Problem 67
Question
A parallel-plate air capacitor has a capacitance of 920 pF. The charge on each plate is 2.55\(\mu \mathrm{C}\) . (a) What is the potential difference between the plates? (b) If the charge is kept constant, what will be the potential difference between the plates if the separation is doubled? (c) How much work is required to double the separation?
Step-by-Step Solution
Verified Answer
a) 2770 V, b) 5540 V, c) 3.23 mJ of work is needed.
1Step 1: Identify the Formula for Potential Difference
To find the potential difference (V) between the plates of a capacitor, use the formula: \( V = \frac{Q}{C} \), where \( Q \) is the charge on the plates and \( C \) is the capacitance.
2Step 2: Calculate Potential Difference (Part a)
Given \( Q = 2.55 \, \mu\text{C} = 2.55 \times 10^{-6} \text{C} \) and \( C = 920 \, \text{pF} = 920 \times 10^{-12} \text{F} \), use the formula: \( V = \frac{2.55 \times 10^{-6}}{920 \times 10^{-12}} = 2.77 \times 10^3 \, \text{V} \).
3Step 3: Understand the Effect of Separation Change
If the separation is doubled while keeping the charge constant, the capacitance will become half, because capacitance is inversely proportional to separation \( (C \propto \frac{1}{d}) \).
4Step 4: Calculate New Capacitance (Part b)
The new capacitance \( C' \) is \( \frac{C}{2} = \frac{920 \times 10^{-12}}{2} = 460 \times 10^{-12} \text{F} \).
5Step 5: Find New Potential Difference (Part b)
With the same charge \( Q = 2.55 \times 10^{-6} \text{C} \) but the new capacitance \( 460 \times 10^{-12} \text{F} \), the new potential difference \( V' = \frac{2.55 \times 10^{-6}}{460 \times 10^{-12}} = 5.54 \times 10^3 \, \text{V} \).
6Step 6: Calculate Work Done to Change Separation (Part c)
The work done to change the separation is equal to the change in the energy stored: \( W = \Delta U = \frac{1}{2}Q^2\left(\frac{1}{C'} - \frac{1}{C}\right) \).
7Step 7: Compute Work Done (Part c)
Using \( Q = 2.55 \times 10^{-6} \text{C} \), \( C = 920 \times 10^{-12} \text{F} \), and \( C' = 460 \times 10^{-12} \text{F} \), calculate \( W = \frac{1}{2} \times \frac{(2.55 \times 10^{-6})^2}{460 \times 10^{-12}} - \frac{1}{2} \times \frac{(2.55 \times 10^{-6})^2}{920 \times 10^{-12}} = 3.23 \times 10^{-3} \, \text{J} \).
Key Concepts
Potential DifferenceCapacitor ChargeElectric FieldEnergy Stored in Capacitor
Potential Difference
The potential difference between the plates of a capacitor, often denoted as \( V \), is an essential concept in understanding how capacitors function. This potential difference is the amount of electric potential energy per unit charge that is needed to move a charge between the plates of a capacitor. It is calculated using the formula \( V = \frac{Q}{C} \) where:
By changing the parameters, we see how the potential difference is affected, bringing deeper insights into capacitor behavior.
- \( Q \) is the charge stored on one plate of the capacitor in Coulombs.
- \( C \) is the capacitance in Farads, describing the capacitor's ability to store charge.
By changing the parameters, we see how the potential difference is affected, bringing deeper insights into capacitor behavior.
Capacitor Charge
Charge in a capacitor is denoted by \( Q \) and is one of the most fundamental attributes of a capacitor. It is the measure of electric charge stored on the plates. In this problem, the charge is given as 2.55 microcoulombs, which equals \( 2.55 \times 10^{-6} \) Coulombs.
When the separation distance between the plates of the capacitor is altered while maintaining the charge, the potential difference changes. This modification does not change the stored charge itself but impacts how that charge interacts with the changing electric field.
Thus, charge stability is important in examining how different physical changes to the capacitor influence other properties like capacitance and potential difference.
When the separation distance between the plates of the capacitor is altered while maintaining the charge, the potential difference changes. This modification does not change the stored charge itself but impacts how that charge interacts with the changing electric field.
Thus, charge stability is important in examining how different physical changes to the capacitor influence other properties like capacitance and potential difference.
Electric Field
The electric field inside a capacitor is a constant field that develops between the two charged plates. It is more intense when the charges are closer together and less intense as they are further separated. The electric field in a parallel-plate capacitor can be considered uniform, pointing from the positive plate to the negative one.
- It is related to potential difference and separation by \( E = \frac{V}{d} \), where \( d \) is the separation distance between plates.
- The stronger the electric field, the more potential energy per charge available in the system.
Energy Stored in Capacitor
A capacitor not only stores charge but also energy, commonly known as the electric potential energy. This energy is stored in the electric field between the plates. The energy stored \( U \) in a capacitor can be expressed in multiple formulas, with one being \( U = \frac{1}{2} C V^2 \).
In this provided problem, another formula is applied during the calculation of work done to change the separation, \( W = \Delta U = \frac{1}{2}Q^2\left(\frac{1}{C'} - \frac{1}{C}\right) \). This equation highlights how altering plate separation impacts stored energy and requires work due to changes in capacitance and potential difference.
In this provided problem, another formula is applied during the calculation of work done to change the separation, \( W = \Delta U = \frac{1}{2}Q^2\left(\frac{1}{C'} - \frac{1}{C}\right) \). This equation highlights how altering plate separation impacts stored energy and requires work due to changes in capacitance and potential difference.
- Stored energy provides insights into the potential capacity of the circuit to perform work.
- Understanding energy transformations in capacitors underlines their significance in circuits, such as energy management, regulation, and storage.
Other exercises in this chapter
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