The Secret of the Isolated Plates
Mastering Charge Distribution
Welcome to an intriguing puzzle from the world of electrostatics! At first glance, a circuit with multiple capacitors might look like a tangled web, but by applying a few fundamental principles, we can unravel it beautifully. Let's dive into the logic behind finding the exact charge on a specific plate.
The Principle of Facing Plates
Our journey begins with a crucial piece of information: the left plate of the 10μF capacitor carries a charge of −30μC.
Before we even look at the rest of the circuit, we must recall the most fundamental property of a capacitor: the facing plates of a capacitor always carry equal and opposite charges. This happens because the electric field inside the conducting material of the plates must be zero. Therefore, if the left plate has −30μC, the right plate of the 10μF capacitor must hold exactly +30μC.
The Isolated System
Now, let's trace the wire connected to that right plate. It branches out and connects to the left plates of both the 6μF and 4μF capacitors.
Notice something special about this H-shaped section of wire and plates? It is completely disconnected from any external battery or ground. It forms an isolated system. Assuming the capacitors were initially uncharged before any external connections were made, the law of conservation of charge dictates that the net charge of this isolated system must remain zero.
Mathematically, this means:
q10R+q6L+q4L=0
Substituting the value we found:
+30μC+q6L+q4L=0
This tells us that a total charge of −30μC is distributed between the left plates of the parallel combination.
Parallel Distribution
How does this −30μC split between the 6μF and 4μF capacitors? Because they are connected in parallel, they share the same potential difference (V).
Since Q=CV, and V is constant, the charge Q is directly proportional to the capacitance C. The larger capacitor will grab a larger share of the charge. We can use the charge division rule:
q6L=(C6+C4C6)×qtotal
The Final Trap
We've successfully calculated that the left plate of the 6μF capacitor holds −18μC. But wait! Read the question carefully. It asks for the charge on the right plate of the 6μF capacitor.
This is a classic trap. We must apply our first principle again. If the left plate has −18μC, the right plate must have the equal and opposite charge:
And there we have it! By systematically applying charge conservation and the rules of parallel circuits, we bypassed the irrelevant 2μF capacitor and arrived at the correct answer.