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Q.Find the equivalent resistance between points A and B for the network shown in the figure.

Figure — 55/6/1 Q17
Figure
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Figure — 55/6/1 Q17
Figure — 55/6/1 Q17

The real network (see figure) is a 5-node bridge -- A through a 1 Ω1\,\Omega resistor to node P, then P branches into a bridge of nodes T (top), Ctr (centre), and Bot (bottom) before rejoining at node Q, which connects to B by a plain wire. Because node Ctr connects to four different nodes (P, T, Bot, and Q), this network does not reduce by simple series-parallel combination -- it must be solved with Kirchhoff's laws (the node-voltage / junction-rule method). Doing so gives RAB=6517667 Ω≈9.77 ΩR_{AB}=\dfrac{6517}{667}\,\Omega\approx 9.77\,\Omega.

Why this needs Kirchhoff's laws, not series-parallel shortcuts

Reading the figure: A connects to P through 1 Ω1\,\Omega. From P, three resistors fan out to T (5 Ω5\,\Omega), to Ctr (25 Ω25\,\Omega), and to Bot (15 Ω15\,\Omega). T and Bot each also connect to Ctr (5 Ω5\,\Omega and 10 Ω10\,\Omega respectively) and to Q (10 Ω10\,\Omega and 30 Ω30\,\Omega respectively, the two diagonal resistors). Ctr also connects directly to Q (20 Ω20\,\Omega). Finally Q connects to B by a plain wire (so Q and B are the same node electrically).

No two of these nine resistors share both their end-nodes with each other in a simple loop -- every node except A and B touches at least three resistors -- so there is no legal series or parallel combination anywhere in the T/Ctr/Bot/Q cluster. This is the hallmark of a genuine bridge network, and the textbook-correct tool for it is Kirchhoff's junction rule applied at every internal node (equivalently, the node-voltage method).

Setting up the node equations

Since Q and B are the same node, set VQ=VB=0V_Q=V_B=0 (reference) and inject a test current II at A. All of II passes through the 1 Ω1\,\Omega resistor into P, so VP=VA−I(1)V_P = V_A - I(1), and RAB=VA−VBI=1+VPIR_{AB}=\dfrac{V_A-V_B}{I}=1+\dfrac{V_P}{I} (taking I=1I=1 for convenience, since the network beyond P is linear).

Applying ∑Iout=0\sum I_{\text{out}}=0 at each of the three internal nodes (T, Ctr, Bot), with VP=x1V_P=x_1 unknown for now:

Node T: VT−VP5+VT−VCtr5+VT10=0\dfrac{V_T-V_P}{5}+\dfrac{V_T-V_{Ctr}}{5}+\dfrac{V_T}{10}=0

Node Ctr: VCtr−VP25+VCtr−VT5+VCtr−VBot10+VCtr20=0\dfrac{V_{Ctr}-V_P}{25}+\dfrac{V_{Ctr}-V_T}{5}+\dfrac{V_{Ctr}-V_{Bot}}{10}+\dfrac{V_{Ctr}}{20}=0

Node Bot: VBot−VP15+VBot−VCtr10+VBot30=0\dfrac{V_{Bot}-V_P}{15}+\dfrac{V_{Bot}-V_{Ctr}}{10}+\dfrac{V_{Bot}}{30}=0

Solving the first and third equations for VTV_T and VBotV_{Bot} in terms of VPV_P and VCtrV_{Ctr}, then substituting into the middle equation, gives (with VP=1V_P=1 for a unit test voltage there): …

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