Analyzing the Setup
Welcome to the fascinating world of Zener diodes! Imagine you are an electrical engineer tasked with ensuring a delicate component receives exactly 15 V, no matter what.
That is exactly what this circuit does. We have a 22 V main power supply, but our load resistor RL only needs 15 V.
To achieve this, we place a Zener diode in parallel with the load. The Zener diode acts like a strict bouncer, refusing to let the voltage across it rise above its breakdown voltage of 15 V.
The Master Equation
First, we must confirm the bouncer is awake. Since our supply is 22 V, which is greater than 15 V, the Zener diode is actively in its breakdown region.
This means the voltage across the parallel load resistor RL is locked at 15 V. But where does the extra voltage go?
It is dropped across the series resistor Rs. The voltage across Rs is simply the difference: Vs=22−15=7 V.
Now, let's track the flow of electrons. Using Ohm's law, the total current leaving the battery is I=RsVs=357=51 A.
This total current reaches the junction and splits. A portion goes through the load, and the rest goes through the Zener diode.
The current through the load is IL=RLVz=9015=61 A.
Final Calculation
To find the current forced through the Zener diode, we apply Kirchhoff's Current Law. We subtract the load current from the total current.
This gives us Iz=I−IL=51−61=301 A.
Finally, we need the power dissipated by the Zener diode. Power is the product of voltage and current, so P=Vz×Iz=15×301=0.5 W.
The question asks for the answer in the format x×10−1 W. We can rewrite 0.5 W as 5×10−1 W.
Therefore, our final integer value is x=5.