Physics·Revision Notes

Impedance — Revision Notes

NEET UG
Version 1Updated 22 Mar 2026

⚡ 30-Second Revision

  • Impedance (Z):Total opposition to AC current. Unit: Ohm (Ω\Omega).\n- Resistance (R): Frequency-independent, dissipates heat. VRV_R in phase with II.\n- **Inductive Reactance (XLX_L):** XL=ωL=2πfLX_L = \omega L = 2\pi f L. Increases with ff. Current lags voltage by 9090^\circ (ELI).\n- **Capacitive Reactance (XCX_C):** XC=1ωC=12πfCX_C = \frac{1}{\omega C} = \frac{1}{2\pi f C}. Decreases with ff. Current leads voltage by 9090^\circ (ICE).\n- Series RLC Impedance: Z=R2+(XLXC)2Z = \sqrt{R^2 + (X_L - X_C)^2}.\n- **Phase Angle (ϕ\phi):** tanϕ=XLXCR\tan \phi = \frac{X_L - X_C}{R}. Positive ϕ\phi (inductive), Negative ϕ\phi (capacitive), ϕ=0\phi=0 (resistive/resonance).\n- Resonance: XL=XC    Z=RX_L = X_C \implies Z=R (minimum), ImaxI_{max}, ϕ=0\phi=0. Resonant frequency f0=12πLCf_0 = \frac{1}{2\pi\sqrt{LC}}.\n- Power Factor: cosϕ=RZ\cos \phi = \frac{R}{Z}.

2-Minute Revision

Impedance (ZZ) is the AC equivalent of resistance, representing the total opposition to current flow. It's composed of resistance (RR), inductive reactance (XLX_L), and capacitive reactance (XCX_C).

Resistance is constant, but XLX_L increases with frequency (XL=2πfLX_L = 2\pi f L) and XCX_C decreases with frequency (XC=12πfCX_C = \frac{1}{2\pi f C}). These components don't add arithmetically due to phase differences: current is in phase with voltage across RR, lags by 9090^\circ across LL, and leads by 9090^\circ across CC.

For a series RLC circuit, impedance is calculated as Z=R2+(XLXC)2Z = \sqrt{R^2 + (X_L - X_C)^2}. The phase angle ϕ=arctan(XLXCR)\phi = \arctan\left(\frac{X_L - X_C}{R}\right) tells us if the circuit is inductive (XL>XCX_L > X_C, voltage leads current) or capacitive (XC>XLX_C > X_L, voltage lags current).

The special condition where XL=XCX_L = X_C is called resonance, leading to minimum impedance (Z=RZ=R), maximum current, and zero phase angle. The power factor, cosϕ=R/Z\cos \phi = R/Z, indicates how effectively power is utilized.

5-Minute Revision

Impedance (ZZ) is the crucial concept for understanding AC circuits, generalizing resistance to include the effects of inductors and capacitors. It's the total opposition to alternating current, measured in Ohms.

Unlike resistance, impedance is frequency-dependent due to its reactive components: inductive reactance (XL=2πfLX_L = 2\pi f L) and capacitive reactance (XC=12πfCX_C = \frac{1}{2\pi f C}). XLX_L increases with frequency, while XCX_C decreases.

Resistance (RR) remains constant.\n\nIn a series RLC circuit, these three components combine vectorially. The voltage across the resistor (VRV_R) is in phase with the current (II). The voltage across the inductor (VLV_L) leads the current by 9090^\circ, and the voltage across the capacitor (VCV_C) lags the current by 9090^\circ.

This 9090^\circ phase difference means we use the Pythagorean theorem to find the total impedance: Z=R2+(XLXC)2Z = \sqrt{R^2 + (X_L - X_C)^2}. The term (XLXC)(X_L - X_C) is the net reactance, XX. If XL>XCX_L > X_C, the circuit is inductive, and the total voltage leads the current.

If XC>XLX_C > X_L, it's capacitive, and the total voltage lags the current. The phase angle ϕ\phi is given by tanϕ=XLXCR\tan \phi = \frac{X_L - X_C}{R}.\n\nResonance is a critical condition where XL=XCX_L = X_C.

At this specific resonant frequency (f0=12πLCf_0 = \frac{1}{2\pi\sqrt{LC}}), the net reactance becomes zero, and the impedance is at its minimum value, Z=RZ=R. This leads to the maximum current in the circuit for a given voltage, and the phase angle ϕ=0\phi=0, meaning the circuit behaves purely resistively.

Understanding how to calculate ZZ, XLX_L, XCX_C, and ϕ\phi is essential for solving problems related to current, voltage drops across components, and power factor (cosϕ=R/Z\cos \phi = R/Z) in AC circuits.

Prelims Revision Notes

Impedance (Z) - NEET Quick Notes\n\n1. Definition: Total opposition to AC current flow. Unit: Ohm ($\Omega$).\n\n2. Components of Impedance:\n * Resistance (R):\n * Opposition due to energy dissipation (heat).\n * Independent of frequency.\n * Voltage ($V_R$) and current ($I$) are in phase.\n * Inductive Reactance ($X_L$):\n * Opposition by an inductor (L) to changing current.\n * Formula: $X_L = \omega L = 2\pi f L$.\n * Increases linearly with frequency ($f$).\n * Current lags voltage by $90^\circ$ (ELI: E leads I in L).\n * Capacitive Reactance ($X_C$):\n * Opposition by a capacitor (C) to changing voltage.\n * Formula: $X_C = \frac{1}{\omega C} = \frac{1}{2\pi f C}$.\n * Decreases inversely with frequency ($f$).\n * Current leads voltage by $90^\circ$ (ICE: I leads E in C).\n\n3. Series RLC Circuit Impedance:\n * Total impedance: $Z = \sqrt{R^2 + (X_L - X_C)^2}$.\n * Net Reactance: $X = X_L - X_C$.\n * Impedance Triangle: Right triangle with sides $R$, $X$, and hypotenuse $Z$.\n\n4. Phase Angle ($\phi$):\n * Phase difference between total voltage and total current.\n * Formula: $\tan \phi = \frac{X_L - X_C}{R}$.\n * If $X_L > X_C$: Circuit is inductive, $\phi$ is positive (voltage leads current).\n * If $X_C > X_L$: Circuit is capacitive, $\phi$ is negative (voltage lags current).\n * If $X_L = X_C$: Circuit is purely resistive, $\phi = 0$.\n\n5. Resonance in Series RLC Circuit:\n * Condition: $X_L = X_C$.\n * Resonant Frequency ($f_0$): $f_0 = \frac{1}{2\pi\sqrt{LC}}$.\n * At Resonance: $Z = R$ (minimum impedance), $I_{rms} = V_{rms}/R$ (maximum current), $\phi = 0$.\n\n6. Ohm's Law for AC Circuits:\n * $I_{rms} = V_{rms}/Z$ or $I_{peak} = V_{peak}/Z$.\n\n7. Power Factor (PF):\n * $PF = \cos \phi = \frac{R}{Z}$.\n * Measures how much of the apparent power is real power.\n\nKey Points for NEET:\n* Always convert units (mH to H, $\mu$F to F) before calculation.\n* Remember vectorial addition for $Z$, not arithmetic sum.\n* Master phase relationships (ELI vs ICE).

Vyyuha Quick Recall

To remember the phase relationships in AC circuits: ELI the ICE man\n\n* ELI: In an inductor (L), Voltage (E) leads Current (I).\n* ICE: In a capacitor (C), Current (I) leads Voltage (E).

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