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(a) How much work would it take to push two protons very slowly from a separation of \(2.00 \times 10^{-10} \mathrm{~m}\) (a typical atomic distance) to \(3.00 \times 10^{-15} \mathrm{~m}\) (a typical nuclear distance)? (b) If the protons are both released from rest at the closer distance in part (a), how fast are they moving when they reach their original separation?

Short Answer

Expert verified
(a) The work done is approximately \(7.68 \times 10^{-14} \, \text{J}\). (b) The speed of the protons is \(3.04 \times 10^7 \, \text{m/s} \).

Step by step solution

01

Understand the concept of work done

To find the work done in bringing two protons from one point to another, we need to consider the electrostatic force between them. This force is given by Coulomb's Law: \[ F = \frac{k \cdot |q_1 \cdot q_2|}{r^2} \]where \( k \) is the Coulomb's constant \( (8.99 \times 10^9 \text{ Nm}^2/\text{C}^2) \) and \( q_1 \) and \( q_2 \) are the charges of the protons. Protons have the same charge \( (1.602 \times 10^{-19} \text{ C}) \).
02

Calculate work done to change distance

The work done, \( W \), in moving the two protons from an initial distance \( r_1 \) to a final distance \( r_2 \) is calculated using:\[ W = \int_{r_1}^{r_2} F \, dr = \int_{r_1}^{r_2} \frac{k \cdot e^2}{r^2} \, dr \]This integral evaluates to:\[ W = k \cdot e^2 \left( \frac{1}{r_2} - \frac{1}{r_1} \right) \]Substitute \( k = 8.99 \times 10^9 \, \text{Nm}^2/\text{C}^2 \), \( e = 1.602 \times 10^{-19} \, \text{C} \), \( r_1 = 2.00 \times 10^{-10} \, \text{m} \), and \( r_2 = 3.00 \times 10^{-15} \, \text{m} \).
03

Compute the numerical value for work done

Substituting the values into the work formula we get:\[ W = (8.99 \times 10^9) \cdot (1.602 \times 10^{-19})^2 \left( \frac{1}{3.00 \times 10^{-15}} - \frac{1}{2.00 \times 10^{-10}} \right) \]Calculating:\[ W \approx 8.99 \times 10^9 \cdot 2.566 \times 10^{-38} \cdot (3.33 \times 10^{14}) \approx 7.68 \times 10^{-14} \, \text{J} \]
04

Use conservation of energy for velocity

In part (b), when released, potential energy converts to kinetic energy. Using conservation of energy, the total kinetic energy of both protons is equal to the work done:\[ 2 \cdot \frac{1}{2} mv^2 = W \]This simplifies to:\[ mv^2 = W \]
05

Solve for proton speed

Rearranging to find speed \( v \):\[ v = \sqrt{\frac{W}{m}} \]where \( m \) is the mass of a proton, \( 1.67 \times 10^{-27} \text{ kg} \). Substitute the work done:\[ v = \sqrt{\frac{7.68 \times 10^{-14}}{1.67 \times 10^{-27}}} \approx 3.04 \times 10^7 \, \text{m/s} \]

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Coulomb's Law
Coulomb's Law is fundamental in understanding electrostatics. It describes the force between two charged objects. The law states that the electrostatic force (\( F \)) between two charges is directly proportional to the product of the magnitudes of the charges and inversely proportional to the square of the distance between them. Mathematically, this is expressed as:
\[ F = \frac{k \cdot |q_1 \cdot q_2|}{r^2} \]where:
  • \( k \) is the Coulomb's constant \( (8.99 \times 10^9 \text{ Nm}^2/\text{C}^2) \).
  • \( q_1 \) and \( q_2 \) are the magnitudes of the charges.
  • \( r \) is the distance between the centers of the two charges.
For protons, both charges are equal (\( 1.602 \times 10^{-19} \text{ C} \)), making these forces repulsive. This foundational law helps calculate how charges interact and is a building block for deeper electrostatic concepts.
Work Done in Electric Fields
The concept of work done in electric fields involves moving charges under the influence of an electrostatic force. Similar to mechanical work, it refers to the energy needed to move a charge against the electric force. Here, work done (\( W \)) by an electric field in moving a charge from one point to another is given by:
\[ W = \int_{r_1}^{r_2} F \, dr = \int_{r_1}^{r_2} \frac{k \cdot e^2}{r^2} \, dr \]When you solve this integral, you find:
\[ W = k \cdot e^2 \left( \frac{1}{r_2} - \frac{1}{r_1} \right) \]This expression calculates the work required to bring two protons closer or push them apart. In our problem, we are moving protons from a distance of \( r_1 = 2.00 \times 10^{-10} \text{ m} \) to \( r_2 = 3.00 \times 10^{-15} \text{ m} \). The work done is the energy needed to overcome the electrostatic repulsion between them.
Conservation of Energy
The principle of conservation of energy states that energy cannot be created or destroyed, only converted from one form to another. In the context of the proton exercise, it helps us understand how potential energy converts into kinetic energy.
The initial potential energy when protons are at their closest (\( r_2 \)) equals the work done to bring them from \( r_1 \) to \( r_2 \). When released, this potential energy becomes kinetic energy, causing the protons to accelerate away from each other. The equation for kinetic energy conversion is:
\[ 2 \cdot \frac{1}{2} mv^2 = W \]Simplifying gives:
\[ mv^2 = W \]Here, \( m \) is the mass of a proton (\( 1.67 \times 10^{-27} \text{ kg} \)). With known work done (\( 7.68 \times 10^{-14} \text{ J} \)), you can find the speed \( v \) using the rearranged formula:
\[ v = \sqrt{\frac{W}{m}} \]This formula allows us to calculate the speed of protons when they are released from rest.
Proton-Proton Interaction
Protons are positively charged particles found in atomic nuclei, and they interact with each other through electrostatic forces. This interaction is crucial in understanding nuclear forces and structures. In our exercise, two protons start at a typical atomic distance of \( 2.00 \times 10^{-10} \text{ m} \) and are brought closer to a typical nuclear distance of \( 3.00 \times 10^{-15} \text{ m} \).
As they are both positively charged, they repel each other. This repulsion must be overcome to bring them closer, requiring work to be done against this electrostatic force. The work done in this process is part of the energy concepts in electrostatics, illustrating how energy considerations are crucial for understanding nuclear interactions. Understanding this interaction helps explain not only atomic structures but also phenomena like nuclear fusion, where such close proton-proton interactions occur.

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Most popular questions from this chapter

The electric potential \(V\) in a region of space is given by $$ V(x, y, z)=A\left(x^{2}-3 y^{2}+z^{2}\right) $$ where \(A\) is a constant. (a) Derive an expression for the electric field \(\overrightarrow{\boldsymbol{E}}\) at any point in this region. (b) The work done by the field when a \(1.50-\mu \mathrm{C}\) test charge moves from the point \((x, y, z)=\) \((0,0,0.250 \mathrm{~m})\) to the origin is measured to be \(6.00 \times 10^{-5} \mathrm{~J}\). Determine \(A\). (c) Determine the electric field at the point \((0,0\), \(0.250 \mathrm{~m}\) ). (d) Show that in every plane parallel to the \(x z\)-plane the equipotential contours are circles. (e) What is the radius of the equipotential contour corresponding to \(V=1280 \mathrm{~V}\) and \(\mathrm{y}=2.00 \mathrm{~m}\) ?

Charges \(+q,-q,+q,-q\) areplaced at corners \(A B C D\) of a square of a side \(a\). A charge \(+q\) is placed at its centre. Find the interaction energy of the system

A point charge \(q_{1}\) is held stationary at the origin. A second charge \(q_{2}\) is placed at point \(a\), and the electric potential energy of the pair of charges is \(+5.4 \times 10^{-8} \mathrm{~J}\). When the second charge is moved to point \(b\), the electric force on the charge does \(-1.9 \times 10^{-8} \mathrm{~J}\) of work. What is the electric potential energy of the pair of charges when the second charge is at point \(b\) ?

A non-conducting slab infinite in the \(x-y\) direction and thickness \(L\) in the \(z\) direction carries uniform positive volume charge density \(\rho(z)=\rho_{0}\) (a) Find and sketch the electric field as a function of ' \(z\) ' both outside and inside the slab. (b) If potential at \(z=0\) is taken to be zero, then find and sketch the electrostatic potential as a function of \(z\) both outside and inside the slab.

* (a) Calculate the potential energy of a system of two small spheres, one carrying a charge of \(2.00 \mu \mathrm{C}\) and the other a charge of \(-3.50 \mu \mathrm{C}\), with their centers separated by a distance of \(0.250 \mathrm{~m}\). Assume zero potential energy when the charges are infinitely separated. (b) Suppose that one of the spheres is held in place and the other sphere, which has a mass of \(1.50 \mathrm{~g}\), is shot away from it. What minimum initial speed would the moving sphere need in order to escape completely from the attraction of the fixed sphere? (To escape, the moving sphere would have to reach a velocity of zero when it was infinitely distant from the fixed sphere.)

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