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Battery charger bridge 15 V: currents, power, efficiency

Short answer

For the 15 V rms bridge charging a 12 V battery through 2 ohm, conduction occurs only when rectified voltage exceeds 12 V. Average charging current is 1.865 A, rms current 2.613 A, battery power 22.38 W, rectifier output 36.03 W. Charging efficiency is 62.1%.

Figure shows a full wave rectifier circuit used to charge a 12V battery through a 2 ohm resistor. (i) Draw the waveform of output voltage V0 and charging current i0. (ii) Calculate the average and rms value of charging current. (iii) Power supplied to the battery. (iv) Power output from the rectifier. (v) Efficiency of the charging system. [Figure: single-phase diode bridge (four diodes) fed from Vs = 15 V (rms), f = 50 Hz; output Vo feeds R = 2 Ω in series with a battery Eb = 12 V; charging current io]

Given: single-phase diode bridge, Vs=15V_s = 15 V rms, 50 Hz; R=2 ΩR = 2\ \Omega; battery E=12E = 12 V.

(i) Waveforms

In a diode rectifier charging a battery of emf EE through resistance RR, a diode pair conducts only when the instantaneous supply voltage exceeds EE.

 v  ^      .--.          .--.
    |    .'    '.      .'    '.  vs (rectified)
  E |---+--------+----+--------+--- battery emf
    |  /|        |\  /|        |
    | / |  io    | \/ |        |
 ---+---+--------+----+--------+--> wt
       t1     pi-t1  pi+t1
 io  ^   .--.          .--.
     |  /    \        /    \
 ----+-+------+------+------+--> wt

Conduction starts at θ1=sin⁡−1(E/Vm)\theta_1 = \sin^{-1}(E/V_m) and ends at π−θ1\pi - \theta_1 in every half cycle. During conduction io=Vmsin⁡ωt−ERi_o = \frac{V_m\sin\omega t - E}{R}.

Iavg=1πR[2Vmcos⁡θ1−E(π−2θ1)]Irms2=1πR2[(Vm22+E2)(π−2θ1)+Vm22sin⁡2θ1−4VmEcos⁡θ1]\begin{aligned} I_{avg} &= \frac{1}{\pi R}\left[2V_m\cos\theta_1 - E(\pi - 2\theta_1)\right] \\ I_{rms}^2 &= \frac{1}{\pi R^2}\left[\left(\frac{V_m^2}{2} + E^2\right)(\pi - 2\theta_1) + \frac{V_m^2}{2}\sin 2\theta_1 - 4V_mE\cos\theta_1\right] \end{aligned}

Power to the battery =EIavg= E I_{avg}; loss in the resistor =Irms2R= I_{rms}^2 R; rectifier output =EIavg+Irms2R= E I_{avg} + I_{rms}^2 R.

(ii) Average and rms charging current

Vm=2×15=21.21 Vθ1=sin⁡−11221.21=34.45∘=0.6013 rad,π−2θ1=1.9391 radIavg=12π[2×21.21×0.8246−12×1.9391]=34.99−23.276.283=1.865 A\begin{aligned} V_m &= \sqrt{2} \times 15 = 21.21\ \text{V} \\ \theta_1 &= \sin^{-1}\frac{12}{21.21} = 34.45^\circ = 0.6013\ \text{rad}, \qquad \pi - 2\theta_1 = 1.9391\ \text{rad} \\ I_{avg} &= \frac{1}{2\pi}\left[2 \times 21.21 \times 0.8246 - 12 \times 1.9391\right] = \frac{34.99 - 23.27}{6.283} = 1.865\ \text{A} \end{aligned}

With sin⁡2θ1=0.9330\sin 2\theta_1 = 0.9330:

Irms2=14π[(225+144)(1.9391)+225(0.9330)−4(21.21)(12)(0.8246)]=6.826I_{rms}^2 = \frac{1}{4\pi}\left[(225 + 144)(1.9391) + 225(0.9330) - 4(21.21)(12)(0.8246)\right] = 6.826 Irms=2.613 AI_{rms} = 2.613\ \text{A}

(iii) Power supplied to the battery

Pb=EIavg=12×1.865=22.38 WP_b = E I_{avg} = 12 \times 1.865 = 22.38\ \text{W}

(iv) Power output of the rectifier

Po=Pb+Irms2R=22.38+2.6132×2=22.38+13.65=36.03 WP_o = P_b + I_{rms}^2 R = 22.38 + 2.613^2 \times 2 = 22.38 + 13.65 = 36.03\ \text{W}

(v) Efficiency of charging

η=PbPo=22.3836.03=62.1%\eta = \frac{P_b}{P_o} = \frac{22.38}{36.03} = 62.1\%

Answer: Iavg=1.865I_{avg} = 1.865 A, Irms=2.613I_{rms} = 2.613 A, Pb=22.38P_b = 22.38 W, Po=36.03P_o = 36.03 W, η=62.1%\eta = 62.1\%.

✓ Answer checked by Claude Opus 5.5 (high effort)

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