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Parallel RL and RC branch currents, power

Short answer

Z1 = 18+j24 = 30∠53.13° Ω, Z2 = 15-j30 = 33.54∠-63.43° Ω. I1 = 200∠53.8° / Z1 = 6.667∠0.67° A, I2 = 200∠53.8° / Z2 = 5.963∠117.23° A. Total current I = I1+I2 = 6.667∠53.8° A. Real power = I1²×18 + I2²×15 = 1333.3 W.

From the given circuit, find total current (I), branch currents I1I_1 and I2I_2, and real power. [Figure: source 200∠53.8°200\angle 53.8° V feeding two parallel branches; branch 1 (I1I_1) has 18 Ω18\ \Omega in series with j24 Ωj24\ \Omega; branch 2 (I2I_2) has 15 Ω15\ \Omega in series with −j30 Ω-j30\ \Omega.]

Given: V=200∠53.8∘V=200\angle53.8^\circ V, Z1=18+j24=30∠53.13∘ ΩZ_1=18+j24=30\angle53.13^\circ\ \Omega, Z2=15−j30=33.54∠−63.43∘ ΩZ_2=15-j30=33.54\angle-63.43^\circ\ \Omega.

Branch currents:

I1=VZ1=200∠53.8∘30∠53.13∘=6.667∠0.67∘ AI_1=\frac{V}{Z_1}=\frac{200\angle53.8^\circ}{30\angle53.13^\circ}=6.667\angle0.67^\circ\ \text{A} I2=VZ2=200∠53.8∘33.54∠−63.43∘=5.963∠117.23∘ AI_2=\frac{V}{Z_2}=\frac{200\angle53.8^\circ}{33.54\angle-63.43^\circ}=5.963\angle117.23^\circ\ \text{A}

Total current (phasor sum):

I=I1+I2=(6.667+j0.078)+(−2.728+j5.302)=3.939+j5.380I=I_1+I_2=(6.667+j0.078)+(-2.728+j5.302)=3.939+j5.380

In polar form, I=6.667∠53.8∘I=6.667\angle53.8^\circ A. The total current is in phase with the source voltage: the reactive parts of the two branch admittances cancel (1Z1+1Z2=130\frac{1}{Z_1}+\frac{1}{Z_2}=\frac{1}{30} S), so the combination behaves as a pure 30 Ω resistance.

Real power:

P=I12R1+I22R2=(6.667)2×18+(5.963)2×15=800+533.3=1333.3 WP=I_1^2R_1+I_2^2R_2=(6.667)^2\times18+(5.963)^2\times15=800+533.3=1333.3\ \text{W}

Check with P=VIcos⁡ϕ=200×6.667×cos⁡0∘=1333.3P=VI\cos\phi=200\times6.667\times\cos0^\circ=1333.3 W, where ϕ=0\phi=0 since II and VV have the same angle.

Answer: I=6.667∠53.8∘I=6.667\angle53.8^\circ A, I1=6.667∠0.67∘I_1=6.667\angle0.67^\circ A, I2=5.963∠117.23∘I_2=5.963\angle117.23^\circ A, P=1333.3P=1333.3 W (unity power factor).

✓ Answer checked by Claude Opus 5.5 (high effort)

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