D.C. Circuits: Question 3

Syllabus 10.1, 10.2

Structured AS 10 marks

A battery has e.m.f. 9.0 V9.0\text{ V} and internal resistance 0.50 Ω0.50\ \Omega. It is connected to a single external resistor of resistance 4.0 Ω4.0\ \Omega.

(a) Write down Kirchhoff's second law for this circuit, and use it to calculate the current II in the circuit. [3]

(b) Calculate the terminal potential difference of the battery. [2]

(c) Calculate the potential difference across the internal resistance (the "lost volts"). [2]

(d) Calculate the power dissipated in the internal resistance, and hence determine the efficiency of the transfer of energy from the battery to the external resistor. [3]

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Worked solution

Part (a): Kirchhoff’s second law and the current

Kirchhoff’s second law states that, around any complete loop, the sum of the e.m.f.s equals the sum of the potential drops (a consequence of conservation of energy). Going around this single-loop circuit: E=IR+Ir=I(R+r)E = IR + Ir = I(R+r)

Rearranging for II and substituting E=9.0 VE=9.0\text{ V}, R=4.0 ΩR=4.0\ \Omega, r=0.50 Ωr=0.50\ \Omega: I=ER+r=9.04.0+0.50=9.04.5=2.0 AI = \frac{E}{R+r} = \frac{9.0}{4.0+0.50} = \frac{9.0}{4.5} = 2.0\text{ A}

Check: 4.5×2.0=9.0 V4.5\times2.0=9.0\text{ V}, which matches EE. Confirmed.

Part (b): Terminal potential difference

The terminal p.d. is the potential difference actually available across the battery’s terminals, the p.d. across the external resistor RR: Vterminal=IR=2.0×4.0=8.0 VV_{\text{terminal}} = IR = 2.0\times4.0 = 8.0\text{ V}

Check by an independent route: the terminal p.d. also equals EIr=9.0(2.0×0.50)=9.01.0=8.0 VE-Ir=9.0-(2.0\times0.50)=9.0-1.0=8.0\text{ V}. Both routes agree.

Part (c): Potential difference across the internal resistance (lost volts)

The “lost volts” is the potential difference across the internal resistance itself: Vlost=Ir=2.0×0.50=1.0 VV_{\text{lost}} = Ir = 2.0\times0.50 = 1.0\text{ V}

Check: the terminal p.d. and the lost volts should add up to the e.m.f.: 8.0+1.0=9.0 V=E8.0+1.0=9.0\text{ V}=E. Confirmed.

Part (d): Power dissipated in rr and efficiency

The power dissipated in the internal resistance is: Pr=I2r=(2.0)2×0.50=4.0×0.50=2.0 WP_r = I^2r = (2.0)^2\times0.50 = 4.0\times0.50 = 2.0\text{ W}

The total power supplied by the battery is: Ptotal=EI=9.0×2.0=18.0 WP_{\text{total}} = EI = 9.0\times2.0 = 18.0\text{ W}

Check using the external resistor: the useful power delivered to RR is PR=I2R=(2.0)2×4.0=16.0 WP_R=I^2R=(2.0)^2\times4.0=16.0\text{ W}, and PR+Pr=16.0+2.0=18.0 W=PtotalP_R+P_r=16.0+2.0=18.0\text{ W}=P_{\text{total}}. Confirmed. Energy is conserved between the two resistances.

The efficiency of the energy transfer to the external resistor is the ratio of useful power output to total power supplied: efficiency=PRPtotal=16.018.0=0.8889\text{efficiency} = \frac{P_R}{P_{\text{total}}} = \frac{16.0}{18.0} = 0.8889

Check as a fraction: 16.018.0=89=0.8889\frac{16.0}{18.0}=\frac{8}{9}=0.8889, the same value. So the efficiency is 88.9%\boxed{88.9}\% (3 s.f.).

Final answers

  • (a) E=I(R+r)E=I(R+r), giving I=2.0 AI=\boxed{2.0}\text{ A}
  • (b) Terminal p.d. =8.0 V=\boxed{8.0}\text{ V}
  • (c) Lost volts =1.0 V=\boxed{1.0}\text{ V}
  • (d) Power dissipated in r=2.0 Wr=\boxed{2.0}\text{ W}; efficiency =88.9%=\boxed{88.9}\%