Related Formula
Voltage division across load RL$R_L$ with series resistance Rₛ$R_s$ without Zener regulation:
VL = Vᵢₙ ( (RL)/(Rₛ + RL) )$$V_L = V_{\text{in}} \left( \frac{R_L}{R_s + R_L} \right)$$
If VL > Vz$V_L > V_z$, the Zener diode enters breakdown, and potential across the parallel load is clamped at VL = Vz$V_L = V_z$.
Core Logic
Verify if Zener diode operates in the breakdown region:
V₁ = 12 × ( (400)/(100 + 400) ) = 12 × (4)/(5) = 9.6 ~V$$V_1 = 12 \times \left( \frac{400}{100 + 400} \right) = 12 \times \frac{4}{5} = 9.6 \mathrm{~V}$$
Since V₁ > Vz$V_1 > V_z$ (9.6 ~V > 4 ~V$9.6 \mathrm{~V} > 4 \mathrm{~V}$), breakdown occurs, and the parallel branch voltage is fixed at Vz = 4 ~V$V_z = 4 \mathrm{~V}$.
Step 1: Calculate Branch Current
The voltage across the 400 Ω$400 \Omega$ load resistor (which is in series with the ammeter) is locked at 4 ~V$4 \mathrm{~V}$.
The current I$I$ through the ammeter is:
I = (Vz)/(RL) = 4 ~V400 Ω = 10⁻² ~A = 10 ~mA$$I = \frac{V_z}{R_L} = \frac{4 \mathrm{~V}}{400 \Omega} = 10^{-2} \mathrm{~A} = 10 \mathrm{~mA}$$
Pattern Recognition
Sees: Parallel Zener diode configuration.
Shortcut: Always calculate the open-circuit load voltage first. If it exceeds Vz$V_z$, use Vz$V_z$ as the branch potential. The branch current is simply Vz / RL$V_z / R_L$. Here, 4 / 400 = 10 ~mA$4 / 400 = 10 \mathrm{~mA}$.
Chapter Mix
Class 12 Physics: Semiconductor Electronics: Materials, Devices and Simple Circuits