Analyzing the Setup
When dealing with Zener diode circuits, the most robust strategy is to use proof by contradiction. We start by assuming the Zener diode is in its breakdown region. If this assumption leads to a physically impossible scenario, we know the diode is actually off.
The Master Equation
Let's assume the Zener diode is in breakdown. This clamps the voltage across the entire parallel section to exactly Vz​=10 V.
Since the total source voltage is 12 V, the remaining voltage must drop across the series resistor R1​.
Now, we can find the total current supplied by the battery, which flows entirely through R1​:
Itotal​=R1​VR1​​=500 Ω2 V​=4 mA
Checking the Constraints
Next, let's look at the two R2​ resistors. They are both 1500 Ω and are connected in parallel. Their equivalent resistance is:
R2eq​=21500 Ω​=750 Ω
If the voltage across this parallel combination is indeed 10 V, the current required by these resistors alone would be:
IR2​=750 Ω10 V​=13.33 mA
The Contradiction
Here is where the physics breaks down. The main branch is only supplying 4 mA of current. However, the parallel resistors are demanding 13.33 mA to maintain the 10 V drop.
By Kirchhoff's Current Law, the current through the Zener diode would have to be:
Iz​=Itotal​−IR2​=4 mA−13.33 mA=−9.33 mA
A negative current implies the Zener diode is acting as a power source, which is impossible for a passive component in this configuration.
Final Calculation
Because our assumption led to a contradiction, the Zener diode never reached the breakdown voltage. It remains reverse-biased but non-conducting, acting effectively as an open circuit.
Therefore, the current through the Zener diode is exactly zero.
(Bonus Insight: If you remove the Zener and calculate the actual voltage across the parallel resistors, it comes out to 7.2 V, which is well below the 10 V threshold needed to turn the Zener on!)