Problem + Hard 3.3
Source: Problem 25-28 - pag 135 - HALLIDAY, RESNICK,
WALKER, Jearl - Book: Fundamentals of Physics - Vol 3 - Ed. LTC - 8th edition - 2009.
The capacitor C3 of the circuit in the figure below, on the left, is a capacitor whose capacitance can be varied. O
graph in the figure below, on the right, represents the electric potential V1 between the plates of the capacitor
C1 as a function of C3. For different values of C3 we have different values for
V1. We know that the electric potential V1 tends asymptotically to 10 volts when
C3 → ∞.
Determine:
a) The electric potential V of the source;
b) The values of C1 and C2.
Solution of the Problem + Hard 3.3
Item a
For the solution of this problem it is very important that we keep in mind the equation that relates charge, capacitance and voltage in
a capacitor. Below, we present this equation.
From the statement of the problem, it is known that when C3 → ∞ , the voltage across
the capacitor C1 approaches the value of 10 volts. If C3 → ∞,
it can be said that the association parallel of C2 and C3 is equal to C3.
Then the equivalent capacitance of the entire circuit will be equal to the value of C1, as the capacitors
are in series. And since the equation shown above should be satisfied, obviously it can be said that the voltage V23 drops asymptotically to zero. Then all the tension
of the voltage source will be applied to the capacitor C1. Therefore, it is concluded that:
V = V1 = 10 volts
Item b
To answer this item, two particularities must be taken into account:
1) Capacitors in series have equal charges, that is, q23 = q1.
2) From the graph provided in the problem, it can be seen that when C3 = 6 µF the voltage across the capacitor C1 is V1 = 5 volts. So it's obvious that V23 = 5 volts. Now, notice that if the charges are equal on the capacitors and the voltage across them is also equal, it follows that:
C1 = C2 + 6
In other words: the capacitance of the parallel association of C2 and C3 must be equal to
capacitance of C1.
Another information that can be taken from the graph: when C3 = 0 we have V1 = 2 volts.
Well, if V1 = 2 volts then V23 = 8 volts, because the sum of these voltages must be equal to voltage from the source, (V = 10 volts).
And, once again, as the charges must be equal, that is, q1 = q2, it follows that:
q1 = q2 ⇒ 2 C1 = 8 C2
Doing the simplification:
C1 = 4 C2
Therefore, a system of two equations with two unknowns with an extremely easy solution was obtained.
Therefore, the values of C1 and C2 are: