Problem 52
Question
A small sphere with mass \(5.00 \times 10^{-7} \mathrm{kg}\) and charge \(+3.00 \mu C\) is released from rest a distance of 0.400 \(\mathrm{m}\) above a large horizontal insulating sheet of charge that has uniform surface charge density \(\sigma=+8.00 \mathrm{pC} / \mathrm{m}^{2} .\) Using energy methods, calculate the speed of the sphere when it is 0.100 \(\mathrm{m}\) above the sheet of charge?
Step-by-Step Solution
Verified Answer
The speed of the sphere is approximately 7.17 m/s when it is 0.100 m above the sheet.
1Step 1: Understand the Problem
We have a small sphere with a given mass and charge that starts from rest and falls toward a charged sheet. We need to calculate its speed at a certain distance above the sheet using energy conservation principles.
2Step 2: Identify Relevant Formulas
The energy conservation principle involves equating the change in electric potential energy to the change in kinetic energy. The formula for electric potential energy change \[ \Delta U = q \cdot \Delta V \]where \( q \) is the charge of the sphere and \( \Delta V \) is the change in electric potential. The kinetic energy at a height \( h \):\[ K = \frac{1}{2} m v^2 \].
3Step 3: Calculate Electric Field from Surface Charge Density
The electric field \( E \) due to a large sheet with surface charge density \( \sigma \) is given by \[ E = \frac{\sigma}{2\varepsilon_0} \]where \( \varepsilon_0 \) is the permittivity of free space \( 8.85 \times 10^{-12} \, \mathrm{C^2/N \, m^2} \). Substitute \( \sigma = 8.00 \, \mathrm{pC/m^2} \) into the formula to find \( E \).
4Step 4: Calculate Change in Electric Potential
To calculate the change in electric potential (\( \Delta V \)), use \[ \Delta V = E \cdot \Delta h \]where \( \Delta h \) is the change in height from \( 0.400 \, \mathrm{m} \) to \( 0.100 \, \mathrm{m} \).
5Step 5: Calculate Change in Electric Potential Energy
Use \[ \Delta U = q \cdot \Delta V \],with \( q = 3.00 \times 10^{-6} \, \mathrm{C} \) to find the change in electric potential energy as the sphere moves closer to the sheet.
6Step 6: Apply Energy Conservation
The total mechanical energy is conserved, implying that the initial potential energy change is converted into kinetic energy. Therefore, solve \[ \Delta U = \frac{1}{2} m v^2 \]for \( v \), where \( m = 5.00 \times 10^{-7} \, \mathrm{kg} \).
7Step 7: Solve for the Speed
Rearrange and solve the equation \[ v = \sqrt{\frac{2 \times \Delta U}{m}} \]to find the speed \( v \) of the sphere when it is \( 0.100 \, \mathrm{m} \) above the charged sheet.
Key Concepts
Kinetic EnergyElectric FieldEnergy Conservation
Kinetic Energy
Kinetic energy is the energy that an object possesses due to its motion. In the context of our small sphere, we are interested in determining its kinetic energy as it approaches the charged sheet from an initial state of rest. The formula for calculating kinetic energy, denoted as \( K \), is given by:
\[ K = \frac{1}{2} m v^2 \]
where:
\[ K = \frac{1}{2} m v^2 \]
where:
- \( m \) is the mass of the object (in this case, the sphere).
- \( v \) is the speed of the object.
Electric Field
An electric field is a region around a charged object where force is exerted on other charged objects. In this problem, the electric field is created by the charged sheet, which has a uniform surface charge density \( \sigma \). The formula to find the magnitude of the electric field \( E \) due to a large sheet is:
\[ E = \frac{\sigma}{2\varepsilon_0} \]
where:
\[ E = \frac{\sigma}{2\varepsilon_0} \]
where:
- \( \sigma \) is the surface charge density (given as \( 8.00 \, \mathrm{pC/m^2} \)).
- \( \varepsilon_0 \) is the permittivity of free space (\( 8.85 \times 10^{-12} \, \mathrm{C^2/N \, m^2} \)).
Energy Conservation
Energy conservation is a fundamental principle stating that within a closed system, total energy remains constant. It involves converting one form of energy into another without any loss. In the exercise with the sphere, we apply energy conservation by equating the change in electric potential energy to the change in kinetic energy, ensuring the total mechanical energy remains the same throughout the sphere's movement.
The change in electric potential energy \( \Delta U \) is calculated using:
\[ \Delta U = q \cdot \Delta V \]
where:
\[ \frac{1}{2} m v^2 = \Delta U \]
we find the speed of the sphere. This principle helps ensure accurate computations and predictions of the sphere's dynamics as it interacts with the electric field of the charged sheet.
The change in electric potential energy \( \Delta U \) is calculated using:
\[ \Delta U = q \cdot \Delta V \]
where:
- \( q \) is the charge of the sphere (\( 3.00 \mu C \)).
- \( \Delta V \) is the change in electric potential.
\[ \frac{1}{2} m v^2 = \Delta U \]
we find the speed of the sphere. This principle helps ensure accurate computations and predictions of the sphere's dynamics as it interacts with the electric field of the charged sheet.
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