Problem 55
Question
A particle with charge \(+7.60 \mathrm{nC}\) is in a uniform electric field directed to the left. Another force, in addition to the electric force, acts on the particle so that when it is released from rest, it moves to the right. After it has moved \(8.00 \mathrm{cm},\) the additional force has done \(6.50 \times 10^{-5} \mathrm{J}\) of work and the particle has \(4.35 \times 10^{-5} \mathrm{J}\) of kinetic energy. (a) What work was done by the electric force? (b) What is the potential of the starting point with respect to the end point? (c) What is the magnitude of the electric field?
Step-by-Step Solution
Verified Answer
(a) Work by electric force: \(-2.15 \times 10^{-5} \mathrm{J}\). (b) Potential difference: \(2.83 \times 10^{3} \mathrm{V}\). (c) Electric field: \(3.54 \times 10^{3} \mathrm{N/C}\).
1Step 1: Determine Work Done by Electric Force
To find the work done by the electric force, we use the work-energy principle. The total work done on the particle is the sum of the work done by the electric force and the additional force, which equals the change in kinetic energy.Given:- Work done by additional force, \(W_a = 6.50 \times 10^{-5} \mathrm{J}\)- Change in kinetic energy, \(\Delta KE = 4.35 \times 10^{-5} \mathrm{J}\)Since the sum of the works done by the electric force and the additional force equals the change in kinetic energy, we have:\[ W_e + W_a = \Delta KE \]Rearranging gives:\[ W_e = \Delta KE - W_a = 4.35 \times 10^{-5} - 6.50 \times 10^{-5} = -2.15 \times 10^{-5} \mathrm{J} \]Thus, the work done by the electric force is \(-2.15 \times 10^{-5} \mathrm{J}\).
2Step 2: Calculate Potential Difference
To find the potential difference between the starting and ending points, use the definition of work done by an electric field and potential difference:\[ W_e = -q \Delta V \]Where:- \(W_e = -2.15 \times 10^{-5} \mathrm{J}\) (work done by the electric field)- \(q = 7.60 \times 10^{-9} \mathrm{C}\) (charge of the particle)Rearranging gives:\[ \Delta V = -\frac{W_e}{q} = -\frac{-2.15 \times 10^{-5} \mathrm{J}}{7.60 \times 10^{-9} \mathrm{C}} \approx 2.83 \times 10^{3} \mathrm{V} \]Thus, the potential difference is \(2.83 \times 10^{3} \mathrm{V}\), meaning the potential at the starting point is higher by this value compared to the endpoint.
3Step 3: Determine Electric Field Magnitude
To find the magnitude of the electric field, we relate work done by an electric force, electric field \(E\), charge \(q\), and displacement \(d\):\[ W_e = - qEd \]Given:- Displacement, \(d = 8.00 \mathrm{cm} = 0.08 \mathrm{m}\)- \(W_e = -2.15 \times 10^{-5} \mathrm{J}\) (work done by the electric field)- \(q = 7.60 \times 10^{-9} \mathrm{C}\) (charge)Rearranging for \(E\) gives:\[ E = -\frac{W_e}{qd} = -\frac{-2.15 \times 10^{-5} \mathrm{J}}{7.60 \times 10^{-9} \mathrm{C} \times 0.08 \mathrm{m}} \approx 3.54 \times 10^{3} \mathrm{N/C} \]So, the magnitude of the electric field is \(3.54 \times 10^{3} \mathrm{N/C}\).
Key Concepts
Work-Energy PrinciplePotential DifferenceElectric Field Magnitude
Work-Energy Principle
The work-energy principle is a fundamental concept in physics that describes the relationship between work done on an object and its kinetic energy change. It states that the work done by all forces acting on an object equals the change in its kinetic energy.
In this problem, the charged particle moves under the influence of both an electric force and an additional force. The total work is the sum of these forces' contributions, changing the particle's kinetic energy. If you know the work done by one of the forces and the change in kinetic energy, you can find the work done by the other force.
For our particle, the work-energy formula is: \[W_e + W_a = \Delta KE\]where:
In this problem, the charged particle moves under the influence of both an electric force and an additional force. The total work is the sum of these forces' contributions, changing the particle's kinetic energy. If you know the work done by one of the forces and the change in kinetic energy, you can find the work done by the other force.
For our particle, the work-energy formula is: \[W_e + W_a = \Delta KE\]where:
- \(W_e\) is the work done by the electric force
- \(W_a\) is the work done by the additional force
- \(\Delta KE\) is the change in kinetic energy
Potential Difference
Potential difference (voltage) is crucial when dealing with electric fields and is the work done per unit charge to move a charge between two points. In simple terms, it's the difference in electric potential energy per charge.
The formula for potential difference given the work done by an electric field is: \[\Delta V = -\frac{W_e}{q}\]where:
This result can be interpreted as the electric potential being greater where the particle starts, relative to where it stops, by the calculated potential difference. Understanding potential difference helps to grasp how electric fields store and transfer energy.
The formula for potential difference given the work done by an electric field is: \[\Delta V = -\frac{W_e}{q}\]where:
- \(W_e\) is the work done by the electric force
- \(q\) is the charge
This result can be interpreted as the electric potential being greater where the particle starts, relative to where it stops, by the calculated potential difference. Understanding potential difference helps to grasp how electric fields store and transfer energy.
Electric Field Magnitude
The electric field magnitude is a measure of the force per charge exerted by the electric field. It is a crucial quantity when analyzing electric forces in physics.
To find the electric field magnitude, utilize the relationship between work, electric field, charge, and displacement:\[W_e = - qEd\]Given that:
With this understanding, one can predict how charged particles will behave in any field and how much force they will experience over a distance.
To find the electric field magnitude, utilize the relationship between work, electric field, charge, and displacement:\[W_e = - qEd\]Given that:
- \(W_e\) is the work done by the electric field
- \(q\) is the charge
- \(d\) is the displacement
With this understanding, one can predict how charged particles will behave in any field and how much force they will experience over a distance.
Other exercises in this chapter
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