Problem 98
Question
A small sphere with mass \(m\) carries a positive charge \(q\) and is attached to one end of a silk fiber of length \(L\) . The other end of the fiber is attached to a large vertical insulating sheet that has a positive surface charge density \(\sigma\) . Show that when the sphere is in equilibrium, the fiber makes an angle equal to arctan \(\left(q \sigma / 2 m g \epsilon_{0}\right)\) with the vertical shee..
Step-by-Step Solution
Verified Answer
The fiber makes an angle \( \theta = \arctan \left( \frac{q\sigma}{2mg\epsilon_0} \right) \) with the vertical sheet.
1Step 1: Identify Forces
In equilibrium, the sphere is subjected to several forces: the gravitational force downward, the tension in the silk fiber, and the electric force due to the charged sheet. The gravitational force can be expressed as \( F_g = mg \), and the electric force on the sphere due to the charged sheet can be calculated using the formula for the electric field of an infinite sheet of charge, which is \( E = \frac{\sigma}{2\epsilon_0} \). Therefore, the electric force on the sphere is \( F_e = qE = \frac{q\sigma}{2\epsilon_0} \).
2Step 2: Break Down Forces Into Components
The tension in the fiber, \( T \), will have two components: a horizontal component \( T_{x} \) that balances the electric force and a vertical component \( T_{y} \) that balances the gravitational force. Thus, \( T_{y} = mg \) and \( T_{x} = \frac{q\sigma}{2\epsilon_0} \).
3Step 3: Express Components in Terms of Angle
Since the components of tension relate to the angle the fiber makes with the vertical, use trigonometry. The angle \( \theta \) with the vertical gives the relations \( T_{x} = T \sin(\theta) \) and \( T_{y} = T \cos(\theta) \). Thus, we have \( \tan(\theta) = \frac{T_{x}}{T_{y}} \).
4Step 4: Solve for Angle \( \theta \)
Plug the relations from Step 2 into the equation \( \tan(\theta) = \frac{T_{x}}{T_{y}} \) to get \( \tan(\theta) = \frac{\frac{q\sigma}{2\epsilon_0}}{mg} = \frac{q\sigma}{2mg\epsilon_0} \). Therefore, \( \theta = \arctan \left( \frac{q\sigma}{2mg\epsilon_0} \right) \).
Key Concepts
Electric fieldForce equilibriumTrigonometry in physics
Electric field
The concept of an electric field is foundational in electrostatics. Imagine an electric field as a region around a charged object where other charges feel a force. For example, our problem involves a large vertical insulating sheet with a positive surface charge density, denoted as \( \sigma \). This sheet creates an electric field around it, impacting the small charged sphere hanging by the fiber.
The electric field \( E \) produced by an infinite sheet of charge is uniform and can be calculated using the formula:
The electric field \( E \) produced by an infinite sheet of charge is uniform and can be calculated using the formula:
- \( E = \frac{\sigma}{2\varepsilon_0} \)
- \( F_e = qE = \frac{q\sigma}{2\varepsilon_0} \)
Force equilibrium
In physics, equilibrium refers to a state where all forces acting on an object balance each other, resulting in no net motion. This is crucial for analyzing the small sphere connected to the charged sheet in our exercise. The sphere is in equilibrium when the net force is zero, meaning the forces balance perfectly.Three forces act on the sphere:
- Gravitational force, which pulls the sphere downward with a force of \( mg \)
- Electric force from the charged sheet, pushing horizontally with force \( \frac{q\sigma}{2\varepsilon_0} \)
- Tension in the silk fiber, balancing the other two forces
Trigonometry in physics
Trigonometry is a mathematical tool that becomes very practical in physics, especially when dissecting forces into components. In this exercise, the angle \( \theta \) the fiber makes with the vertical is crucial for interpreting the forces.The tension in the fiber \( T \) is split into:
- Horizontal component: \( T_x = T \sin(\theta) \)
- Vertical component: \( T_y = T \cos(\theta) \)
- \( \tan(\theta) = \frac{\frac{q\sigma}{2\varepsilon_0}}{mg} = \frac{q\sigma}{2mg\varepsilon_0} \)
- \( \theta = \arctan\left(\frac{q\sigma}{2mg\varepsilon_0}\right) \)
Other exercises in this chapter
Problem 95
Positive charge \(+Q\) is distributed uniformly along the \(+x\) -axis from \(x=0\) to \(x=a .\) Negative charge \(-Q\) is distributed uniformly along the \(-x\
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View solution Problem 100
Two very large parallel sheets are 5.00 \(\mathrm{cm}\) apart. Sheet \(A\) carries a uniform surface charge density of \(-9.50 \mu \mathrm{C} / \mathrm{m}^{2}\)
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Two very large horizontal sheets are 4.25 \(\mathrm{cm}\) apart and carry equal but opposite uniform surface charge densities of magnitude \(\sigma .\) You want
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