Given: C = 100 μ F ; R = 34 Ω ; v ( t ) = 220 ⋅ s i n ( 314 ⋅ t ) V C=100\mu F; R=34\Omega; v(t)=220\cdot sin(314\cdot t)V C = 100 μ F ; R = 34Ω ; v ( t ) = 220 ⋅ s in ( 314 ⋅ t ) V
Solution: (a) An AC voltage source in our problem has w = 314 r a d / s w=314 rad/s w = 314 r a d / s and can be written as v ( t ) = I m ( V a ⋅ e i w t ) v(t)=Im(V_a\cdot e^{iwt}) v ( t ) = I m ( V a ⋅ e i wt ) where V a = 220 V V_a=220V V a = 220 V (Note e i w t = c o s ( w t ) + i ⋅ s i n ( w t ) e^{iwt}=cos(wt)+i\cdot sin(wt) e i wt = cos ( wt ) + i ⋅ s in ( wt ) ).
To find the current in a series AC circuit we determine the component of its impedance
(1) Z = R + 1 i w C = R − i X c Z=R+\frac{1}{iwC}=R-iX_c Z = R + i wC 1 = R − i X c , where X c = 1 w C = 1 100 ⋅ 1 0 − 6 F ⋅ 314 r a d / s = 31.8 Ω X_c=\frac{1}{wC}=\frac{1}{100\cdot 10^{-6}F\cdot 314 rad/s}=31.8\Omega X c = wC 1 = 100 ⋅ 1 0 − 6 F ⋅ 314 r a d / s 1 = 31.8Ω
We can write the impedance in a form
(2) Z = ∣ Z ∣ ⋅ e i ϕ Z=|Z|\cdot e^{i\phi} Z = ∣ Z ∣ ⋅ e i ϕ , where ∣ Z ∣ = R 2 + X c 2 = 3 4 2 + 31. 8 2 Ω = 46.6 Ω |Z|=\sqrt{R^2+X_c^2}=\sqrt{34^2+31.8^2}\Omega=46.6\Omega ∣ Z ∣ = R 2 + X c 2 = 3 4 2 + 31. 8 2 Ω = 46.6Ω and ϕ = a r c t a n ( − X c R ) = − a r c t a n ( 31.8 34 ) = − 0.753 r a d \phi=arctan(\frac{-X_c}{R})=-arctan(\frac{31.8}{34})=-0.753 rad ϕ = a rc t an ( R − X c ) = − a rc t an ( 34 31.8 ) = − 0.753 r a d (a r c t a n arctan a rc t an also denote as t a n − 1 tan^{-1} t a n − 1 )
(2) According to the definition of impedance we have Z = v i Z=\frac{v}{i} Z = i v thus
(3) i = v Z i=\frac{v}{Z} i = Z v , where v = V a ⋅ e i w t v=V_a\cdot e^{iwt} v = V a ⋅ e i wt and
(4) i ( t ) = I m ( i ) = I m ( V a ⋅ e i w t ∣ Z ∣ e i ϕ ) = V a ∣ Z ∣ ⋅ I m ( e i w t ⋅ e − i ϕ ) = V a ∣ Z ∣ s i n ( w t − ϕ ) i(t)=Im(i)=Im(\frac{V_a\cdot e^{iwt}}{|Z|e^{i\phi}})=\frac{V_a}{|Z|}\cdot Im(e^{iwt}\cdot e^{-i\phi})=\frac{V_a}{|Z|}sin(wt-\phi) i ( t ) = I m ( i ) = I m ( ∣ Z ∣ e i ϕ V a ⋅ e i wt ) = ∣ Z ∣ V a ⋅ I m ( e i wt ⋅ e − i ϕ ) = ∣ Z ∣ V a s in ( wt − ϕ ) and finally
(5) i ( t ) = V a ∣ Z ∣ s i n ( w t − ϕ ) = 220 V 46.6 Ω s i n ( 314 t + 0.753 ) = 4.72 ⋅ s i n ( 314 t + 0.753 ) A i(t)=\frac{V_a}{|Z|}sin(wt-\phi)=\frac{220V}{46.6\Omega}sin(314t+0.753)=4.72\cdot sin(314t+0.753)A i ( t ) = ∣ Z ∣ V a s in ( wt − ϕ ) = 46.6Ω 220 V s in ( 314 t + 0.753 ) = 4.72 ⋅ s in ( 314 t + 0.753 ) A
(b) Real power of our circuit is
P = ∣ I r m s ∣ 2 ⋅ R = ( 4.72 / 2 ) 2 ⋅ A 2 ⋅ 34 Ω = 379 W P=|I_{rms}|^2\cdot R=(\frac{4.72}{/\sqrt{2}})^2\cdot A^2\cdot 34\Omega=379W P = ∣ I r m s ∣ 2 ⋅ R = ( / 2 4.72 ) 2 ⋅ A 2 ⋅ 34Ω = 379 W
Reactive power is
Q = ∣ I r m s ∣ 2 ⋅ X c = ( 4.72 / 2 ) 2 ⋅ A 2 ⋅ 31.8 Ω = 354 V A r Q=|I_{rms}|^2\cdot X_c=(\frac{4.72}{/\sqrt{2}})^2\cdot A^2\cdot 31.8\Omega=354VAr Q = ∣ I r m s ∣ 2 ⋅ X c = ( / 2 4.72 ) 2 ⋅ A 2 ⋅ 31.8Ω = 354 V A r
apparent power is
S = P 2 + Q 2 = 519 V A S=\sqrt{P^2+Q^2}=519 VA S = P 2 + Q 2 = 519 V A
The power factor is P S = 379 519 = 0.73 \frac{P}{S}=\frac{379}{519}=0.73 S P = 519 379 = 0.73 or 73 73% 73 %
(c) The average power consumed by the circuit is equals P = 378.7 W P=378.7W P = 378.7 W as the reactive power isn't consumed.
Answers: (a) The current is i ( t ) = 4.72 ⋅ s i n ( 314 t + 0.753 ) A i(t)=4.72\cdot sin(314t+0.753)A i ( t ) = 4.72 ⋅ s in ( 314 t + 0.753 ) A
(b) The power factor of the circuit is 73%
(c) The average power consumed by the circuit is 379 W
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