Problem 39
Question
Two large, parallel, metal plates carry opposite charges of equal magnitude. They are separated by \(45.0 \mathrm{mm},\) and the potential difference between them is 360 \(\mathrm{V}\) (a) What is the magnitude of the electric field (assumed to be uniform) in the region between the plates? (b) What is the magnitude of the force this field exerts on a particle with charge \(+2.40 \mathrm{nC}^{\prime}\) (c) Use the results of part (b) to compute the work done by the field on the particle as it moves from the higher-potential plate to the lower. (d) Compare the result of part (c) to the change of potential energy of the same charge, computed from the electric potential.
Step-by-Step Solution
Verified Answer
(a) 8000 V/m, (b) 1.92 × 10^{-5} N, (c) 8.64 × 10^{-7} J, (d) Same work and potential energy change.
1Step 1: Calculate Electric Field (E)
The electric field between two parallel plates is given by the formula \( E = \frac{V}{d} \), where \( V \) is the potential difference and \( d \) is the separation distance. Given \( V = 360 \; \mathrm{V} \) and \( d = 45.0 \; \mathrm{mm} = 0.045 \; \mathrm{m} \), plugging these values into the formula gives \( E = \frac{360}{0.045} = 8000 \; \mathrm{V/m} \).
2Step 2: Calculate Force (F) on the Charge
The force on a charge in an electric field is calculated using \( F = qE \), where \( q \) is the charge and \( E \) is the electric field. With \( q = +2.40 \; \mathrm{nC} = 2.40 \times 10^{-9} \; \mathrm{C} \) and \( E = 8000 \; \mathrm{V/m} \), the force is \( F = 2.40 \times 10^{-9} \times 8000 = 1.92 \times 10^{-5} \; \mathrm{N} \).
3Step 3: Calculate Work Done (W) by the Field
The work done by the electric field when moving a charge over a potential difference is given by \( W = qV \). Using \( q = 2.40 \times 10^{-9} \; \mathrm{C} \) and \( V = 360 \; \mathrm{V} \), we find \( W = 2.40 \times 10^{-9} \times 360 = 8.64 \times 10^{-7} \; \mathrm{J} \).
4Step 4: Compare Work Done and Potential Energy Change
The change in electric potential energy for a charge moving through a potential difference \( V \) is also given by \( \Delta U = qV \). As \( \Delta U = 8.64 \times 10^{-7} \; \mathrm{J} \), same as work done by the field, the work done by the electric field on the charge matches the change in potential energy.
Key Concepts
Electric Field CalculationForce on a Charge in an Electric FieldWork Done by Electric FieldPotential Energy Change in Electric Field
Electric Field Calculation
To determine the electric field between two parallel plates, we rely on a straightforward formula: \[ E = \frac{V}{d} \] where \( E \) signifies the electric field, \( V \) is the potential difference, and \( d \) is the distance separating the plates. It becomes simple when you recognize it as the ratio of potential voltage to separation distance. With the particulars from the problem, where \( V \) equals 360 volts and \( d \) is 0.045 meters (converting 45 mm into meters), it results in an electric field magnitude of \( 8000 \, \text{V/m} \).
This uniform field indicates a constant force experienced by any charge placed between these plates, facilitating consistent calculations for related quantities.
This uniform field indicates a constant force experienced by any charge placed between these plates, facilitating consistent calculations for related quantities.
Force on a Charge in an Electric Field
The force that an electric field exerts on a charge is calculated by the formula: \[ F = qE \] where \( F \) is the force, \( q \) is the charge, and \( E \) is the electric field.
This illustrates how electric fields can exert influence on charged particles, propelling them based on the field's intensity and the charge magnitude.
- Given a charge \( q = +2.40 \, \text{nC} = 2.40 \times 10^{-9} \, \text{C} \)
- Using the previously found electric field \( E = 8000 \, \text{V/m} \)
This illustrates how electric fields can exert influence on charged particles, propelling them based on the field's intensity and the charge magnitude.
Work Done by Electric Field
When a charge moves in an electric field, the work done by that field is determined by \[ W = qV \] where \( W \) is the work done, \( q \) is the charge, and \( V \) is the potential difference. The process involves the charge moving from one potential to another, transferring energy.
Work is essentially the energy required to move the charge across the plates, emphasizing the relationship between electric fields and energy transfer.
- Substituting \( q = 2.40 \times 10^{-9} \, \text{C} \)
- And \( V = 360 \, \text{V} \)
Work is essentially the energy required to move the charge across the plates, emphasizing the relationship between electric fields and energy transfer.
Potential Energy Change in Electric Field
The change in potential energy for a charge within an electric field is captured by the equation: \[ \Delta U = qV \] where \( \Delta U \) is the change in potential energy. In this exercise, it mirrors the work done formula, showing that the work done by the electric field exactly equals the change in the charge’s potential energy.
Using values
This correspondence illustrates the conservation of energy principles, reflecting how energy changes its form but remains constant in terms of quantity when moving through the electric field.
Using values
- \( q = 2.40 \times 10^{-9} \, \text{C} \)
- \( V = 360 \, \text{V} \)
This correspondence illustrates the conservation of energy principles, reflecting how energy changes its form but remains constant in terms of quantity when moving through the electric field.
Other exercises in this chapter
Problem 37
Axons. Neurons are the basic units of the nervous system. They contain long tubular structures called axons that propagate electrical signals away from the ends
View solution Problem 38
Two large, parallel conducting plates carrying opposite charges of equal magnitude are separated by 2.20 \(\mathrm{cm} .\) (a) If the surface charge density for
View solution Problem 40
Electrical Sensitivity of Sharks. Certain sharks can detect an electric field as weak as 1.0\(\mu \mathrm{V} / \mathrm{m} .\) To grasp how weak this field is, i
View solution Problem 41
(a) Show that \(V\) for a spherical shell of radius \(R,\) that has charge \(q\) distributed uniformly over its surface, is the same as \(V\) for a solid conduc
View solution