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Battery charger bridge 30 V: conduction, power

Short answer

Conduction period per half cycle is 111.10° (6.17 ms) from 34.45° to 145.55°. Average charging current I_o = 1.492 A. Power to battery is 35.80 W; gross rectifier output power is 57.65 W.

Below figure shows a full-wave diode rectifier circuit used to charge a 24V battery through a 5 ohm resistor. Calculate: (i) Conduction period of charging current io. (ii) Average value of charging current io (iii) Power supplied to the battery and gross power output from the rectifier [Figure: single-phase diode bridge (D1, D3 top; D4, D2 bottom) fed from Vs = 30 V (rms); output Vo feeds R = 5 Ω in series with a battery Eb = 24 V; charging current io]

In a battery-charging rectifier, a diode conducts only when the instantaneous supply voltage exceeds the battery emf EE. In each half cycle current flows from α\alpha to π−α\pi-\alpha, where Vmsin⁡α=EV_m\sin\alpha = E, and is limited by RR:

io=Vmsin⁡ωt−ER,α<ωt<π−αi_o = \frac{V_m\sin\omega t - E}{R}, \qquad \alpha < \omega t < \pi - \alpha
     io     R
 P o--->---/\/\/---+
                   |
                 + |
                 ===  Eb (battery)
                 - |
 N o---------------+
 (P, N = output of the diode bridge)

Data: Vs=30V_s = 30 V (rms), Eb=24E_b = 24 V, R=5 ΩR = 5\ \Omega, ideal diodes. D1, D2 conduct in the positive half cycle and D3, D4 in the negative half cycle, but only while ∣vs∣>24|v_s| > 24 V.

 |vs|   ___         ___
       / | \       / | \       --- 24 V level
 -----/--+--\-----/--+--\----
 io      /\          /\
 -------/  \--------/  \-----
      a  180-a  180+a  360-a

i) Conduction period

Vm=2×30=42.43 Vα=sin⁡−1EVm=sin⁡−12442.43=34.45∘=0.6013 rad\begin{aligned} V_m &= \sqrt2 \times 30 = 42.43\ \text{V} \\ \alpha &= \sin^{-1}\frac{E}{V_m} = \sin^{-1}\frac{24}{42.43} = 34.45^\circ = 0.6013\ \text{rad} \end{aligned} θc=π−2α=180∘−2(34.45∘)=111.10∘=1.9391 radtc=111.10∘360∘×20 ms=6.17 ms (in each half cycle)\begin{aligned} \theta_c &= \pi - 2\alpha = 180^\circ - 2(34.45^\circ) = 111.10^\circ = 1.9391\ \text{rad} \\ t_c &= \frac{111.10^\circ}{360^\circ} \times 20\ \text{ms} = 6.17\ \text{ms (in each half cycle)} \end{aligned}

ii) Average charging current

Io=1π∫απ−αVmsin⁡ωt−ER d(ωt)=1πR[2Vmcos⁡α−E(π−2α)]=1π×5[2(42.43)(0.8246)−24(1.9391)]=69.971−46.53815.7080=1.492 A\begin{aligned} I_o &= \frac{1}{\pi}\int_{\alpha}^{\pi-\alpha}\frac{V_m\sin\omega t - E}{R}\,d(\omega t) = \frac{1}{\pi R}\left[2V_m\cos\alpha - E(\pi-2\alpha)\right] \\ &= \frac{1}{\pi \times 5}\left[2(42.43)(0.8246) - 24(1.9391)\right] = \frac{69.971 - 46.538}{15.7080} = 1.492\ \text{A} \end{aligned}

iii) Power to battery and gross power output

Irms2=1πR2[(Vm22+E2)(π−2α)+Vm22sin⁡2α−4VmEcos⁡α]=2862.06+839.66−3358.6378.540=4.368Irms=2.090 A\begin{aligned} I_{rms}^2 &= \frac{1}{\pi R^2}\left[\left(\frac{V_m^2}{2}+E^2\right)(\pi-2\alpha) + \frac{V_m^2}{2}\sin2\alpha - 4V_mE\cos\alpha\right] \\ &= \frac{2862.06 + 839.66 - 3358.63}{78.540} = 4.368 \\ I_{rms} &= 2.090\ \text{A} \end{aligned} Pbatt=E Io=24×1.492=35.80 WPR=Irms2R=4.368×5=21.84 WPgross=Pbatt+PR=35.80+21.84=57.65 W\begin{aligned} P_{batt} &= E\,I_o = 24 \times 1.492 = 35.80\ \text{W} \\ P_R &= I_{rms}^2R = 4.368 \times 5 = 21.84\ \text{W} \\ P_{gross} &= P_{batt} + P_R = 35.80 + 21.84 = 57.65\ \text{W} \end{aligned}

Answer: (i) conduction 111.10° (6.17 ms) per half cycle, from 34.45° to 145.55°; (ii) Io=1.492I_o = 1.492 A; (iii) Pbatt=35.80P_{batt} = 35.80 W, gross output =57.65= 57.65 W.

✓ Answer checked by Claude Opus 5.5 (high effort)

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