What is the average power dissipation in an RLC series circuit with R=10 ohm, L=0.1 H, C=10 MF, when driven at resonance by 100 V-RMS source
P=Irms×UrmsP=I_{rms}\times U_{rms}P=Irms×Urms ; Z=R2+(LLC−LCC)2Z=\sqrt{R^2+(\frac{L}{\sqrt{LC}}-\frac{\sqrt{LC}}{C})^2}Z=R2+(LCL−CLC)2
Irms=UrmsZ=I_{rms}=\frac{U_{rms}}{Z}=Irms=ZUrms= UrmsR2+(LLC−LCC)\frac{U_{rms}}{\sqrt{R^2+(\frac{L}{\sqrt{LC}}-\frac{\sqrt{LC}}{C})}}R2+(LCL−CLC)Urms =100102+(0.10.1×10−2−0.1×10−210−2)2=10=\frac{100}{\sqrt{10^2+(\frac{0.1}{\sqrt{0.1\times10^{-2}}}-\frac{\sqrt{0.1\times10^{-2}}}{10^{-2}})^2}}=10=102+(0.1×10−20.1−10−20.1×10−2)2100=10 A
P=10×100=1000P=10\times100=1000P=10×100=1000 W.
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