Capacitor | Principle Of Capacitor
Capacitor | Principle Of Capacitor :- A capacitor is a device used to store a large amount of electric charge and electrical energy in a small space. In general, a capacitor consists of a pair of conductors carrying equal and opposite charges, separated by an insulating (dielectric) medium, which is capable of storing a definite amount of charge.
Principle Of Capacitor
The principle of a capacitor is based on the fact that the capacitance can be increased by reducing the potential while keeping the charge constant.
Suppose a conducting plate M is given a positive charge Q until its electric potential increases to the maximum value (V). If more charge is supplied beyond this, it will start leaking from the plate.
At this time, the capacitance of plate M,
- Shape/Area of the plates
- Distance between the plates
- Nature of the medium (Dielectric constant K)
For example, the capacitance of a parallel plate capacitor is :
Here you can see that it has neither Q nor V.
Then the question arises: “When we decrease the potential, the capacitance increases — so doesn’t this mean that capacitance depends on V?“
There is a very subtle point hidden here :
➡️ When you decrease the voltage and increase the capacitance, you keep Q constant. This means that you are changing the geometry or the medium of the capacitor.
Example :
If you insert a dielectric material between the two plates —
- The dielectric reduces the potential
- But you keep Q constant
- Therefore, according to C = Q/V, the capacitance increases
➡️ This means that you actually changed the medium, rather than decreasing V ‘independently’.
Conclusion :
- Capacitance does not depend on the voltage V; rather, it depends on the physical construction of the capacitor.
- When we say that “capacitance increases by decreasing the potential”, it means that we have done something (such as inserting a dielectric or reducing the distance between plates) that caused V to decrease while Q remained constant — resulting in an increase in capacitance.
- However, this does not mean that C depends on V.
Mathematical example :
🔷 Condition 1 : Capacitor without dielectric material
Let’s say you have a parallel plate capacitor with the following characteristics :
- Area of the plates A = 1 m2
- Distance between the plates d = 1 mm = 10-3 m
- No dielectric material (K = 1)
- Let the total charge on the plates be Q = 1 μC = 10−6 C
Capacitance :
Potential :
🔷 Condition 2 : Now, we insert a dielectric material between the plates
Now, let’s say you keep the capacitor as it is, but insert a dielectric material between the plates with a dielectric constant K = 5
New capacitance :
New potential :
🔶 Now understand this changes :
| Change | Initially (no dielectric material) | Later (a dielectric material was inserted) |
| (Charge) | 10-6 C | Same |
| (Capacitance) | 8.85 × 10−9 F | Increased to 44.25 × 10−9 F |
| (Potential) | ≈ 113 V | Decreased to ≈ 22.6 V |
🔷 Conclusion :
- You changed the medium by inserting a dielectric material → this is a physical change, which increased the capacitance.
- The potential decreased, but that was the effect — not the cause.
- Therefore, capacitance does not depend on the potential; rather, the potential changes due to the capacitance and charge



