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University Physics with Modern Physics

Hugh D. Young, Roger A. Freeman

Chapter 23

Electric Potential - all with Video Answers

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+ 3 more educators

Chapter Questions

04:18

Problem 1

A point charge $q_{1}=+2.40 \mu C$ is held stationary at the origin. A second point charge $q_{2}=-4.30 \mu C$ moves from the point $x=0.150 \mathrm{m}, y=0$ to the point $x=0.250 \mathrm{m}, y=0.250 \mathrm{m} .$ How much work is done by the electric force on $q_{2} ?$

Katie Mcalpine
Katie Mcalpine
Numerade Educator
05:58

Problem 2

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 $b ?$

Mohit Khurana
Mohit Khurana
Texas A&M University
05:12

Problem 3

Energy of the Nucleus. How much work is needed to assemble an atomic nucleus containing three protons (such as Be) if we model it as an equilateral triangle of side $2.00 \times 10^{-13} \mathrm{m}$ with a proton at each vertex? Assume the protons started from very far away.

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
07:07

Problem 4

(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 atomicdistance) 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?

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
10:07

Problem 5

A small metal sphere, carrying a net charge of $q_{1}=$ $-2.80 \mu C$ , is held in a stationary position by insulating sup- ports. A second small metal sphere, with a net charge of $q_{2}=$ $-7.80 \mu C$ and mass 1.50 $\mathrm{g}$ , is projected toward $q_{0} .$ 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, 23.30$)$ . 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 $q_{1} ?$

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
03:00

Problem 6

How far from a $-7.20-\mu \mathrm{C}$ point charge must $\mathrm{a}+2.30-\mu \mathrm{C}$ point charge be placed for the electric potential energy $U$ of the pair of charges to be $-0.400 \mathrm{J}$ ? (Take $U$ to be zero when the charges have infinite separation.)

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
12:28

Problem 7

A point charge $Q=+4.60 \mu \mathrm{C}$ is held fixed at the origin. A second point charge $q=+1.20 \mu \mathrm{C}$ with mass of $2.80 \times 10^{-4} \mathrm{kg}$ is placed on the $x$ -axis, 0.250 $\mathrm{m}$ from the origin. (a) What is the electric potential energy $U$ of the pair of charges? (Take $U$ to be zero when the charges have infinite scparation.) (b) The scond point charge is released from rest. What is its speed when its distance from the origin is (i) $0.500 \mathrm{m} ;$ (ii) $5.00 \mathrm{m} ;$ (iii) 50.0 $\mathrm{m} ?$

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
02:46

Problem 8

Three equal $1.20-\mu \mathrm{C}$ point charges are placed at the corners of an equilateral triangle whose sides are 0.500 $\mathrm{m}$ long. What is the potential energy of the system? (Take as zero the potential energy of the three charges when they are infinitely far apart)

Katie Mcalpine
Katie Mcalpine
Numerade Educator
10:49

Problem 9

A point charge $q_{1}=4.00 \mathrm{nC}$ is placed at the origin, and a second point charge $q_{2}=-3.00 \mathrm{nC}$ is placed on the $x$ -axis at$x=+20.0 \mathrm{cm} .$ A third point charge $q_{3}=2.00 \mathrm{nC}$ is to be placed on the $x$ -axis between $q_{1}$ and $q_{2}$ . Take as zero the potential energy of the three charges when they are infinitely far apart.) (a) What is

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
01:02

Problem 10

Four electrons are located at the corners of a square 10.0 $\mathrm{nm}$ on a side, with an alpha particle at its midpoint. How much work is needed to move the alpha particle to the midpoint of one of the sides of the square?

Anand Jangid
Anand Jangid
Numerade Educator
04:28

Problem 11

Three point charges, which initially are infinitely far apart, are placed at the corners of an equilateral triangle with sides $d$ . Two of the point charges are identical and have charge $q$ . If zerv net work is required to place the three charges at the comers of the triangle, what must the value of the third charge be?

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
06:04

Problem 12

Two protons are aimed directly toward each other by a cyclotron accelerator with speeds of 1000 $\mathrm{km} / \mathrm{s}$ , measured relative to the earth. Find the maximum electrical force that these protons will exert on each other.

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
02:08

Problem 13

A uniform electric field is directed due east. Point $B$ is 2.00 $\mathrm{m}$ west of point $A,$ point $C$ is 2.00 $\mathrm{m}$ east of point $A,$ and point $D$ is 2.00 $\mathrm{m}$ south of $\mathrm{A}$ . For cach point, $B, C,$ and $D,$ is the potential at that point larger, smaller, or the same as at point $A ?$ Give the reasoning behind your answers.

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
02:46

Problem 14

Identical point charges $q=+5.00 \mu \mathrm{C}$ are placed at opposite corners of a square. The length of each side of the square is 0.200 $\mathrm{m}$ . A point charge $q_{0}=-2.00 \mu \mathrm{C}$ is placed at one of the empty comers. How much work is done on $q_{0}$ by the electric force when $q_{0}$ is moved to the other empty comer?

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
06:59

Problem 15

A small particle has charge $-5.00 \mu \mathrm{C}$ and mass $2.00 \times 10^{-4} \mathrm{kg}$ . It moves from point $A$ , where the electric potential is $V_{A}=+200 \mathrm{V},$ to point $B$ , where the electric potential is $V_{B}=+800 \mathrm{V}$ . The electric force is the only force acting on the particle. The particle has speed 5.00 $\mathrm{m} / \mathrm{s}$ at point $A .$ What is its speed at point $B ?$ Is it moving faster or slower at $B$ than at $A ?$ Explain.

Katie Mcalpine
Katie Mcalpine
Numerade Educator
05:16

Problem 16

A particle with a charge of $+4.20 \mathrm{nC}$ is in a uniform electric field $\overrightarrow{\boldsymbol{E}}$ directed to the left. It is released from rest and moves to the left; after it has moved $6.00 \mathrm{cm},$ its kinetic energy is found to be $+1.50 \times 10^{-6} \mathrm{J}$ . $\mathrm{J}$ (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 $\overrightarrow{\boldsymbol{E}} ?$

Athiru Pathiraja
Athiru Pathiraja
Numerade Educator
06:26

Problem 17

A charge of 28.0 $\mathrm{nC}$ is placed in a uniform electric field that is directed vertically upward and has a magnitude of $4.00 \times 10^{4} \mathrm{V} / \mathrm{m}$ . What work is done by the electric force when the charge moves (a) 0.450 $\mathrm{m}$ to the right; (b) 0.670 $\mathrm{m}$ upward; (c) 2.60 $\mathrm{m}$ at an angle of $45.0^{\circ}$ downward from the horizontal?

John-Paul Mann
John-Paul Mann
Numerade Educator
14:22

Problem 18

Two stationary point charges $+3.00 \mathrm{nC}$ and $+2.00 \mathrm{nC}$ are separated by a distance of 50.0 $\mathrm{cm}$ . An electron is released from rest at a point midway between the two charges and moves along the line connecting the two charges. What is the speed of the electron when it is 10.0 $\mathrm{cm}$ from the $+3.00-\mathrm{charge}$ ?

Mohit Khurana
Mohit Khurana
Texas A&M University
02:11

Problem 19

A point charge has a charge of $2.50 \times 10^{-11} \mathrm{C}$ . At what distance from the point charge is the electric potential (a) 90.0 $\mathrm{V}$ and (b) 30.0 $\mathrm{V}$ ? Take the potential to be zero at an infinite distance from the charge.

Darshan Maheshwari
Darshan Maheshwari
Numerade Educator
10:37

Problem 20

Two charges of equal magnitude $Q$ are beld a distance $d$ apart. Consider only points on the line passing through both charges. (a) If the two charges have the same sign, find the location of all points (if there are any) at which (i) the potential (relative to infinity) is zero (is the electric field zero at these points?), and (ii) the electric field is zero (is the potential zero at these points?). and (b) Repeat part (a) for two charges having opposite signs.

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
04:28

Problem 21

Two point charges $q_{1}=$ $+2.40 \mathrm{nC}$ and $q_{2}=-6.50 \mathrm{nC}$ are 0.100 $\mathrm{m}$ apart. Point $A$ is midway between them; point $B$ is 0.080 $\mathrm{m}$ from $q_{1}$ and 0.060 $\mathrm{m}$ from $q_{2}$ (Fig. 23.31$)$ . Take the electric potential to be zero at infinity. Find (a) the potential at point $A ;$ (b) the potential at point $B ;$ (c) the work done by the electric fleld on a charge of 2.50 $\mathrm{nC}$ that travels from point $B$ to point $A$ .

Kai Chen
Kai Chen
Princeton University
05:11

Problem 22

Two positive point charges, each of magnitude $q,$ are fixed on the $y$ -axis at the points $y=+a$ and $y=-a$ . Take the potential to be zero at an infinite distance from the charges. (a) Show the positions of the charges in a diagram. (b) What is the potenntial $V_{0}$ at the origin? (c) Show that the potential at any point on the $x$ -axis is $$ V=\frac{1}{4 \pi \epsilon_{0}} \frac{2 q}{\sqrt{a^{2}+x^{2}}} $$ (d) Graph the potential on the $x$ -axis as a function of $x$ over the range from $x=-4 a$ to $x=+4 a$ . (e) What is the potential when $x \gg a ?$ Explain why this result is obtained.

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
03:21

Problem 23

A positive charge $+q$ is located at the point $x=0, y=-a$ and a negative charge $-q$ is located at the point $x=0, y=+a$ . (a) Show the positions of the charges in a diagram. (b) Derive an expression for the potential $V$ at points on the $x$ -axis as a function of the coondinate $x$ . Take $V$ to be zero at an infinite distance from the charges. (c) Graph $V$ at points on the $x$ -axis as a function of $x$ over the range from $x=-4 a$ to $x=+4 a$ . (d) What is the answer to part (b) if the two charges are interchanged so that $+q$ is at $y=+a$ and $-q$ is at $y=-a ?$

Darshan Maheshwari
Darshan Maheshwari
Numerade Educator
07:30

Problem 24

Consider the arrangement of charges described in cise 23.23 (a) Derive an expression for the potential $V$ at points on the $y$ -axis as a function of the coordinate $y$ . Take $V$ to be zero at an infinite distance from the charges. (b) Graph $V$ at points on the $y$ -axis as a function of $y$ over the range from $y=-4 a$ to positive $y$ -axis is given by $V=-\left(1 / 4 \pi \epsilon_{0}\right) 2 q a / y^{2} .$ (d) What are the answers to parts $(a)$ and $(c)$ if the two charges are interchanged so that $+q$ is at $y=+a$ and $-q$ is at $y=-a ?$

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
03:51

Problem 25

A positive charge $q$ is fixed at the point $x=0, y=0,$ and a negative charge $-2 q$ is fixed at the point $x=a, y=0$ . (a) Show the positions of the charges in a diagram. (b) Derive an expression for the potential $V$ at points on the $x$ -axis as a function of the coordinate $x$ . Take $V$ to be zero at an infinite distance from the charges. (c) At which positions on the $x$ -axis is $V=0 ?(\text { d) Graph }$ $V$ at points on the $x$ -axis as a function of $x$ in the range from $x=-2 a$ to $x=+2 a$ (e) What does the answer to part $(b)$ become when $x \gg a ?$ Explain why this result is obtained.

Salamat Ali
Salamat Ali
Numerade Educator
06:00

Problem 26

Consider the arrangement of point charges described in Exercise $23.25 .$ (a) Derive an expression for the potential $V$ at points on the $y$ -axis as a function of the coordinate $y$ . Take $V$ to be zero at an infinite distance from the charges. (b) At which positions on the $y$ -axis is $V=0 ?(\text { c) Graph } V \text { at points on the } y \text { -axis as a }$ function of $y$ in the range from $y=-2 a$ to $y=+2 a$ . (d) What does the answer to part (a) become when $y \gg a$ ? Explain why this result is obtained.

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
03:50

Problem 27

Before the advent of solid-state electronics, vacuum tubes were widely used in radios and other devices. A simple type of vacuum tube known as a diode consists essentially of two electrodes within a highly evacuated enclosure. One electrode, the cathode, is maintained at a high temperature and emits electrons from its surface. A potential difference of a few hundred volts is maintained between the cathode and the other electrode, known as the anode, with the anode at the higher potential. Suppose that in a particular vacuum tube the potential of the anode is 295 $\mathrm{V}$ higher than that of the cathode. An electron leaves the surface of the cathode with zero initial speed. Find its speed when it strikes the anode.

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
03:37

Problem 28

At a certain distance from a point charge, the potential and electric-field magnitude due to that charge are 4.98 $\mathrm{V}$ and $12.0 \mathrm{V} / \mathrm{m},$ respectively. (Take the potential to be zero at infinity.) (a) What is the distance to the point charge? (b) What is the magnitude of the charge? (c) Is the electric field directed toward or away from the point charge?

Katie Mcalpine
Katie Mcalpine
Numerade Educator
05:12

Problem 29

A uniform electric field has magnitude $E$ and is directed in the negative $x$ -direction. The potential difference between point $a$ (at $x=0.60 \mathrm{m}$ ) and point $b$ (at $x=0.90 \mathrm{m} )$ is 240 $\mathrm{V}$ . (a) Which point, $a$ or $b$ , is at the higher potential? (b) Calculate the value of E. (c) A negative point charge $q=-0.200 \mu \mathrm{C}$ is moved from $b$ to a. Calculate the work done on the point charge by the electric field.

John-Paul Mann
John-Paul Mann
Numerade Educator
36:05

Problem 30

For each of the following arrangements of two point charges, find all the points along the line passing through both charges for which the electric potential $V$ is zero (take $V=0$ infinitely far from the charges) and for which the electric field $E$ is zero: (a) charges $+Q$ and $+2 Q$ separated by a distance $d$ , and (b) charges $-Q$ and $+2 Q$ separated by a distance $d$ . (c) Are both $V$ and $E$ zero at the same places? Explain.

Mohit Khurana
Mohit Khurana
Texas A&M University
05:53

Problem 31

(a) An electron is to be accelerated from $3.00 \times 10^{6} \mathrm{m} / \mathrm{s}$ to $8.00 \times 10^{6} \mathrm{m} / \mathrm{s}$ . Through what potential difference must the electron pass to accomplish this? (b) Through what potential difference must the electron pass if it is to be slowed from $8.00 \times 10^{6} \mathrm{m} / \mathrm{s}$ to a halt?

Kai Chen
Kai Chen
Princeton University
06:52

Problem 32

A total electric charge of 3.50 $\mathrm{nC}$ is distributed uniformly over the surface of a metal sphere with a radius of $24.0 \mathrm{cm} .$ If the potential is zero at a point at infinity, find the value of the potential at the following distances from the center of the sphere: (a) $48.0 \mathrm{cm} ;(\mathrm{b}) 24.0 \mathrm{cm}$ (c) $12.0 \mathrm{cm} .$

Mohit Khurana
Mohit Khurana
Texas A&M University
08:24

Problem 33

A uniformly charged thin ring has radius 15.0 $\mathrm{cm}$ and total charge $+24.0 \mathrm{nC}$ . An electron is placed on the ring's axis a dis0tance 30.0 $\mathrm{cm}$ from the center of the ring and is constrained to stay on the axis of the ring. The electron is then released from rest. (a) Describe the subsequent motion of the electron. (b) Find the speed of the electron when it reaches the center of the ring.

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
05:19

Problem 34

An infinitely long line of charge has linear charge density $5.00 \times 10^{-12} \mathrm{C} / \mathrm{m} .$ A proton (mass $1.67 \times 10^{-27} \mathrm{kg}$ . charge $+1.60 \times 10^{-19} \mathrm{C} )$ is 18.0 $\mathrm{cm}$ from the line and moving directly toward the line at $1.50 \times 10^{3} \mathrm{m} / \mathrm{s}$ (a) Calculate the proton's initial kinetic energy. (b) How close does the proton get to the line of charge? (Hints See Example $23.10 . )$

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
03:56

Problem 35

A very long wire carries a uniform linear charge density $\lambda$ . Using a voltmeter to measure potential difference, you find that when one probe of the meter is placed 2.50 $\mathrm{cm}$ from the wire and the other probe is 1.00 $\mathrm{cm}$ farther from the wire, the meter reads 575 $\mathrm{V}$ . (a) What is $\lambda 2$ (b) If you now place one probe at 3.50 $\mathrm{cm}$ from the wire and the other probe 1.00 $\mathrm{cm}$ farther away, will the voltmeter read 575 $\mathrm{V} ?$ If not, will it read more or less than 575 $\mathrm{V}$ ? Why? (c) If you place both probes 3.50 $\mathrm{cm}$ from the wire but 17.0 $\mathrm{cm}$ from each other, what will the voltmeter read?

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
08:19

Problem 36

A very long insulating cylinder of charge of radius 2.50 $\mathrm{cm}$ carries a uniform linear density of 15.0 $\mathrm{nC} / \mathrm{m}$ . If you put one probe of a voltmeter at the surface, how far from the surface must the other probe be placed so that the voltmeter reads 175 $\mathrm{V} ?$

Mohit Khurana
Mohit Khurana
Texas A&M University
04:14

Problem 37

A very long insulating cylindrical shell of radius 6.00 $\mathrm{cm}$ carries charge of linear density 8.50$\mu \mathrm{C} / \mathrm{m}$ spread uniformly over its outer surface. What would a voltmeter read if it were connected between (a) the surface of the eylinder and a point 4.00 $\mathrm{cm}$ above the surface, and $(\mathrm{b})$ the surface and a point 1.00 $\mathrm{cm}$ from the cen- tral axis of the cylinder?

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
07:22

Problem 38

A ring of diameter 8.00 $\mathrm{cm}$ is fixed in place and carries a charge of $+5.00 \mu \mathrm{C}$ unifurnly spread over its circumference. (a) How much work does it take to move a tiny $+3.00-\mu \mathrm{C}$ charged ball of mass 1.50 $\mathrm{g}$ from very far away to the center of the ring? (b) Is it necessary to take a path along the axis of the ring? Why? (c) If the ball is slightly displaced from the center of the ring, what will it do and what is the maxi- mum speed it will reach?

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
02:09

Problem 39

Two very large, parallel metal plates carry charge densities of the same magnitude but opposite signs (Fig, 23.32$)$ . Assume they are close enough together to be treated as ideal infinite plates. Taking the potential to be zero at the left surface of the negative plate, sketch a graph of the potential as a function of $x$ . Include all regions from the left of the plates to the right of the plates.

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
04:50

Problem 40

Two large, parallel conducting plates carrying opposite charges of equal magnitude are separated by 2.20 $\mathrm{cm}$ . (a) If the nsurface charge density for each plate has magnitude 47.0 $\mathrm{nC} / \mathrm{m}^{2}$ , what is the magnitude of $\overrightarrow{\boldsymbol{E}}$ in the region between the plates? (b) What is the potential difference between the two plates? (c) If the separation between the plates is doubled while the surface charge density is kept constant at the value in part (a), what happens to the magnitude of the electric field and to the potential difference?

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
02:37

Problem 41

Two large, parallel, metal plates carry opposite charges of equal magnitude. They are separated by $45.0 \mathrm{mm},$ and the potential difference between them is 360 $\mathrm{V}$ . (a) What is the magnitude of the electric field (assumed to be uniform) in the region between the plates? (b) What is the magnitude of the force this field exerts on a particle with charge $+2.40 \mathrm{nC} ?$ (c) Use the results of part (b) to compute the work done by the field on the particle as it moves from the higher-potential plate to the lower. (d) Compare the result of part (c) to the change of potential energy of the same charge, computed from the electric potential.

Salamat Ali
Salamat Ali
Numerade Educator
01:44

Problem 42

(a) How much excess charge must be placed on a copper sphere 25.0 $\mathrm{cm}$ in diameter so that the potential of its center, relative to infinity, is 1.50 $\mathrm{kV}$ ? (b) What is the potential of the sphere's surface relative to infinity?

Athiru Pathiraja
Athiru Pathiraja
Numerade Educator
03:26

Problem 43

(a) Show that $V$ for a spherical shell of radius $R$ , that has charge $q$ distributed uniformly over its surface, is the same as $V$ for a solid conductor with radius $R$ and charge $q$ . (b) You $\mathrm{rub}$ an inflated balloon on the carpet and it acquires a potential that is 1560 $\mathrm{V}$ lower than its potential before it became charged. If the charge is uniformly distributed over the surface of the balloon and if the radius of the balloon is $15 \mathrm{cm},$ what is the net charge on the balloon? (c) In light of its $1200-\mathrm{V}$ potential difference relative to you, do you think this balloon is dangerous? Explain.

Athiru Pathiraja
Athiru Pathiraja
Numerade Educator
View

Problem 44

The electric field at the surface of a charged, solid, copper 0sphere with radius 0.200 $\mathrm{m}$ is 3800 $\mathrm{N} / \mathrm{C}$ , directed toward the center of the sphere. What is the potential at the center of the sphere, if we take the potential to be zero infinitely far from the sphere?

Susan Hallstrom
Susan Hallstrom
Numerade Educator
02:46

Problem 45

A potential difference of 480 $\mathrm{V}$ is established between large, parallel, metal plates. Let the potential of one plate be 480 $\mathrm{V}$ and the other be 0 $\mathrm{V}$ . The plates are separated by $d=1.70 \mathrm{cm} .$ (a) Sketch the equipotential surfaces that correspond to $0,120,$ $240,360,$ and 480 $\mathrm{V}$ . (b) In your sketch, show the electric field lines. Does your sketch confirm that the field lines and equipotential surfaces are mutually perpendicular?

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
08:49

Problem 46

A very large plastic sheet carries a uniform charge density of $-6.00 \mathrm{nC} / \mathrm{m}^{2}$ on one face. (a) As you move away from the sheet along a line perpendicular to it, does the potential increase or decrease? How do you know, without doing any calculations? Does your answer depend on where you choose the reference point for potential? (b) Find the spacing between equipotential surfaces that differ from each other by 1.00 $\mathrm{V}$ . What type of surfaces are these?

Mohit Khurana
Mohit Khurana
Texas A&M University
05:48

Problem 47

In a certain region of space, the electric potential is $V(x, y, z)=A x y-B x^{2}+C y,$ where $A, B,$ and $C$ are positive constants. (a) Calculate the $x-y$ - and $z$ -components of the electric field. (b) At which points is the electric field equal to zero?

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
05:27

Problem 48

The potential due to a point charge $Q$ at the origin may be written as $$ V=\frac{Q}{4 \pi \epsilon_{0} r}=\frac{Q}{4 \pi \epsilon_{0} \sqrt{x^{2}+y^{2}+z^{2}}} $$ (a) Calculate $E_{x}, E_{y}$ and $E_{z}$ using Eqs. $(23.19) .$ (b) Show that the results of part (a) agrecs with Eq. $(21.7)$ for the electric field of a point charge.

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
14:11

Problem 49

A metal sphere with radius $r_{a}$ is supported on an insulating stand at the center of a hollow, metal, spherical shell with radius $r_{b}$ . There is charge $+q$ on the inner sphere and charge $-q$ on the outer spherical shell. (a) Calculate the potential $V(r)$ for (i) $r < r_{c}$ : (ii) $r_{a} < r < r_{b} ;(\text { iii }) r > r_{b}$ (Hint: The net potential is the sum of the potentials due to the individual spheres.) Take $V$ to be zero when $r$ is infinite. (b) Show that the potential of the inner sphere with respect to the outer is $$ V_{a b}=\frac{q}{4 \pi \epsilon_{0}}\left(\frac{1}{r_{a}}-\frac{1}{r_{b}}\right) $$ (c) Use Eq. $(23.23)$ and the result from part (a) to show that the electric field at any point between the spheres has magnitude $$ E(r)=\frac{V_{a b}}{\left(1 / r_{a}-1 / r_{b}\right)} \frac{1}{r^{2}} $$ (d) Use Eq. $(23.23)$ and the result from part (a) to find the electric field at a point outside the larger sphere at a distance $r$ from the center, where $r > r_{b}$ (e) Suppose the charge on the outer sphere is not $-q$ but a negative charge of different magnitude, say $-Q$ . Show that the ans

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
07:58

Problem 50

A metal sphere with radius $r_{a}=1.20 \mathrm{cm}$ is supported on an insulating stand at the center of a hollow, metal, spherical shell with radius $r_{b}=9.60 \mathrm{cm} .$ Charge $+q$ is put on the inner sphere and charge $-q$ on the outer spherical shell. The magnitude of $q$ is chosen to make the potential difference between the spheres $500 \mathrm{V},$ with the inner sphere at higher potential. (a) Use the result of Exercise 23.49 (b) to calculate $q .$ (b) With the help of the result of Exercise $23.49(\mathrm{a}),$ sketch the equipotential surfaces that correspond to $500.400,300,200,100,$ and $0 \mathrm{V} .$ (c) In your sketch, show the electric field lines. Are the electric field lines and equipotential surfaces mutually perpendicular? Are the equipotential sur- faces closer together when the magnitude of $\vec{E}$ is largest?

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
07:01

Problem 51

A very long cylinder of radius 2.00 $\mathrm{cm}$ carries a uniform charge density of 1.50 $\mathrm{nC} / \mathrm{m}$ . (a) Describe the shape of the equipotential surfaces for this cylinder. (b) Taking the reference level for the zero of potential to be the surface of the cylinder, find the radius of equipotential surfaces having potentials of $10.0 \mathrm{V}, 20.0 \mathrm{V},$ and 30.0 $\mathrm{V}$ . (c) Are the equipotential surfaces equally spaced? If not, do they get closer together or farther apart as $r$ increases?

Athiru Pathiraja
Athiru Pathiraja
Numerade Educator
03:00

Problem 52

Figure 23.33 shows the potential of a charge distribution as a function of $x$ . Sketch a graph of the electric field $E_{x}$ over the region shown.

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
02:32

Problem 53

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?

Salamat Ali
Salamat Ali
Numerade Educator
04:51

Problem 54

In the Rohr model of the hydrogen atom, a single electron revolves around a single proton in a circle of radius $r .$ Assume that the proton remains at rest. (a) By equating the electric force to the electron mass times its acceleration, derive an expression for the electron's speed. (b) Obtain an expression for the electron's kinetic energy, and show that its magnitude is just half that of the electric potential energy. (c) Obtain an expression for the total energy, and evaluate it using $r=5.29 \times 10^{-11} \mathrm{m} .$ Give your numerical result in joules and in electron volts.

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
05:28

Problem 55

A vacuum tube diode (see Exercise 23.27$)$ consists of con- centric cylindrical electrodes, the negative cathode and the positive anode. Because of the accumulation of charge near the cathode, the electric potential between the electrodes is not a linear function of the position, even with planar geometry, but is given by $$ V(x)=C x^{4 / 3} $$ where $x$ is the distance from the cathode and $C$ is a constant, characteristic of a particular diode and operating conditions. Assume that the distance between the cathode and anode is 13.0 $\mathrm{mm}$ and the potential difference between electrodes is 240 $\mathrm{V}$ . (a) Determine the value of $C .$ ( b) Obtain a formula for the electric field between the electrodes as a function of $x$ . (c) Determine the force on an electron when the electron is halfway between the electrodes.

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
04:23

Problem 56

Two oppositely charged identical insulating spheres, cach 50.0 $\mathrm{cm}$ in diameter and carrying a uniform charge of magnitude 175$\mu \mathrm{C}$ , are placed 1.00 $\mathrm{m}$ apart center to center (Fig, 23.34$)$ (a) If a voltmeter is connected between the nearest points $(a \text { and } b)$ on their surfaces, what will it read? (b) Which point, $a$ or $b,$ is at the higher potential? How can you know this without any calculations?

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
07:48

Problem 57

An Ionic Crystal. ure 23.35 shows eight point charges arranged at the corners of a cube with sides of length $d$ . The values of the charges are $+q$ and $-q,$ as shown. This is a model of one cell of a cubic ionic crystal. In sodium chloride $(\mathrm{NaCl}),$ for instance, the positive ions are $\mathrm{Na}^{+}$ and the negative ions are $\mathrm{Cl}^{-}$ . (a) Calculate the potential energy $U$ of this arrangement. (Take as zero the potential energy of the eight charges when they are infinitely far apart.) (b) In part (a), you should have found that $U<0$ . Explain the relationship between this result and the observation that such ionic crystals exist in nature.

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
04:31

Problem 58

(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.)

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
08:00

Problem 59

The $\mathbf{H}_{2}^{+}$ Ion. The $\mathbf{H}_{2}^{+}$ ion is composed of two protons, each of charge $+e=1.60 \times 10^{-19} \mathrm{C},$ and an electron of charge $-e$ and mass $9.11 \times 10^{-31} \mathrm{kg} .$ The separation between the pro- tons is $1.07 \times 10^{-10} \mathrm{m}$ . The protons and the electron may be treated as point charges. (a) Suppose the electron is located at the point midway between the two protons. What is the potential energy of the interaction between the electron and the two protons? (Do not include the potential energy due to the interaction between the two protons.) (b) Suppose the electron in part (a) has a velocity of magnitude $1.50 \times 10^{6} \mathrm{m} / \mathrm{s}$ in a direction along the perpendicular bisector of the line connecting the two protons. How far from the point midway between the two protons can the electron move? Because the masses of the protons are much greater than the clectron mass, the motions of the protons are very slow and can be ignored. (Note: A realistic description of the electron motion requires the use of quantum mechanics, not Newtonian mechanics.)

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
03:17

Problem 60

A small sphere with mass 1.50 g hangs by a thread between two parallel vertical plates 5.00 $\mathrm{cm}$ apart (Fig, 23.36$)$ . The plates are insulating and have uniform surface charge densities $+\sigma$ and $-\sigma .$ The charge on the sphere is $q=8.90 \times 10^{-6} \mathrm{C}$ . What potential difference between the plates will cause the thread to assume an angle of $30.0^{\circ}$ with the vertical?

Supratim Pal
Supratim Pal
Numerade Educator
15:22

Problem 61

Coasial Cylinders. Along metal cylinder with radius $a$ is supported on an insulating stand on the axis of a long, hollow, metal tube with radius $b$ . The positive charge per unit length on the inner cylinder is $\lambda,$ and there is an equal negative charge per unit length on the outer cylinder. (a) Calculate the potential $V(r)$ for supported on an insulating stand on the axis of a long, hollow, metal tube with radius $b$ . The positive charge per unit length on the inner cylinder is $\lambda,$ and there is an equal negative charge per unit length on the outer cylinder. (a) Calculate the potential $V(r)$ for (i) $r < \alpha ;$ (ii) $a < r < b ;$ (iii) $r > b .$ (Hint: The net potential is the sum of the potentials due to the individual conductors.) Take $V=0$ at $r=b .(b)$ Show that the potential of the inner cylinder with respect to the outer is $$V_{a b}=\frac{\lambda}{2 \pi \epsilon_{0}} \ln \frac{b}{a}$$ (c) Use Eq. $(23.23)$ and the result from part (a) to show that the electric field at any point between the cylinders has magnitude $$ E(r)=\frac{V_{a b}}{\ln (b / a)} \frac{1}{r} $$ (d) What is the potential difference between the two cylinders if the outer cylinder has no net charge?

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
05:00

Problem 62

A Geiger counter detects radiation such as alpha particles by using the fact that the radiation ionizes the air along its path. A thin wire lics on the axis of a hollow metal cylinder and is insulated from it (Fig. 23.37$)$ . A large potential difference is established between the wire and the outer cylinder, with the wire at higher potential; this sets up a strong electric field directed radially higher potential; this sets up a strong electric field directed radially outward. When ionizing radiation enters the device, it ionizes a few air molecules. The free electrons produced are accelerated by the electric field toward the wire and, on the way there, ionize many more air molecules. Thus a current pulse is produced that can be detected by appropriate electronic circuitry and converted to an audible "click" Suppose the radius of the central wire is 145$\mu \mathrm{m}$ and the radius of the hollow cylinder is $1.80 \mathrm{cm} .$ What potential difference between the wire and the cylinder produces an

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
27:18

Problem 63

Deflection in a CRT. Cathode-ray tubes (CRTs) are often found in oscilloscopes and computer monitors. In Fig. 23.38 an electron with an initial speed of $6.50 \times 10^{6} \mathrm{m} / \mathrm{s}$ is projected along the axis midway between the deflection plates of a cathode-ray tube. The uniform electric field between the plates has a magnitude of $1.10 \times 10^{3} \mathrm{V} / \mathrm{m}$ and is upward. (a) What is the force (magnitude and direction) on the electron when it is between the plates? (b) What is the acceleration of the electron (magnitude and direction) when acted on by the force in part (a)? (c) How far below the axis has the electron moved when it reaches the end of the plates? (d) At what angle with the axis is it moving as it leaves the plates? (e) How far below the axis will it strike the fluorescent screen $\mathrm{S}$ ?

Maria Gabriela Cota Moreira
Maria Gabriela Cota Moreira
Numerade Educator
04:35

Problem 64

Deflecting Plates of an Oscilioscope. The vertical deflecting plates of a typical classroom oscilloscope are a pair of parallel square metal plates carrying equal but opposite charges. Typical dimensions are about 3.0 $\mathrm{cm}$ on a side, with a separation of about 5.0 $\mathrm{mm}$ . The plates are close enough that we can ignore fringing at the ends. Under these conditions: (a) how much charge is on each plate, and (b) how strong is the electric field between the plates?(c) If an electron is ejected at rest from the negative plates, how fast is it moving when it reaches the positive plate?

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
06:04

Problem 65

Electrostatic precipitators use electric forces to remove pollutant particles from smoke, in particular in the smokestacks of a coal-burning power plants. One form of precipitator consists of a vertical, hollow, metal cylinder with a thin wire, insulated from the cylinder, running along its axis (Fig. $23.39 ) .$ A large potential difference is established between the wire and the outer cylinder, with the wire at lower potential. This sets up a strong radial electric field directed inward. The field produces a region of ionized air near the wire. Smoke enters the precipitator at the bottom, ash and dust in it pick up electrons, and the charged pollutants are accelerated

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
06:16

Problem 66

A disk with radius $R$ has uniform surface charge density $\sigma .$ (a) By regarding the disk as a series of thin concentric rings, calculate the electric potential $V$ at a point on the disk's axis a distance $x$ . from the center of the disk. Assume that the potential is zero at infinity. (Hint: Use the result of Example 23.11 in Section $23.3 . )$ (b) Calculate $-\partial V / \partial x$ . Show that the result agrees with the expression for $E_{x}$ calculated in Example 21.12$(\text { Section } 21.5 \text { ). }$

Mohit Khurana
Mohit Khurana
Texas A&M University
07:46

Problem 67

(a) From the expression for $E$ obtained in Problem 22.40 , find the expressions for the electric potential $V$ as a function of $r$ , both inside and outside the cylinder. Let $V=0$ at the surface of the cylinder. In each case, express your result in terms of the charge per unit length $\lambda$ of the charge distribution. (b) Graph $V$ and $E$ as functions of $r$ from $r=0$ to $r=3 R$ .

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
08:03

Problem 68

Alpha particles $\left(\text { mass }=6.7 \times 10^{-27} \mathrm{kg}, \text { charge }=+2 e\right)$ are shot directly at a gold foil target. We can model the gold nucleus as a uniform sphere of charge and assume that the gold does not move. (a) If the radius of the gold nucleus is $5.6 \times$ $10^{-15} \mathrm{m}$ , what minimum speed do the alpha particles need when they are far away to reach the surface of the gold nucleus? (lanore relativistic effects.) (b) Give good physical reasons why we can ignore the effects of the orbital electrons when the alpha particle is (i) outside the electron orbits and (ii) inside the electron orbits.

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
03:06

Problem 69

For the ring of charge described in Example 23.11 (Section 23.3 ), integrate the expression for $E_{x}$ found in Example 21.10 $(\text { Section } 21.5)$ to find the potential at point $P$ on the ring's axis. Assume that $V=0$ at infinity. Compare your result to that obtained in Example 23.11 using Eq. $(23.16)$

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
03:43

Problem 70

A thin insulating rod is bent into a semicircular are of radius $a,$ and a total electric charge $Q$ is distributed uniformly along the rod. Calculate the potential at the center of curvature of the are if the potential is assumed to be zero at infinity.

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
04:02

Problem 71

Self-Energy of a Sphere of Charge. A solid sphere of radius $R$ contains a total charge $Q$ distributed uniformly through- out its volume. Find the energy needed to assemble this charge by bringing infinitesimal charges from far away. This energy is called the "self-energy" of the charge distribution. (Hint: After you have assembled a charge $q$ in a sphere of radius $r$ , how much energy would it take to add a spherical shell of thickness $d r$ having charge $d q ?$ Then integrate to get the total energy.)

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
08:47

Problem 72

(a) From the expression for $E$ obtained in Example 22.9 (Section 22.4$)$ , find the expression for the electric potential $V$ as a function of $r$ both inside and outside the uniformly charged sphere. Assume that $V=0$ at infinity. (b) Graph $V$ and $E$ as functions of $r$ from $r=0$ to $r=3 R$

Guilherme Barros
Guilherme Barros
Numerade Educator
04:17

Problem 73

A solid insulating sphere with radius $R$ has charge $\mathcal{O}$ uni- formly distributed throughout its volume. (a) Use the results of Problem 23.72 to find the magnitude of the potential difference between the surface of the sphere and its center. (b) Which is at higher potential, the surface or the center, if (i) $Q$ is positive and (ii) $Q$ is negative?

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
07:01

Problem 74

An insulating spherical shell with inner radius 25.0 $\mathrm{cm}$ and outer radius 60.0 $\mathrm{cm}$ carries a charge of $+150.0 \mu \mathrm{C}$ uniformly distributed over its outer surface (see Exercise $23.43 ) .$ Point $a$ is at the center of the shell, point $b$ is on the inner surface, and point $c$ is on the outer surface. (a) What will a voltmeter read if it is connected between the following points: (i) $a$ and $b ;$ (ii) $b$ and $c ;$ (iii) $c$ and infinity; (iv) $a$ and $c ?(b)$ Which is at higher potential: (i) $a$ or $b$ ; (ii) $b$ or $c ;$ (iii) $a$ or $c ?$ (c) Which, if any, of the answers would change sign if the charges were $-150 \mu \mathrm{C} ?$

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
10:08

Problem 75

Exercise 23.43 shows that, outside a spherical shell with uniform surface charge, the potential is the same as if all the charge were concentrated into a point charge at the center of the sphere. (a) Use this result to show that for two uniformly charged insulating shells, the force they exert on each other and their mutual electrical energy are the same as if all the charge were concentrated at their centers. (Hint: See Section $12.6 . )$ (b) Does this same result hold for solid insulating spheres, with charge distrib- uniformly throughout their volume? (c) Does this same result hold for the force between two charged conducting shells? Between two charged solid conductors? Explain.

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
09:27

Problem 76

Two plastic spheres, each carrying charge uniformly distributed throughout its interior, are initially placed in contact and then released. One sphere is 60.0 $\mathrm{cm}$ in diameter, has mass 50.0 $\mathrm{g}$ and contains $-10.0 \mu \mathrm{C}$ of charge. The other sphere is 40.0 $\mathrm{cm}$ in diameter, has mass 150.0 $\mathrm{g}$ , and contains $-30.0 \mu \mathrm{C}$ of charge. Find the maximum acceleration and the maximum speed achieved by each sphere (relative to the fixed point of their initial location in space), assuming that no other forces are acting on them. (Hint: The uniformly distributed charges behave as though they were concentrated at the centers of the two spheres.)

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
02:45

Problem 77

Use the electric field calculated in Problem 22.43 to calculate the potential difference between the solid conducting sphere and the thin insulating shell.

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
07:25

Problem 78

Consider a solid conducting sphere inside a hollow conduct-ing sphere, with radii and charges specified in Problem 22.42 . Take $V=0$ as $r \rightarrow \infty$ . Use the olectric ficld calculated in Problem 22.42 to calculate the potential $V$ at the following values of $r$ (a) $r=c$ (at the outer surface of the hollow sphere); (b) $r=b$ (at the inner surface of the hollow sphere); (c) $r=a$ (at the surface of the solid sphere); (d) $r=0$ (at the center of the solid sphere).

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
23:07

Problem 79

Electric charge is distributed uniformly along a thin rod of length $a,$ with total charge $Q .$ Take the potential to be zero at infinity. Find the potential at the following points (Fig. $23.40 ) :$ (a) point $P,$ a distance $x$ to the right of the rod, and (b) point $R,$ a distance $y$ above the right-hand end of the rod. (c) In parts (a) and (b), what does your result reduce to as $x$ or $y$ becomes much larger than $a ?$

Yaqub Khan
Yaqub Khan
Numerade Educator
05:57

Problem 80

(a) If a spherical raindrop of radius 0.650 $\mathrm{mm}$ carries a charge of $-1.20 \mathrm{pC}$ uniformly distributed over its volume, what is the potential at its surface? (Take the potential to be zero at an infinite distance from the raindrop.) (b) Two identical raindrops, each with radius and charge specified in part (a), collide and merge into one larger raindrop. What is the radius of this larger drop, and what is the potential at its surface, if its charge is uniformly distributed over its volume?

Kai Chen
Kai Chen
Princeton University
02:25

Problem 81

Two metal spheres of different sizes are charged such that the electric potential is the same at the surface of each. Sphere $A$ has a radius three times that of sphere $B$ . Let $Q_{A}$ and $Q_{B}$ be the charges on the two spheres, and let $E_{A}$ and $E_{B}$ be the electric-field magnitudes at the surfaces of the two spheres. What are (a) the ratio $Q_{B} / Q_{A}$ and (b) the ratio $E_{B} / E_{A} ?$

Salamat Ali
Salamat Ali
Numerade Educator
02:26

Problem 82

An alpha particle with kinetic energy 11.0 MeV makes a head-on collision with a lead nucleus at rest. What is the distance of closest approach of the two particles? (Assume that the lead nucleus remains stationary and that it may be treated as a point charge. The atomic number of lead is $82 .$ The alpha particle is a helium nucleus, with atomic number $2 .$ )

Aspen Fenzl
Aspen Fenzl
Numerade Educator
13:03

Problem 83

A metal sphere with radius $R_{1}$ has a charge $Q_{1}$ . Take the electric potential to be zero at an infinite distance from the sphere. (a) What are the electric field and electric potential at the surface of the sphere? This sphere is now connected by a long, thin conducting wire to another sphere of radius $R_{2}$ that is several meters from the first sphere. Before the connection is made, this second sphere is uncharged. After electrostatic equilibrium has been reached, what are (b) the total charge on each sphere; (c) the electric potential at the surface of each sphere (d) the electric field at the surface of each sphere? Assume that the amount of charge on the wire is much less than the charge on each sphere.

Mohit Khurana
Mohit Khurana
Texas A&M University
06:22

Problem 84

Use the charge distribution and electric field calculated in Problem $22.57 .$ ( a) Show that for $r \geq R$ the potential is identical to that produced by a point charge $Q .$ (Take the potential to be zero at infinity.) (b) Obtain an expression for the electric potential valid in the region $r \leq R$ .

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
12:00

Problem 85

Nuclear Fusion in the Sun. The source of the sun's energy is a sequence of nuclear reactions that occur in its core. The first of these reactions involves the collision of two protons, which fuse together to form a heavier nucleus and release energy. For this process, called nuclear fusion, to occur, the two protons must first approach until their surfaces are essentially in contact. (a) Assume both protons are moving with the same speed and they collide head-on. If the radius of the proton is $1.2 \times 10^{-15} \mathrm{m}$ , what is the minimum speed that will allow fusion to occur? The charge distribution within a proton is spherically symmetric, so the electric field and potential outside a proton are the same as if it were a point charge. The mass of the proton is $1.67 \times 10^{-27} \mathrm{kg}$ . (b) Another nuclear fusion reaction that occurs in the sun's core involves a collision between two helium nuclei, each of which has 2.99 times the mass of the proton, charge $+2 e,$ and radius $1.7 \times 10^{-15} \mathrm{m}$ . Assuming the same collision geometry as in part (a), what minimum speed is required for this fusion reaction to take place if the nuclei must approach a center-to-center distance of about $3.5 \times 10^{-15} \mathrm{m} ?$ As for the proton, the charge of the helium nucleus is uniformly distributed throughout its volume. (c) In Section 18.3 it was shown that the average translational kinetic energy of a particle with mass $m$ in a gas at absolute temperature $T$ is $\frac{3}{2} k T$ , where $k$ is the Boltxmann constant (given in Appendix F) For two protons with kinetic energy equal to this average value to be able to undergo the process described in part (a), what absolute temperature is required? What absolute temperature is required for two average helium nuclei to be able to undergo the process described in part (b)? (At these temperatures, atoms are completely ionized, so nuclei and electrons move separately.) (d) The temperature in the sun's core is about $1.5 \times 10^{7} \mathrm{K}$ . How does this compare to the temperatures calculated in part (c)? How can the reactions described in parts $(a)$ and $(b)$ occur at all in the interior of the sun? (Hint ) See the discussion of the distribution of molecular speeds in Section $18.5 .$ )

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
14:19

Problem 86

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 $\vec{E}$ 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 $(x, y, z)=$ 1.50-\muC 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 $(0,0,0.250$ 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 $y=2.00 \mathrm{m} ?$

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
09:55

Problem 87

Nuclear Fission. The unstable nucleus of uranium- 236 can be regarded as a uniformly charged sphere of charge $Q=+92 e$ and radius $R=$ $7.4 \times 10^{-15} \mathrm{m}$ . In nuclear fission, this can divide into twosion, this can divide into two smaller nuclei, each with half the charge and half the volume of the original uranium- 236 nucleus. This is one of the reactions that occurred in the nuclear weapon that exploded over Hiroshima, Japan, in August 1945 . (a) Find the radii of the two "daughter" nuclei of charge $+46 e$ . (b) In a simple model for the fission process, immediately after the uranium- 236 nucleus has undergone fission, the "daughter" nuclei are at rest and just touching, as shown in Fig. 23.41 . Calculate the kinetic energy that each of the "daughter" nuclei will have when they are very far apart. (c) In this model the sum of the kinetic energics of the two "daugh-teer" nuclei, calculated in part $(b),$ is the energy released by the fission of one uranium- 236 nucleus. Calculate the energy released bythe fission of 10.0 kg of uraninm- 236 . The atomic mass of nranium-236 is $236 \mathrm{u},$ where $1 \mathrm{u}=1$ atomic mass unit $=1.66 \times 10^{-24} \mathrm{kg}$ of this model, discuss why an atomic bomb could just as well be called an "electric bomb."

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
14:57

Problem 88

In a certain region, a charge distribution exists that is spher- ically symmetric but nonuniform. That is, the volume charge density $\rho(r)$ depends on the distance $r$ from the center of the distribution but not on the spherical polar angles $\theta$ and $\phi$ . The electric potential $V(r)$ due to this charge distribution is $$ V(r)=\left\{\begin{array}{l}{\frac{\rho_{0} a^{2}}{18 \epsilon_{0}}\left[1-3\left(\frac{r}{a}\right)^{2}+2\left(\frac{r}{a}\right)^{3}\right] \quad \text { for } r \leq a} \\ {\text { for } r \geq a}\end{array}\right. $$ where $\rho_{0}$ is a constant having units of $\mathrm{C} / \mathrm{m}^{3}$ and $a$ is a constant hav- ing units of meters. (a) Derive expressions for $\overrightarrow{\boldsymbol{E}}$ for the regions $r \leq a$ and $r \geq a$ . [Hint: Use Eq. $(23.23) . ]$ Explain why $\overrightarrow{\boldsymbol{E}}$ has only a radial component. (b) Derive an expression for $\rho(r)$ in each of the two regions $r \leq a$ and $r \geq a$ [Hint: Use Gauss's law for two spherical shells, one of radius $r$ and the other of radius $r+d r$ . The volume of a sphere of radius greater than or equal to $a$ is zero. IHint: Integrate the expressions derived in part (b) for $\rho(r)$ over a spherical volume of radius greater than or equal to $a$ . Is this result consistent with the electric field for $r>a$ that you calculated in part (a)?

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
08:49

Problem 89

In experiments in which atomic nuclei collide, head-on col0lisions like that described in Problem 23.82 do happen, but "near- misses" are more common. Suppose the alpha particle in Problem 23.82 was not "aimed" at the center of the lead nucleus, but had an initial nonzero angular momentum (with respect to the stationary lead nucleus) of magnitude $L=p_{0} b,$ where $p_{0}$ is the stationary lead nucleus) of magnitude $L=p_{0} b,$ where $p_{0}$ is the magnitude of the initial momentum of the alpha particle and $b=1.00 \times 10^{-12} \mathrm{m} .$ What is the distance of closest approach? Repeat for $b=1.00 \times 10^{-13} \mathrm{m}$ and $b=1.00 \times 10^{-14} \mathrm{m}$

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
16:08

Problem 90

A hollow, thin-walled insulating cylinder of radius $R$ and length $L$ (like the cardboard tube in a roll of toilet paper) has charge $Q$ uniformly distributed over its surface. (a) Calculate the electric potential at all points along the axis of the tube. Take the origin to be at the center of the tube, and take the potential to be zero at infinity. (b) Show that if $L \ll R$ , the result of part (a) reduces to the potential on the axis of a ring of charge of radius $R$ (See Example 23.11 in Section 23.3$)$ . (c) Use the result of part (a) of ind the electric field at all points along the axis of the tube.

Mohit Khurana
Mohit Khurana
Texas A&M University
08:10

Problem 91

The Milikan Oil-Drop Experiment. The charge of an electron was first measured by the American physicist Robert Millikan during $1909-1913$ . In his experiment, oil is sprayed in very fine drops (around $10^{-4} \mathrm{mm}$ in diameter) into the space between two parallel horizontal plates separated by a distance $d$ . A potential difference $V_{A B}$ is maintained between the parallel plates, causing a downward electric field between them. Some of the oil drops acquire a negative charge because of frictional effects or because of ionization of the surrounding air by $\mathrm{x}$ rays or radio- activity. The drops are observed through a microscope. (a) Show that an oil drop of radius $r$ at rest between the plates will remain at rest if the magnitude of its charge is $$ q=\frac{4 \pi \rho r^{3} g d}{3 V_{A B}} $$ where $\rho$ is the density of the oil. (Ignore the buoyant force of the air.) By adjusting $V_{A B}$ to keep a given drop at rest, the charge of on that drop can be determined, provided its radius is known. (b) Millikan's oil drops were much too small to measure their radii directly. Instead, Millikan determined $r$ by cutting off the electric field and measuring the terminal speed $v_{1}$ of the drop as it fell. (We $$ q=18 \pi \frac{d}{V_{A B}} \sqrt{\frac{\eta^{3} v_{1}^{3}}{2 \rho g}} $$

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
13:48

Problem 92

Two point charges are moving to the right along the $x$ -axis. Point charge 1 has charge $q_{1}=2.00 \mu \mathrm{C}$ . mass $m_{1}=6.00 \times$ $10^{-5} \mathrm{kg}$ , and speed $v_{1}$ . Point charge 2 is to the right of $q$ and has charge $q_{2}=-5.00 \mu \mathrm{C}$ , mass $m_{2}=3.00 \times 10^{-5} \mathrm{kg}$ , and speed $v_{2}$ . At a particular instant, the charges are separated by a distance of 9.00 $\mathrm{mm}$ and have speeds $v_{1}=400 \mathrm{m} / \mathrm{s}$ and $v_{2}=1300 \mathrm{m} / \mathrm{s}$ . The only forces on the particles are the forces they exert on each other. (a) Determine the speed $v_{c m}$ of the center of mass of the system. (b) The relative energy $E_{\text { rel of the system is defined as the total }}$ energy minus the kinetic energy contributed by the motion of the center of mass: $$ E_{\mathrm{rel}}=E-\frac{1}{2}\left(m_{1}+m_{2}\right) v_{\mathrm{c}}^{2} $$ where $E=\frac{1}{2} m_{1} v_{1}^{2}+\frac{1}{2} m_{2} v_{2}^{2}+q_{1} q_{2} | 4 \pi \epsilon_{0} r$ is the total energy of the system and $r$ is the distance between the charges. Show that $E_{\text { rel }}=\frac{1}{2} \mu v^{2}+q_{1} q_{2} | 4 \pi \epsilon_{0} r,$ where $\mu=m_{1} m_{2} /\left(m_{1}+m_{2}\right)$ is called the reduced mass of the system and $v=v_{2}-v_{1}$ is the relative speed of the moving particles. (c) For the numerical values given above, calculate the numerical value of $E_{\text {rel}}$ (d) Based on the result of part (c), for the conditions given above, will the particles escape from one another? Explain. (e) If the particles do escape, what will be their final relative speed when $r \rightarrow \infty$ ? If the particles do not escape, what will be their distance of maximum separation? That is, what will be the value of $r$ when $v=0$ ? (f) Repeat parts $(c)-(e)-(e)$ for $v_{1}=400 \mathrm{m} / \mathrm{s}$ and $v_{2}=1800 \mathrm{m} / \mathrm{s}$ when the sepa- ration is

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator