Analyzing the Setup
Let's carefully analyze the given circuit. We are presented with two parallel branches connected between terminals X and Y. The top branch contains diode D1 and a 10 Ω resistor in series. The bottom branch consists of diode D2 and a 5 Ω resistor.
The problem states that a 5 V battery is connected across X and Y, with the positive terminal specifically at X. This means point X is at a higher potential compared to point Y.
Now, let's check the biasing of both diodes. Diode D1 has its p-side (anode) connected to the positive terminal X, so it is forward biased. On the other hand, diode D2 has its n-side (cathode) connected to the positive terminal X, making it reverse biased.
The Master Equation
Since these are normal silicon diodes, they are not ideal. A practical forward-biased silicon diode acts like a 0.7 V battery opposing the current flow. A reverse-biased diode, however, acts as an open circuit.
Because the bottom branch containing D2 is an open circuit, absolutely no current can flow through it. The entire current I from the battery will flow exclusively through the top branch.
Let's apply Kirchhoff's Voltage Law (KVL) in this closed loop. Starting from the battery and moving clockwise, we gain 5 V, then drop 0.7 V across diode D1, and finally drop 10I volts across the resistor. This gives us our master equation:
Substituting the known voltage drop for a silicon diode:
Final Calculation
Now, it's just simple algebra. Subtracting the voltage drop gives us the net voltage available for the resistor:
Moving the 10I to the other side, we get:
Dividing by 10, we find the total current I supplied by the battery:
This perfectly matches option (d). Always remember to check the polarity of your battery before assuming which branches are active!