Transients, Two-Port Networks, Three-Phase Circuits and Power Measurement
What to remember
- Inductor current and capacitor voltage cannot change instantly. This gives the initial conditions for every transient problem.
- Time constant: τ = L / R for RL and τ = R C for RC. After 5τ the circuit is practically at steady state.
- For a balanced three-phase load, P = √3 V_L I_L cosφ. The two-wattmeter method measures this power, and its readings give the power factor.
Transients in first-order circuits
- RL circuit, DC step V: i(t) = (V/R) (1 - e^(-t/τ)), τ = L/R. Inductor voltage v_L = V e^(-t/τ).
- RC circuit charging: v_C(t) = V (1 - e^(-t/τ)), τ = R C. Charging current i = (V/R) e^(-t/τ).
- Discharge: v_C(t) = V0 e^(-t/τ).
- At t = τ the response has reached 63.2% of its final value (charging) or has fallen to 36.8% (decay). At 5τ it is above 99%.
- Initial conditions at t = 0+: an inductor with zero initial current acts as an open circuit; a capacitor with zero initial voltage acts as a short circuit. At steady state with DC, inductor is a short and capacitor is an open circuit.
- Energy stored: inductor ½ L I²; capacitor ½ C V².
Worked example: R = 10 ohm, L = 0.5 H, V = 100 V. τ = 0.5 / 10 = 0.05 s. Final current = 10 A. At t = τ, i = 10 x 0.632 = 6.32 A.
Worked example: R = 1 kilo-ohm and C = 100 microfarad give τ = 0.1 s. A capacitor charging from 0 reaches 63.2% of the supply in 0.1 s.
Second-order (series RLC) transients
Define α = R / (2L) and ω0 = 1 / √(LC).
| Case | Condition | Response |
|---|---|---|
| Over-damped | α > ω0 (R > 2√(L/C)) | Two real roots, slow non-oscillatory decay |
| Critically damped | α = ω0 (R = 2√(L/C)) | Fastest decay with no oscillation |
| Under-damped | α < ω0 (R < 2√(L/C)) | Decaying oscillation at ωd = √(ω0² - α²) |
Damping ratio ζ = α / ω0. Zero resistance gives undamped oscillation at ω0.
Worked example: L = 1 H, C = 1 microfarad. Critical resistance = 2 √(L / C) = 2 √(10⁶) = 2000 ohm.
Laplace transform pairs: L{1} = 1/s; L{t} = 1/s²; L{e^(-at)} = 1/(s + a); L{sin ωt} = ω / (s² + ω²); L{cos ωt} = s / (s² + ω²). For circuit elements: resistor R, inductor sL (with initial source L i(0)), capacitor 1/(sC) (with initial source v(0)/s). The initial value theorem is f(0+) = lim s F(s) as s tends to infinity; the final value theorem is f(∞) = lim s F(s) as s tends to 0.
Two-port networks
A two-port has an input port (V1, I1) and an output port (V2, I2), both currents taken into the network.
| Parameter set | Equations | Notes |
|---|---|---|
| Z (open-circuit) | V1 = Z11 I1 + Z12 I2; V2 = Z21 I1 + Z22 I2 | Found with ports open |
| Y (short-circuit) | I1 = Y11 V1 + Y12 V2; I2 = Y21 V1 + Y22 V2 | Found with ports shorted |
| ABCD (transmission) | V1 = A V2 - B I2; I1 = C V2 - D I2 | Used for cascade and transmission lines |
| h (hybrid) | V1 = h11 I1 + h12 V2; I2 = h21 I1 + h22 V2 | Used for transistor models |
- Reciprocal network: Z12 = Z21, Y12 = Y21, AD - BC = 1, h12 = -h21.
- Symmetrical network: Z11 = Z22, Y11 = Y22, A = D, and ΔH = 1 for h.
- Connections: series connection adds Z parameters; parallel connection adds Y parameters; cascade connection multiplies ABCD matrices.
- Conversions: Z = Y⁻¹; the determinant of ABCD for a reciprocal network is 1.
- Open-circuit voltage ratio V2/V1 with output open = 1 / A. Input impedance with output open = A / C.
Worked example: a series impedance Z alone has A = 1, B = Z, C = 0, D = 1. A shunt admittance Y alone has A = 1, B = 0, C = Y, D = 1. Cascading them multiplies these matrices.
Three-phase circuits
- Three voltages of equal magnitude, 120° apart in phase. The usual sequence is R-Y-B (positive).
- Star connection: V_L = √3 V_ph and I_L = I_ph. The line voltage leads the phase voltage by 30°. A neutral is available.
- Delta connection: V_L = V_ph and I_L = √3 I_ph. The line current lags the phase current by 30°.
- Power (balanced, either connection): P = √3 V_L I_L cosφ = 3 V_ph I_ph cosφ; Q = √3 V_L I_L sinφ; S = √3 V_L I_L. Here φ is the angle between phase voltage and phase current.
- A balanced delta load of impedance Z_ph is equal to a star load of Z_ph / 3.
- In a balanced system the neutral current is zero. In a four-wire unbalanced star, neutral current is the phasor sum of the three line currents.
- Advantages: constant instantaneous power in a balanced load, smaller conductor for the same power, self-starting motors.
Worked example: balanced delta load, each phase 20 ohm resistive, line voltage 400 V. I_ph = 400 / 20 = 20 A, I_L = 20 √3 = 34.6 A. P = 3 x 20² x 20 = 24 kW.
Worked example: balanced star, V_L = 400 V, each phase 100 ohm resistive. V_ph = 400 / √3 = 231 V; I = 2.31 A; P = 3 x 2.31² x 100 = 1600 W.
Power measurement
- Wattmeter: has a current coil (in series) and a pressure (voltage) coil (in parallel). Reading = V I cosφ.
- Blondel's theorem: to measure total power in an n-wire system, n - 1 wattmeters are enough, with one line as common return. So two wattmeters measure power in a three-wire three-phase system.
- Two-wattmeter method (balanced load): W1 = V_L I_L cos(30° - φ), W2 = V_L I_L cos(30° + φ), total P = W1 + W2. Power factor angle: tanφ = √3 (W1 - W2) / (W1 + W2).
| Power factor | Wattmeter readings |
|---|---|
| Unity (φ = 0) | Equal |
| 0.5 lagging (φ = 60°) | One reads zero, the other reads the full power |
| Below 0.5 | One reading is negative (reverse its connections) |
| Zero (pure reactance) | Equal in magnitude, opposite in sign |
Worked example: W1 = 3000 W and W2 = 0. P = 3000 W. tanφ = √3 x 3000 / 3000 = √3, so φ = 60° and pf = 0.5.
Worked example: W1 = 4000 W, W2 = 2000 W. P = 6000 W. tanφ = √3 x 2000 / 6000 = 0.577, so φ = 30° and pf = 0.866.
- Reactive power by one wattmeter on a balanced load: connect the current coil in one line and the pressure coil across the other two lines; Q = √3 x wattmeter reading.
- Energy meter: induction type meter measures kWh. The meter constant is revolutions per kWh; a pure-LED check uses pulses per kWh.
- Instrument transformers: a current transformer (CT) steps current down for meters (secondary usually 1 A or 5 A and never left open); a potential transformer (PT) steps voltage down (secondary commonly 110 V line). Burden is the load on the secondary, measured in VA.
- Moving coil (PMMC) instruments read DC average; moving iron instruments read RMS on both AC and DC; dynamometer type is used in wattmeters.
- Measurement of power factor: a power factor meter or computation from the two-wattmeter readings.
Exam traps
- Current in an inductor and voltage across a capacitor are continuous; the other quantities can jump.
- τ = L/R for RL but τ = RC for RC; do not swap.
- Critical damping gives the fastest non-oscillatory response, not the slowest.
- Z parameters use open circuits; Y parameters use short circuits.
- Cascade multiplies ABCD; parallel adds Y; series adds Z.
- In delta, line current is √3 times phase current; in star, line voltage is √3 times phase voltage.
- Power formula uses φ between phase voltage and phase current, not line quantities.
- A CT secondary must never be open-circuited; a PT secondary must never be short-circuited.
One-liners
- 1. Time constant of RL is L/R.
- 2. A capacitor reaches 63.2% of its final voltage in one time constant.
- 3. Critical resistance of a series RLC is 2√(L/C).
- 4. Reciprocity in Z-parameters means Z12 = Z21.
- 5. For reciprocal networks AD - BC = 1.
- 6. Star line voltage = √3 x phase voltage.
- 7. Delta line current = √3 x phase current.
- 8. Three-phase power P = √3 V_L I_L cosφ.
- 9. n - 1 wattmeters measure power in an n-wire system.
- 10. At 0.5 pf lagging, one wattmeter reads zero in the two-wattmeter method.
- 11. tanφ = √3 (W1 - W2) / (W1 + W2).
- 12. A current transformer secondary must not be left open.
Practice questions
The time constant of a series RL circuit is
- L / R
- 1 / (R L)
- R / L
- R L
Answer
A. L / R
The inductor current rises with time constant L / R.
The time constant of a series RC circuit is
- R / C
- R C
- 1 / (R C)
- C / R
Answer
B. R C
The capacitor voltage follows time constant RC.
Which quantity cannot change instantly in a circuit?
- Inductor voltage
- Resistor voltage
- Capacitor current
- Inductor current
Answer
D. Inductor current
Inductor current and capacitor voltage are continuous.
A capacitor charging through a resistor reaches what share of its final voltage in one time constant?
- 99 percent
- 63.2 percent
- 36.8 percent
- 50 percent
Answer
B. 63.2 percent
v = V (1 - e^-1) = 0.632 V.
At t = 0+ an uncharged capacitor behaves like
- A resistor of 1 ohm
- An open circuit
- An inductor
- A short circuit
Answer
D. A short circuit
With zero voltage the capacitor initially passes current freely.
At t = 0+ an inductor with zero initial current behaves like
- A capacitor
- A resistor
- An open circuit
- A short circuit
Answer
C. An open circuit
The current cannot jump, so the inductor opens at the instant.
In steady state with DC, an inductor behaves like
- A short circuit
- An open circuit
- A capacitor
- A battery
Answer
A. A short circuit
There is no voltage drop across an ideal inductor in DC steady state.
A two-port is reciprocal when
- Z12 = Z21
- Z11 = Z22
- Z11 = Z12
- Z12 = -Z21
Answer
A. Z12 = Z21
Equality of the transfer impedances gives reciprocity.
For a reciprocal two-port the ABCD parameters satisfy
- A = D
- B = C
- A + D = 1
- AD - BC = 1
Answer
D. AD - BC = 1
The determinant of the transmission matrix is unity.
In a balanced star connection the line voltage is
- Root three times smaller than the phase voltage
- One-third of the phase voltage
- Root three times the phase voltage
- Equal to the phase voltage
Answer
C. Root three times the phase voltage
V_L = sqrt(3) V_ph in star.
In a balanced delta connection the line current is
- Equal to the phase current
- Root three times the phase current
- Three times the phase current
- Half the phase current
Answer
B. Root three times the phase current
I_L = sqrt(3) I_ph in delta.
The power in a balanced three-phase system is
- 3 x V_L x I_L
- Root three x V_ph x I_L
- Root three x V_L x I_L x cos phi
- V_L x I_L x cos phi
Answer
C. Root three x V_L x I_L x cos phi
P = sqrt(3) V_L I_L cos(phi).
For a series RL circuit with R = 10 ohm and L = 0.5 H, the time constant is
- 20 s
- 0.05 s
- 0.5 s
- 5 s
Answer
B. 0.05 s
tau = L / R = 0.5 / 10 = 0.05 s.
A circuit has R = 1 kilo-ohm and C = 100 microfarad. The time constant is
- 10 s
- 0.01 s
- 1 s
- 0.1 s
Answer
D. 0.1 s
tau = R C = 1000 x 100 x 10^-6 = 0.1 s.
A 100 V DC step is applied to R = 10 ohm, L = 0.5 H. The current at t = one time constant is about
- 6.32 A
- 10 A
- 3.68 A
- 5 A
Answer
A. 6.32 A
Final 10 A, and i = 10 x 0.632 = 6.32 A.
The critical resistance of a series RLC circuit with L = 1 H and C = 1 microfarad is
- 500 ohm
- 2000 ohm
- 1000 ohm
- 4000 ohm
Answer
B. 2000 ohm
R = 2 sqrt(L / C) = 2 x 1000 = 2000 ohm.
A series RLC circuit has R = 500 ohm, L = 1 H and C = 1 microfarad. The response is
- Under-damped
- Over-damped
- Critically damped
- Undamped
Answer
A. Under-damped
Critical resistance is 2000 ohm; R below it gives an under-damped response.
A balanced delta load has 20 ohm resistive per phase on 400 V line voltage. The line current is about
- 60 A
- 11.5 A
- 20 A
- 34.6 A
Answer
D. 34.6 A
I_ph = 400 / 20 = 20 A; I_L = 20 x 1.732 = 34.6 A.
For the same delta load (20 ohm per phase, 400 V) the total power is
- 8 kW
- 48 kW
- 24 kW
- 12 kW
Answer
C. 24 kW
P = 3 x I_ph squared x R = 3 x 400 x 20 = 24 kW.
A balanced star load of 100 ohm per phase is on a 400 V line supply. The total power is about
- 2770 W
- 1600 W
- 533 W
- 4800 W
Answer
B. 1600 W
I = 231 / 100 = 2.31 A; P = 3 x 2.31 squared x 100 = 1600 W.
A balanced star system has a line voltage of 400 V. The phase voltage is about
- 231 V
- 400 V
- 133 V
- 693 V
Answer
A. 231 V
400 / 1.732 = 231 V.
A balanced load takes 10 A at 400 V line voltage with 0.8 power factor. The power is about
- 9.6 kW
- 3.2 kW
- 4.0 kW
- 5.54 kW
Answer
D. 5.54 kW
P = 1.732 x 400 x 10 x 0.8 = 5543 W.
A balanced three-phase load draws 5 A at 400 V line. The apparent power is about
- 2.0 kVA
- 10.4 kVA
- 3.46 kVA
- 6.0 kVA
Answer
C. 3.46 kVA
S = 1.732 x 400 x 5 = 3464 VA.
In the two-wattmeter method the readings are 3000 W and 0 W. The power factor is
- 0.707
- 0.866
- 1.0
- 0.5
Answer
D. 0.5
tan phi = sqrt(3) x 3000 / 3000 = sqrt(3), so phi = 60 degrees and pf = 0.5.
The two wattmeters read 4000 W and 2000 W. The total power is
- 6000 W
- 2000 W
- 3000 W
- 8000 W
Answer
A. 6000 W
The total is the sum of the two readings.
For readings of 4000 W and 2000 W the power factor is
- 0.5
- 0.866
- 1.0
- 0.707
Answer
B. 0.866
tan phi = sqrt(3) x 2000 / 6000 = 0.577, phi = 30 degrees, pf = 0.866.
In the two-wattmeter method both readings are 2 kW. The power factor and total power are
- 0.5 and 2 kW
- 0.866 and 4 kW
- Unity and 4 kW
- Unity and 2 kW
Answer
C. Unity and 4 kW
Equal readings mean zero phase angle, so pf = 1, total = 4 kW.
At power factor below 0.5, in the two-wattmeter method
- Both read zero
- Both read equal
- One reads exactly half
- One wattmeter reads negative
Answer
D. One wattmeter reads negative
When phi exceeds 60 degrees, W2 becomes negative.
By Blondel's theorem, the number of wattmeters needed for an n-wire system is
- n + 1
- n - 1
- 2 n
- n
Answer
B. n - 1
One line is taken as a common return.
A single wattmeter used for reactive power on a balanced load reads 2 kW. The reactive power is about
- 3.46 kVAR
- 2 kVAR
- 1.15 kVAR
- 6 kVAR
Answer
A. 3.46 kVAR
Q = sqrt(3) x 2 = 3.46 kVAR.
The Laplace transform of e^(-3t) is
- 1 / (s - 3)
- 3 / s
- 1 / (s + 3)
- s / (s + 3)
Answer
C. 1 / (s + 3)
L{e^(-at)} = 1 / (s + a).
An inductor of 2 H carries 3 A. The stored energy is
- 9 J
- 18 J
- 3 J
- 6 J
Answer
A. 9 J
W = 0.5 x 2 x 9 = 9 J.
A 100 microfarad capacitor is charged to 10 V. The stored energy is
- 50 mJ
- 10 mJ
- 1 mJ
- 5 mJ
Answer
D. 5 mJ
W = 0.5 x 100 x 10^-6 x 100 = 5 mJ.
A reciprocal two-port has A = 2, B = 3 and C = 1. The parameter D is
- 1
- 2
- 3
- 0.5
Answer
B. 2
AD - BC = 1 gives 2D - 3 = 1, so D = 2.
A current transformer's secondary should never be
- Short-circuited
- Connected to an ammeter
- Left open-circuited
- Earthed
Answer
C. Left open-circuited
An open secondary develops a dangerously high voltage.
Consider: 1. Z parameters are found with ports open-circuited. 2. Y parameters are found with ports short-circuited.
- 1 only
- 2 only
- Both 1 and 2
- Neither 1 nor 2
Answer
C. Both 1 and 2
Both statements are correct.
Consider: 1. Cascaded two-ports multiply ABCD matrices. 2. Series-connected two-ports add Y parameters.
- 1 only
- 2 only
- Both 1 and 2
- Neither 1 nor 2
Answer
A. 1 only
Series connection adds Z parameters; parallel adds Y.
Consider: 1. In star, line current equals phase current. 2. In delta, line voltage equals phase voltage.
- 1 only
- 2 only
- Both 1 and 2
- Neither 1 nor 2
Answer
C. Both 1 and 2
Both statements are correct.
Consider: 1. The time constant of an RC circuit is R / C. 2. After about 5 time constants a circuit is nearly at steady state.
- 1 only
- 2 only
- Both 1 and 2
- Neither 1 nor 2
Answer
B. 2 only
The RC time constant is the product R C.
Consider: 1. A critically damped circuit gives the fastest non-oscillatory response. 2. An under-damped circuit has oscillation in the response.
- 1 only
- 2 only
- Both 1 and 2
- Neither 1 nor 2
Answer
C. Both 1 and 2
Both statements describe the damping cases correctly.
Consider: 1. In a balanced system the neutral current is zero. 2. Three-phase balanced power is pulsating.
- 1 only
- 2 only
- Both 1 and 2
- Neither 1 nor 2
Answer
A. 1 only
Instantaneous power of a balanced load is constant.
Match in order: Z parameters, Y parameters, ABCD, h parameters
- Hybrid, transmission, short-circuit admittance, open-circuit impedance
- Transmission, hybrid, open-circuit impedance, short-circuit admittance
- Short-circuit admittance, open-circuit impedance, hybrid, transmission
- Open-circuit impedance, short-circuit admittance, transmission, hybrid
Answer
D. Open-circuit impedance, short-circuit admittance, transmission, hybrid
These are the standard names of the parameter sets.
Match in order: Over-damped, Critically damped, Under-damped, Undamped
- alpha = w0, alpha > w0, R = 0, alpha < w0
- R = 0, alpha < w0, alpha = w0, alpha > w0
- alpha < w0, alpha = w0, alpha > w0, R = 0
- alpha > w0, alpha = w0, alpha < w0, R = 0
Answer
D. alpha > w0, alpha = w0, alpha < w0, R = 0
The damping condition decides the response type.
Three-phase power in a balanced load is constant in time. A key advantage of this is
- Lower voltage
- Smooth torque in motors
- Zero neutral wire needed always
- Higher line frequency
Answer
B. Smooth torque in motors
Constant instantaneous power gives steady motor torque.
A balanced delta load of 30 ohm per phase is replaced by an equivalent star load. Each star arm is
- 17.3 ohm
- 90 ohm
- 30 ohm
- 10 ohm
Answer
D. 10 ohm
Z(star) = Z(delta) / 3 = 10 ohm.