ideal series components in sinusoidal steady state. Reactances depend on ω=2πf. To find phase, retain complex form R+j(XL−XC); magnitude alone loses whether the circuit is net inductive or capacitive. Finally check units, assumptions, measurement conditions and reference quantities against the problem before using the result.
The background states this starting condition: For ideal series R, L and C, the complex impedance is R+j(ωL−1/ωC); the displayed expression is its magnitude.. That limits when the result is a valid model prediction. Compare the problem’s boundary conditions with this assumption before substituting values; real components, material properties or loads can introduce additional effects. The cited reference supports the relation used here but does not remove the need to check whether the specific case fits the model. The equation gives impedance magnitude only for ideal series components in sinusoidal steady state. Reactances depend on ω=2πf. To find phase, retain complex form R+j(XL−XC); magnitude alone loses whether the circuit is net inductive or capacitive. Finally check units, assumptions, measurement conditions and reference quantities against the problem before using the result.
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