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Question: In the given circuit diagram, a wire is joining points B and D. The current in this wire is:...

In the given circuit diagram, a wire is joining points B and D. The current in this wire is:

A

0.4A

B

2A

C

4A

D

zero

Answer

2A

Explanation

Solution

The given circuit is a Wheatstone bridge with a 20V battery connected across points A and C, and a wire connecting points B and D. The resistances are RAB=1ΩR_{AB} = 1\Omega, RBC=2ΩR_{BC} = 2\Omega, RAD=4ΩR_{AD} = 4\Omega, and RDC=3ΩR_{DC} = 3\Omega. We need to find the current in the wire joining B and D.

Let VAV_A, VBV_B, VCV_C, and VDV_D be the potentials at points A, B, C, and D respectively. Let's set VC=0VV_C = 0V and VA=20VV_A = 20V since the battery is connected between A and C with the positive terminal at A.

Let IBDI_{BD} be the current flowing from B to D through the wire. We can use nodal analysis at points B and D.

At node B, by Kirchhoff's current law: Current entering B = Current leaving B IAB=IBC+IBDI_{AB} = I_{BC} + I_{BD} VAVBRAB=VBVCRBC+IBD\frac{V_A - V_B}{R_{AB}} = \frac{V_B - V_C}{R_{BC}} + I_{BD} 20VB1=VB02+IBD\frac{20 - V_B}{1} = \frac{V_B - 0}{2} + I_{BD} 2(20VB)=VB+2IBD2(20 - V_B) = V_B + 2 I_{BD} 402VB=VB+2IBD40 - 2V_B = V_B + 2 I_{BD} 40=3VB+2IBD40 = 3V_B + 2 I_{BD} (Equation 1)

At node D, by Kirchhoff's current law: Current entering D = Current leaving D IAD+IBD=IDCI_{AD} + I_{BD} = I_{DC} VAVDRAD+IBD=VDVCRDC\frac{V_A - V_D}{R_{AD}} + I_{BD} = \frac{V_D - V_C}{R_{DC}} 20VD4+IBD=VD03\frac{20 - V_D}{4} + I_{BD} = \frac{V_D - 0}{3} 3(20VD)+12IBD=4VD3(20 - V_D) + 12 I_{BD} = 4V_D 603VD+12IBD=4VD60 - 3V_D + 12 I_{BD} = 4V_D 60=7VD12IBD60 = 7V_D - 12 I_{BD} (Equation 2)

The problem statement does not specify the resistance of the wire joining B and D. In such problems, it is usually assumed that the wire is ideal, meaning it has zero resistance. If the wire has zero resistance, then points B and D are at the same potential, i.e., VB=VDV_B = V_D. Let VB=VD=VV_B = V_D = V.

Substituting VB=VV_B = V and VD=VV_D = V into Equations 1 and 2: 40=3V+2IBD40 = 3V + 2 I_{BD} (Equation 3) 60=7V12IBD60 = 7V - 12 I_{BD} (Equation 4)

We have a system of two linear equations with two unknowns, VV and IBDI_{BD}. We can solve for IBDI_{BD}. Multiply Equation 3 by 7 and Equation 4 by 3: 7×(40=3V+2IBD)    280=21V+14IBD7 \times (40 = 3V + 2 I_{BD}) \implies 280 = 21V + 14 I_{BD} 3×(60=7V12IBD)    180=21V36IBD3 \times (60 = 7V - 12 I_{BD}) \implies 180 = 21V - 36 I_{BD}

Subtract the second new equation from the first new equation: (280)(180)=(21V+14IBD)(21V36IBD)(280) - (180) = (21V + 14 I_{BD}) - (21V - 36 I_{BD}) 100=14IBD+36IBD100 = 14 I_{BD} + 36 I_{BD} 100=50IBD100 = 50 I_{BD} IBD=10050=2AI_{BD} = \frac{100}{50} = 2A

The current in the wire joining B and D is 2A. Since we assumed the current flows from B to D and got a positive value, the direction of the current is from B to D.

We can also find the potential VV: From Equation 3: 40=3V+2(2)    40=3V+4    3V=36    V=12V40 = 3V + 2(2) \implies 40 = 3V + 4 \implies 3V = 36 \implies V = 12V. So, VB=VD=12VV_B = V_D = 12V.