For MAXIMUM POWER TRANSFER from a source with internal resistance $R_S$ to a load $R_L$, we need
A$R_L = 0$ (short)
B$R_L = R_S$
C$R_L \to \infty$ (open)
D$R_L = 2R_S$
Answer & Solution
Correct answer: B. $R_L = R_S$
1. Total resistance: $R_S + R_L$. Current: $I = V/(R_S + R_L)$.
2. Power in load: $P_L = I^2 R_L = V^2 R_L/(R_S + R_L)^2$.
3. Maximise: $dP_L/dR_L = 0$ gives $R_L = R_S$.
4. At this match, $P_L = V^2/(4R_S)$. Source dissipates equal power, so EFFICIENCY = 50% only.
5. Used in audio amplifier output matching, antenna feed-line matching, etc.
6. Options A, C, D give zero power transfer or sub-optimal.
_Source: Tony Kuphaldt, "Lessons in Electric Circuits — DC", Vol I, Ch 10 (Max power transfer)._
Keep practising Electric Circuits
Browse all Electric Circuits questions for GATE EE, or explore more Electrical Engineering topics.
Related questions
Drop each trait into Thevenin or NortonStack equal resistors into one valueThe QUALITY FACTOR Q of a series RLC resonant circuit measuresThe IMPEDANCE of a series RL circuit at angular frequency $\omega$ isAn RMS AC voltage of $230\,\text{V}$ drives a $100\Omega$ RESISTIVE load. The real power dIn an AC circuit with a pure CAPACITOR, the currentIn an AC circuit with a pure INDUCTOR, the currentA purely RESISTIVE AC load has voltage and current that are