D.C. Circuits: Question 9

Syllabus 10.1, 10.2

Structured AS 10 marks

Two batteries, each of negligible internal resistance, are connected to a common resistor at a junction PP, forming a two-loop network.

  • A battery of e.m.f. 18 V18\text{ V} is connected to PP through a resistor of resistance 2.0 Ω2.0\ \Omega, carrying current I1I_1 towards PP.
  • A battery of e.m.f. 16 V16\text{ V} is connected to PP through a resistor of resistance 4.0 Ω4.0\ \Omega, carrying current I2I_2 towards PP.
  • From PP, a single resistor of resistance 3.0 Ω3.0\ \Omega carries current I3I_3 away from PP and back to the negative terminals of both batteries, which are joined together.

(a) State Kirchhoff's first law, and use it to write an equation relating I1I_1, I2I_2 and I3I_3 at junction PP. [2]

(b) Use Kirchhoff's second law to write one equation for the loop containing the 18 V18\text{ V} battery and the 3.0 Ω3.0\ \Omega resistor, and a second equation for the loop containing the 16 V16\text{ V} battery and the 3.0 Ω3.0\ \Omega resistor. [2]

(c) Solve your three equations from (a) and (b) simultaneously to find I1I_1, I2I_2 and I3I_3. [5]

(d) Calculate the potential difference across the 3.0 Ω3.0\ \Omega resistor. [1]

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Worked solution

Part (a): Kirchhoff’s first law at junction PP

Kirchhoff’s first law is a consequence of the conservation of charge: the total current flowing into a junction must equal the total current flowing out of it. At PP, currents I1I_1 and I2I_2 flow in and current I3I_3 flows out, so: I1+I2=I3I_1 + I_2 = I_3

Part (b): Kirchhoff’s second law for each loop

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. In both loops, current I3I_3 passes through the shared 3.0 Ω3.0\ \Omega resistor.

Loop containing the 18 V18\text{ V} battery: 18=I1(2.0)+I3(3.0)18 = I_1(2.0) + I_3(3.0)

Loop containing the 16 V16\text{ V} battery: 16=I2(4.0)+I3(3.0)16 = I_2(4.0) + I_3(3.0)

Part (c): Solving the three equations simultaneously

Rearranging the two loop equations for I1I_1 and I2I_2: I1=183.0I32.0=9.01.5I3...(1)I_1 = \frac{18-3.0I_3}{2.0} = 9.0 - 1.5I_3 \quad \text{...(1)} I2=163.0I34.0=4.00.75I3...(2)I_2 = \frac{16-3.0I_3}{4.0} = 4.0 - 0.75I_3 \quad \text{...(2)}

Substituting (1) and (2) into the junction equation I1+I2=I3I_1+I_2=I_3: (9.01.5I3)+(4.00.75I3)=I3(9.0-1.5I_3) + (4.0-0.75I_3) = I_3 13.02.25I3=I313.0 - 2.25I_3 = I_3 13.0=3.25I313.0 = 3.25I_3 I3=13.03.25=4.0 AI_3 = \frac{13.0}{3.25} = 4.0\text{ A}

Substituting back into (1) and (2): I1=9.01.5(4.0)=9.06.0=3.0 AI_1 = 9.0 - 1.5(4.0) = 9.0-6.0 = 3.0\text{ A} I2=4.00.75(4.0)=4.03.0=1.0 AI_2 = 4.0 - 0.75(4.0) = 4.0-3.0 = 1.0\text{ A}

Check using the junction equation: I1+I2=3.0+1.0=4.0 A=I3I_1+I_2=3.0+1.0=4.0\text{ A}=I_3. Confirmed.

Check by substituting back into the original loop equations:

  • 18 V18\text{ V} loop: 2.0(3.0)+3.0(4.0)=6.0+12.0=18.0 V2.0(3.0)+3.0(4.0)=6.0+12.0=18.0\text{ V} ✓ matches the e.m.f.
  • 16 V16\text{ V} loop: 4.0(1.0)+3.0(4.0)=4.0+12.0=16.0 V4.0(1.0)+3.0(4.0)=4.0+12.0=16.0\text{ V} ✓ matches the e.m.f.

Both loop equations and the junction equation are satisfied, confirming I1=3.0 AI_1=3.0\text{ A}, I2=1.0 AI_2=1.0\text{ A}, I3=4.0 AI_3=4.0\text{ A}.

Part (d): Potential difference across the 3.0 Ω3.0\ \Omega resistor

V3.0Ω=I3×3.0=4.0×3.0=12 VV_{3.0\Omega} = I_3 \times 3.0 = 4.0\times3.0 = 12\text{ V}

Check using either loop: from the 18 V18\text{ V} loop, the p.d. across the 2.0 Ω2.0\ \Omega resistor is I1×2.0=3.0×2.0=6.0 VI_1\times2.0=3.0\times2.0=6.0\text{ V}, and 6.0+12.0=18.0 V6.0+12.0=18.0\text{ V}, matching the 18 V18\text{ V} e.m.f. Confirmed.

Final answers

  • (a) I1+I2=I3I_1+I_2=\boxed{I_3}
  • (b) 18=2.0I1+3.0I318=2.0I_1+3.0I_3; 16=4.0I2+3.0I316=4.0I_2+3.0I_3
  • (c) I1=3.0 AI_1=\boxed{3.0}\text{ A}, I2=1.0 AI_2=\boxed{1.0}\text{ A}, I3=4.0 AI_3=\boxed{4.0}\text{ A}
  • (d) P.d. across 3.0 Ω3.0\ \Omega resistor =12 V=\boxed{12}\text{ V}