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Question: Find the current through the 10 $\Omega$ resistor shown in figure ...

Find the current through the 10 Ω\Omega resistor shown in figure

A

zero

B

1A

C

2A

D

5A

Answer

zero

Explanation

Solution

To find the current through the 10 Ω resistor, we will use Nodal Analysis.

1. Define Nodes and Potentials: Let's label the nodes in the circuit.

  • Let the bottom wire be the reference node (ground), so its potential VA=0VV_A = 0V.
  • The 4.5V battery is connected between node A and node B, with the positive terminal at B. Therefore, VB=VA+4.5V=0V+4.5V=4.5VV_B = V_A + 4.5V = 0V + 4.5V = 4.5V.
  • The 3V battery is connected between node A and node E, with the positive terminal at E. Therefore, VE=VA+3V=0V+3V=3VV_E = V_A + 3V = 0V + 3V = 3V.
  • Let VCV_C be the potential at node C (between 3Ω, 6Ω, and 10Ω resistors).
  • Let VDV_D be the potential at node D (between 10Ω and 1Ω resistors).

2. Apply Kirchhoff's Current Law (KCL) at Nodes C and D: KCL states that the sum of currents leaving a node is zero.

At Node C: Currents leaving node C flow through the 3Ω, 6Ω, and 10Ω resistors.

  • Current through 3Ω resistor (to B): ICB=VCVB3=VC4.53I_{CB} = \frac{V_C - V_B}{3} = \frac{V_C - 4.5}{3}
  • Current through 6Ω resistor (to A): ICA=VCVA6=VC06=VC6I_{CA} = \frac{V_C - V_A}{6} = \frac{V_C - 0}{6} = \frac{V_C}{6}
  • Current through 10Ω resistor (to D): ICD=VCVD10I_{CD} = \frac{V_C - V_D}{10}

Sum of currents leaving node C = 0: VC4.53+VC6+VCVD10=0\frac{V_C - 4.5}{3} + \frac{V_C}{6} + \frac{V_C - V_D}{10} = 0

To eliminate denominators, multiply the entire equation by the least common multiple of 3, 6, and 10, which is 30: 10(VC4.5)+5(VC)+3(VCVD)=010(V_C - 4.5) + 5(V_C) + 3(V_C - V_D) = 0 10VC45+5VC+3VC3VD=010V_C - 45 + 5V_C + 3V_C - 3V_D = 0 18VC3VD=45(Equation 1)18V_C - 3V_D = 45 \quad \text{(Equation 1)}

At Node D: Currents leaving node D flow through the 10Ω and 1Ω resistors.

  • Current through 10Ω resistor (to C): IDC=VDVC10I_{DC} = \frac{V_D - V_C}{10}
  • Current through 1Ω resistor (to E): IDE=VDVE1=VD31I_{DE} = \frac{V_D - V_E}{1} = \frac{V_D - 3}{1}

Sum of currents leaving node D = 0: VDVC10+VD31=0\frac{V_D - V_C}{10} + \frac{V_D - 3}{1} = 0

To eliminate denominators, multiply the entire equation by 10: (VDVC)+10(VD3)=0(V_D - V_C) + 10(V_D - 3) = 0 VDVC+10VD30=0V_D - V_C + 10V_D - 30 = 0 VC+11VD=30(Equation 2)-V_C + 11V_D = 30 \quad \text{(Equation 2)}

3. Solve the System of Equations: We have two linear equations with two unknowns (VCV_C and VDV_D):

  1. 18VC3VD=4518V_C - 3V_D = 45
  2. VC+11VD=30-V_C + 11V_D = 30

From Equation 2, express VCV_C in terms of VDV_D: VC=11VD30V_C = 11V_D - 30

Substitute this expression for VCV_C into Equation 1: 18(11VD30)3VD=4518(11V_D - 30) - 3V_D = 45 198VD5403VD=45198V_D - 540 - 3V_D = 45 195VD=45+540195V_D = 45 + 540 195VD=585195V_D = 585 VD=585195V_D = \frac{585}{195} VD=3VV_D = 3V

Now, substitute the value of VDV_D back into the expression for VCV_C: VC=11(3)30V_C = 11(3) - 30 VC=3330V_C = 33 - 30 VC=3VV_C = 3V

4. Calculate the Current through the 10 Ω Resistor: The current through the 10 Ω resistor is given by Ohm's Law: I10Ω=VCVD10I_{10\Omega} = \frac{V_C - V_D}{10}. I10Ω=3V3V10I_{10\Omega} = \frac{3V - 3V}{10} I10Ω=010I_{10\Omega} = \frac{0}{10} I10Ω=0AI_{10\Omega} = 0A

The current through the 10 Ω resistor is zero.