Unit 02: Current Electricity • Chapter 03
Kirchhoff's Rules & The Wheatstone Bridge
Conservation laws in multi-loop networks, sign conventions, bridge balance derivation, and galvanometer deflection dynamics.
Socho ek busy road intersection ko: jitni gaadiyan junction par enter karti hain, utni hi bahar nikalni padti hain—koi gaadi hawa me gayab nahi ho sakti (Kirchhoff's Junction Rule / Conservation of Charge). Aur agar aap kisi amusement park ke roller coaster track par ek complete round lagakar wapas apni starting seat par aate hain, toh pure ride ke dauran total gain in altitude aur drop in altitude ka net sum zero hota hai (Kirchhoff's Loop Rule / Conservation of Energy). Jab inhi do rules ko ek diamond network me apply karte hain aur opposite sides ka potential drop equal ho jata hai, toh central bridge branch me current zero ho jata hai—isi ko Balanced Wheatstone Bridge kehte hain!
1. Kirchhoff's First & Second Laws (KCL & KVL)
Junction rule and closed loop potential summation:
Physical origin: KCL is based on Conservation of Charge; KVL is based on Conservation of Energy.
2. Wheatstone Bridge Condition
Null deflection condition in the galvanometer branch ($I_g = 0$):
Where $P, Q, R, S$ are the four resistance arms. When balanced, the bridge has maximum sensitivity when all four resistors are of equal order of magnitude.
Deduction of Wheatstone Bridge Balancing Condition Using Kirchhoff's Laws
1. Consider four resistors $P, Q, R, S$ forming closed loop $ABDA$ and $BCDB$. Battery of EMF $\mathcal{E}$ is connected between $A$ and $C$, and galvanometer of resistance $G$ is connected between $B$ and $D$.
2. Let main current entering node $A$ be $I$. At node $A$, current splits into $I_1$ through arm $AB$ (resistor $P$) and $I_2$ through arm $AD$ (resistor $R$).
3. At node $B$, current $I_g$ flows into the galvanometer. Remaining current through arm $BC$ (resistor $Q$) is $(I_1 - I_g)$.
4. At node $D$, current $I_2$ and $I_g$ join together, so current flowing through arm $DC$ (resistor $S$) is $(I_2 + I_g)$.
• Apply Kirchhoff's Loop Rule (KVL) to Loop 1 ($ABDA$):
• Apply Kirchhoff's Loop Rule (KVL) to Loop 2 ($BCDB$):
• Balanced Condition (Null Deflection in Galvanometer):
When the bridge is balanced, potential at node $B$ equals potential at node $D$ ($V_B = V_D$). Thus, no current flows through the galvanometer: $I_g = 0$.
Substitute $I_g = 0$ into Eq. 1:
Substitute $I_g = 0$ into Eq. 2:
Dividing Eq. 3 by Eq. 4:
Trap 1: Interchanging Battery and Galvanometer
*Board Question:* What happens to the balance condition if the battery and galvanometer are interchanged?
*Answer:* The balance condition REMAINS UNCHANGED! If $P/Q = R/S$, interchanging source and detector simply swaps conjugate arms ($P/R = Q/S$). The galvanometer still shows zero deflection.
Trap 2: KVL Sign Convention Mishaps
• Moving across a resistor *in the direction of current* $\implies$ Potential drop: $\mathbf{-IR}$.
• Moving across a resistor *opposite to current* $\implies$ Potential gain: $\mathbf{+IR}$.
• Moving through a cell from negative to positive terminal $\implies \mathbf{+\mathcal{E}}$.
• Moving from positive to negative terminal $\implies \mathbf{-\mathcal{E}}$.
Trap 3: Maximum Bridge Sensitivity
A Wheatstone bridge is most sensitive (shows maximum noticeable needle deflection for the smallest change in resistance) when all four arms have nearly equal resistances ($P \approx Q \approx R \approx S$). If one arm is $1\text{ }\Omega$ and another is $10{,}000\text{ }\Omega$, sensitivity drops dramatically.
Trap 4: Resistance of Central Galvanometer Arm at Balance
When the bridge is balanced ($I_g = 0$), the central galvanometer branch carries no current. Therefore, it can be completely removed from equivalent resistance calculations! The network simplifies to $(P+Q)$ in parallel with $(R+S)$: $R_{\text{eq}} = \frac{(P+Q)(R+S)}{(P+Q) + (R+S)}$.
Problem: The four arms of a Wheatstone bridge have the following resistances: $AB = 100\text{ }\Omega$, $BC = 10\text{ }\Omega$, $CD = 5\text{ }\Omega$, and $DA = 60\text{ }\Omega$. A galvanometer of resistance $15\text{ }\Omega$ is connected across $BD$. Calculate the current through the galvanometer when a potential difference of $10\text{ V}$ is maintained across $AC$.
Solution:
1. Check bridge balance: $\frac{P}{Q} = \frac{100}{10} = 10$; $\frac{R}{S} = \frac{60}{5} = 12$. Since $10 \ne 12$, bridge is unbalanced ($I_g \ne 0$).
2. Apply KVL to Loop 1 ($ABDA$):
3. Apply KVL to Loop 2 ($BCDB$):
4. From Eq. [2]: $I_2 = 2 I_1 - 6 I_g$. Substitute $I_2$ into Eq. [1]:
5. Substitute $I_1$ to get $I_2$: $I_2 = 2(18.75 I_g) - 6 I_g = 31.5 I_g$.
6. Apply KVL along outer path through source ($AC$): $100 I_1 + 10(I_1 - I_g) = 10 \implies 110 I_1 - 10 I_g = 10$.
Substitute $I_1 = 18.75 I_g$:
Problem: In a Wheatstone bridge, $P = 2\text{ }\Omega, Q = 3\text{ }\Omega, R = 6\text{ }\Omega$, and $S = 8\text{ }\Omega$. What resistance $X$ must be connected in parallel across $S$ to balance the bridge?
Solution:
1. For the bridge to be balanced, the effective resistance in the fourth arm ($S'$) must satisfy:
2. But the existing resistance $S = 8\text{ }\Omega$. Notice that connecting a resistor $X$ in parallel can ONLY decrease the equivalent resistance below $8\text{ }\Omega$ ($S_{\text{parallel}} < 8\text{ }\Omega$). It can NEVER increase resistance to $9\text{ }\Omega$!
Exam Trap Note: To balance this bridge, a resistance of $1\text{ }\Omega$ must be connected in series with $S$ ($8 + 1 = 9\text{ }\Omega$), not in parallel. Examiners deliberately set this trap to catch blind formula substitution!
Kirchhoff Junction (KCL)
$\sum I = 0$ (Charge Cons.)
Kirchhoff Loop (KVL)
$\sum \Delta V = 0$ (Energy Cons.)
Wheatstone Balance
$\frac{P}{Q} = \frac{R}{S} \iff I_g = 0$
Max Sensitivity
$P \approx Q \approx R \approx S$