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Question: Unbalanced wheatstone bridge. ① find $R_{eq}$ of circuit ② Current passes through battery ③ $V_c - ...

Unbalanced wheatstone bridge.

① find ReqR_{eq} of circuit ② Current passes through battery ③ VcVDV_c - V_D ④ current through 3Ω\Omega

Answer
  1. Req=139ΩR_{eq} = \frac{13}{9} \Omega
  2. Current passes through battery = 9013 A\frac{90}{13} \text{ A}
  3. VCVD=3013 VV_C - V_D = -\frac{30}{13} \text{ V}
  4. Current through 3Ω = 1013 A\frac{10}{13} \text{ A} (from D to C)
Explanation

Solution

The circuit given is an unbalanced Wheatstone bridge. We will use Kirchhoff's laws to find the potentials at nodes C and D, and then calculate the required quantities.

Let the potential at the positive terminal of the battery be VP=10VV_P = 10V and at the negative terminal be VQ=0VV_Q = 0V. The resistors are connected as follows:

  • RPC=2ΩR_{PC} = 2\Omega
  • RCQ=1ΩR_{CQ} = 1\Omega
  • RPD=1ΩR_{PD} = 1\Omega
  • RDQ=2ΩR_{DQ} = 2\Omega
  • RCD=3ΩR_{CD} = 3\Omega

Let VCV_C and VDV_D be the potentials at points C and D, respectively.

1. Apply Kirchhoff's Current Law (KCL) at nodes C and D:

  • At node C: Current entering C from P equals current leaving C towards D and Q. VPVCRPC=VCVDRCD+VCVQRCQ\frac{V_P - V_C}{R_{PC}} = \frac{V_C - V_D}{R_{CD}} + \frac{V_C - V_Q}{R_{CQ}} 10VC2=VCVD3+VC01\frac{10 - V_C}{2} = \frac{V_C - V_D}{3} + \frac{V_C - 0}{1} Multiply by 6 to clear denominators: 3(10VC)=2(VCVD)+6VC3(10 - V_C) = 2(V_C - V_D) + 6V_C 303VC=2VC2VD+6VC30 - 3V_C = 2V_C - 2V_D + 6V_C 30=11VC2VD30 = 11V_C - 2V_D (Equation 1)

  • At node D: Current entering D from P and C equals current leaving D towards Q. VPVDRPD+VCVDRCD=VDVQRDQ\frac{V_P - V_D}{R_{PD}} + \frac{V_C - V_D}{R_{CD}} = \frac{V_D - V_Q}{R_{DQ}} 10VD1+VCVD3=VD02\frac{10 - V_D}{1} + \frac{V_C - V_D}{3} = \frac{V_D - 0}{2} Multiply by 6 to clear denominators: 6(10VD)+2(VCVD)=3VD6(10 - V_D) + 2(V_C - V_D) = 3V_D 606VD+2VC2VD=3VD60 - 6V_D + 2V_C - 2V_D = 3V_D 60+2VC8VD=3VD60 + 2V_C - 8V_D = 3V_D 2VC11VD=602V_C - 11V_D = -60 (Equation 2)

2. Solve the system of linear equations for VCV_C and VDV_D: Equation 1: 11VC2VD=3011V_C - 2V_D = 30 Equation 2: 2VC11VD=602V_C - 11V_D = -60

Multiply Equation 1 by 11 and Equation 2 by 2: 121VC22VD=330121V_C - 22V_D = 330 4VC22VD=1204V_C - 22V_D = -120

Subtract the second modified equation from the first: (121VC4VC)(22VD22VD)=330(120)(121V_C - 4V_C) - (22V_D - 22V_D) = 330 - (-120) 117VC=450117V_C = 450 VC=450117=15039=5013 VV_C = \frac{450}{117} = \frac{150}{39} = \frac{50}{13} \text{ V}

Substitute VCV_C back into Equation 1: 11(5013)2VD=3011\left(\frac{50}{13}\right) - 2V_D = 30 550132VD=30\frac{550}{13} - 2V_D = 30 2VD=5501330=55039013=160132V_D = \frac{550}{13} - 30 = \frac{550 - 390}{13} = \frac{160}{13} VD=8013 VV_D = \frac{80}{13} \text{ V}

Now, let's answer the specific questions:

③ Find VCVDV_C - V_D VCVD=50138013=3013 VV_C - V_D = \frac{50}{13} - \frac{80}{13} = -\frac{30}{13} \text{ V}

④ Current through 3Ω resistor Current ICD=VCVDRCD=30/133=1013 AI_{CD} = \frac{V_C - V_D}{R_{CD}} = \frac{-30/13}{3} = -\frac{10}{13} \text{ A} The negative sign indicates that the current flows from D to C. The magnitude of the current through the 3Ω resistor is 1013 A\frac{10}{13} \text{ A}.

② Current passes through battery The total current from the battery is the sum of currents entering nodes C and D from P. Current IPC=VPVCRPC=1050/132=(13050)/132=80/132=4013 AI_{PC} = \frac{V_P - V_C}{R_{PC}} = \frac{10 - 50/13}{2} = \frac{(130 - 50)/13}{2} = \frac{80/13}{2} = \frac{40}{13} \text{ A} Current IPD=VPVDRPD=1080/131=(13080)/131=5013 AI_{PD} = \frac{V_P - V_D}{R_{PD}} = \frac{10 - 80/13}{1} = \frac{(130 - 80)/13}{1} = \frac{50}{13} \text{ A} Total current from battery Ibattery=IPC+IPD=4013+5013=9013 AI_{battery} = I_{PC} + I_{PD} = \frac{40}{13} + \frac{50}{13} = \frac{90}{13} \text{ A}

① Find ReqR_{eq} of circuit The equivalent resistance is the total voltage divided by the total current. Req=VbatteryIbattery=1090/13=10×1390=13090=139ΩR_{eq} = \frac{V_{battery}}{I_{battery}} = \frac{10}{90/13} = 10 \times \frac{13}{90} = \frac{130}{90} = \frac{13}{9} \Omega