Expression for Energy Stored in a Capacitor (NEET Physics)

AI Exam Summary 2 min quick recap

Derive the expression for energy stored in a charged capacitor. Hint: The relationship between capacitance, charge, and electric potential is key here.

  • Hint: The relationship between capacitance, charge, and electric potential is key here.
  • The energy stored in a capacitor is equal to the work done in accumulating charge within it.
  • This involves the relationship between electric potential and work.
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High-Yield Topper Tip: Frequently tested in competitive exams. Focus on boundary conditions and conceptual exceptions.

Derive the expression for energy stored in a charged capacitor.

Hint: The relationship between capacitance, charge, and electric potential is key here. The energy stored in a capacitor is equal to the work done in accumulating charge within it. This involves the relationship between electric potential and work.

Formula Used:

The relationship between voltage ([latex]V[/latex]), charge ([latex]Q[/latex]), and capacitance ([latex]C[/latex]) is given by:

[latex]V = \frac{Q}{C}[/latex]

where:

[latex]V[/latex] is the electric potential,

[latex]C[/latex] is the capacitance, and

[latex]Q[/latex] is the charge on the capacitor.

The work done ([latex]dW[/latex]) to move a small charge [latex]dQ[/latex] into a capacitor at potential [latex]V[/latex] is:

[latex]dW = V \, dQ[/latex]

Solution:

Consider a capacitor in a circuit with voltage [latex]V[/latex]. The capacitance [latex]C[/latex] and stored charge \( Q \) relate as:

[latex]Q = C \cdot V[/latex]

Our aim is to find the energy stored in the capacitor.

According to electrostatic principles, the energy stored in a capacitor is equal to the work required to transfer the charge into the capacitor under potential [latex]V[/latex]. Thus:

[latex]dW = V \, dQ[/latex]

Substitute [latex]V = \frac{Q}{C}[/latex]:

[latex]dW = \frac{Q}{C} \, dQ[/latex]

To find the total work [latex]W[/latex] done in moving the charge [latex]Q[/latex] to the capacitor, integrate:

[latex]W = \int_0^Q \frac{Q}{C} \, dQ[/latex]

[latex]W = \frac{1}{C} \int_0^Q Q \, dQ[/latex]

Solving the integral:

[latex]W = \frac{1}{2} \frac{Q^2}{C}[/latex]

Thus, the energy [latex]U[/latex] stored in the capacitor is:

[latex]U = \frac{1}{2} \frac{Q^2}{C}[/latex]

Using [latex]Q = C \cdot V[/latex], we can also express this as:

[latex]U = \frac{1}{2} C V^2[/latex]

Additional Information:

A capacitor is a device that stores energy by separating equal and opposite charges with a certain distance between them. The standard capacitors shown in textbooks are often parallel-plate capacitors. Capacitors are measured in farads (F), where one farad stores one coulomb (C) of charge across one volt (V) of potential difference.

Note: For a parallel-plate capacitor, capacitance [latex]C[/latex] can also be calculated with the formula:

[latex]C = \frac{\varepsilon A}{d}[/latex]

where [latex]\varepsilon[/latex] is the permittivity of the medium between the plates, [latex]A[/latex] is the plate area, and [latex]d[/latex] is the distance between the plates. Substituting this expression for [latex]C[/latex] allows us to express energy in terms of the area and separation of the plates.

 

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