Problem 5
Question
A small metal sphere, carrying a net charge of \(q_{1}=\) \(-2.80 \mu \mathrm{C},\) is held in a stationary position by insulating supports. A second small metal sphere, with a net charge of \(q_{2}=-7.80 \mu \mathrm{C} \quad\) and \(\operatorname{mass}\) \(1.50 \mathrm{g},\) is projected toward \(q_{1}\). When the two spheres are 0.800 \(\mathrm{m}\) apart, \(q_{2}\) is moving toward \(q_{1}\) with speed 22.0 \(\mathrm{m} / \mathrm{s}\) (Fig. E23.5). Assume that the two spheres can be treated as point charges. You can ignore the force of gravity. (a) What is the speed of \(q_{2}\) when the spheres are 0.400 \(\mathrm{m}\) apart? (b) How close does \(q_{2}\) get to \(q_{1}\) ?
Step-by-Step Solution
Verified Answer
(a) 15.4 m/s, (b) 0.175 m.
1Step 1: Understanding Conservation of Energy
We will use the conservation of energy principle here. The total energy when the spheres are 0.800 m apart is equal to the total energy when they are 0.400 m apart. This includes the kinetic energy and the electric potential energy. The equation is given by:\[ \frac{1}{2}mv_i^2 + k \frac{q_1 q_2}{r_1} = \frac{1}{2}mv_f^2 + k \frac{q_1 q_2}{r_2} \]where \(v_i\) and \(v_f\) are the initial and final velocities, and \(r_1\) and \(r_2\) are the initial and final distances between the charges.
2Step 2: Substitute Known Values
Substituting the known values into our energy conservation equation:\[ \frac{1}{2} imes 1.50 imes 10^{-3} \times 22.0^2 + \frac{8.99 \times 10^9 \times (-2.80 \times 10^{-6}) \times (-7.80 \times 10^{-6})}{0.800} = \frac{1}{2} imes 1.50 \times 10^{-3} \times v_f^2 + \frac{8.99 \times 10^9 \times (-2.80 \times 10^{-6}) \times (-7.80 \times 10^{-6})}{0.400} \]
3Step 3: Solve for Final Velocity
Simplify and solve the equation for \(v_f^2\):- Calculate the initial kinetic energy: \( \frac{1}{2} imes 1.50 imes 10^{-3} imes 22.0^2 \approx 0.363 \) J.- Calculate the initial potential energy: \( \frac{8.99 \times 10^9 imes (21.84 \times 10^{-12})}{0.800} \approx 0.246 \) J.- Calculate the final potential energy: \( \frac{8.99 \times 10^9 imes (21.84 \times 10^{-12})}{0.400} \approx 0.493 \) J.- Solve for final kinetic energy: \( 0.363 + 0.246 = 0.493 + \frac{1}{2} imes 1.50 \times 10^{-3} \times v_f^2 \).- Solve for \(v_f\): \(v_f = 15.4 \) m/s.
4Step 4: Calculate Closest Approach
To find how close \(q_2\) gets to \(q_1\), we set the final velocity \(v_f\) to zero at the closest approach, which gives the minimum potential energy point. Hence, all initial kinetic energy + initial potential energy is converted into potential energy:\[ 0.363 + 0.246 = \frac{8.99 \times 10^9 \times 21.84 \times 10^{-12}}{r_{min}} \]Solving for \(r_{min}\):\(r_{min} \approx 0.175 \) m.
Key Concepts
Electric Potential EnergyKinetic EnergyPoint ChargesElectrostatics
Electric Potential Energy
Electric potential energy is a form of energy associated with the positions of charged particles relative to each other. When two charges are involved, as with the small metal spheres in our example, the electric potential energy reflects their potential to interact via electrical forces.
This energy arises from the electrostatic forces between the charges. The formula for calculating the electric potential energy between two point charges is \[ U = k \frac{q_1 q_2}{r} \]where:
In our scenario, we see how this energy changes as the distance between the charged spheres shifts from 0.800 m to 0.400 m. The change in electric potential energy is crucial in determining new velocities of the spheres as they draw closer.
This energy arises from the electrostatic forces between the charges. The formula for calculating the electric potential energy between two point charges is \[ U = k \frac{q_1 q_2}{r} \]where:
- \( U \) is the electric potential energy,
- \( k \) is Coulomb's constant, approximately \( 8.99 \times 10^9 \text{ Nm}^2/\text{C}^2 \),
- \( q_1 \) and \( q_2 \) are the magnitudes of the charges,
- \( r \) is the distance between the charges.
In our scenario, we see how this energy changes as the distance between the charged spheres shifts from 0.800 m to 0.400 m. The change in electric potential energy is crucial in determining new velocities of the spheres as they draw closer.
Kinetic Energy
Kinetic energy is the energy of motion. It is defined by how fast an object is moving and its mass. In the context of moving charges, kinetic energy can be transformed into other energy forms, such as electric potential energy, as they interact with each other.
The basic formula for calculating kinetic energy is:\[ KE = \frac{1}{2} mv^2 \]where:
In the exercise, when the metal sphere with charge \( q_2 \) moves towards \( q_1 \) with an initial speed, it possesses kinetic energy. As it approaches the other charge, some of this kinetic energy is transformed into potential energy, reducing its speed until it reaches its closest point of approach.
The basic formula for calculating kinetic energy is:\[ KE = \frac{1}{2} mv^2 \]where:
- \( KE \) is the kinetic energy,
- \( m \) is the mass of the object,
- \( v \) is the velocity of the object.
In the exercise, when the metal sphere with charge \( q_2 \) moves towards \( q_1 \) with an initial speed, it possesses kinetic energy. As it approaches the other charge, some of this kinetic energy is transformed into potential energy, reducing its speed until it reaches its closest point of approach.
Point Charges
Point charges are theoretical charges that act as if they are concentrated at a single point in space. This simplification allows us to ignore the actual size of the objects and focus solely on the effects of charge and distance.
In physics problems like the one at hand, treating objects as point charges lets us focus on the fundamental principles of charge interaction without worrying about more complex spatial properties.
This approximation works well for many problems, offering a good understanding of electrostatic interactions between charged bodies by simplifying calculations. Thus, in our exercise, it is assumed that both spheres are point charges, making the calculations manageable while accurately illustrating the core principles of electrostatics.
In physics problems like the one at hand, treating objects as point charges lets us focus on the fundamental principles of charge interaction without worrying about more complex spatial properties.
This approximation works well for many problems, offering a good understanding of electrostatic interactions between charged bodies by simplifying calculations. Thus, in our exercise, it is assumed that both spheres are point charges, making the calculations manageable while accurately illustrating the core principles of electrostatics.
Electrostatics
Electrostatics is a branch of physics dealing with stationary or slow-moving electric charges. This field focuses on the forces and fields created by these charges, which are foundational to understanding many principles of electricity and magnetism.
Culminating in Coulomb's Law, electrostatics describes how charged objects exert forces on each other based on their charges and separation distance. In our example:
Understanding electrostatics involves comprehending conservation of energy principles, especially when dealing with mechanical energies such as kinetic and electric potential energy. This understanding allows us to predict motion and energy changes as charges interact.
Culminating in Coulomb's Law, electrostatics describes how charged objects exert forces on each other based on their charges and separation distance. In our example:
- The two charged spheres repel each other because like charges repel.
- Electrostatic forces result in changes in kinetic and potential energy as the distance between charges varies.
Understanding electrostatics involves comprehending conservation of energy principles, especially when dealing with mechanical energies such as kinetic and electric potential energy. This understanding allows us to predict motion and energy changes as charges interact.
Other exercises in this chapter
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