Homework 2 Due: 11:59pm on Sunday, February 27, 2011 Note: You will receive no credit for late submissions. To learn more, read your instructor's Grading Policy [ Switch to Standard Assignment View] Current Sheet Consider an infinite sheet of parallel wires. The sheet lies in the xy plane. A current runs in the -y direction through each wire. There are wires per unit length in the x direction. Part A Write an expression for , the magnetic field a distance above the xy plane of the sheet. Use for the permeability of free space. Hint A.1 How to approach the problem Hint not displayed Hint A.2 Find Hint not displayed Hint A.3 Determine the direction of the magnetic field Hint not displayed Hint A.4 Magnitude of the magnetic field Hint not displayed Hint A.5 Evaluate MasteringPhysics: Assignment Print View http://session.masteringphysics.com/myct/assignmentPrintView?assignme... 1 of 50 5/12/2011 8:00 PM
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Homework 2Due: 11:59pm on Sunday, February 27, 2011
Note: You will receive no credit for late submissions. To learn more, read your instructor's Grading Policy
[Switch to Standard Assignment View]
Current SheetConsider an infinite sheet of parallel wires. The sheet lies in the xy plane. A current runs in the -y direction
through each wire. There are wires per unit length in the x direction.
Part A
Write an expression for , the magnetic field a distance above the xy plane of the sheet.
Use for the permeability of free space.
Hint A.1 How to approach the problem
Hint not displayed
Hint A.2 Find
Hint not displayed
Hint A.3 Determine the direction of the magnetic field
Express the magnetic field as a vector in terms of any or all of the following: , , , , , and
the unit vectors , , and/or .
ANSWER: =
Correct
This equation is analogous to on either side of a infinitely charged sheet. The
correspondence seems more obvious if you set the current per unit length . Then the
magnetic field you just calculated is
.
The electric field, though, points along the perpendicular to the surface.
Do you see why you had to pick the rean loop you used? That is, why would any other loop not haveworked.Did you notice that by using Ampère's law you could find the field by using a much simpler integral thanBiot-Savart's law? The drawback is that you may not always be able to find a convenient loop insituations where the current distribution is more complicated.
Force between an Infinitely Long Wire and a Square LoopA square loop of wire with side length carries a current . The center of the loop is located a distance
from an infinite wire carrying a current . The infinite wire and loop are in the same plane; two sides of the
square loop are parallel to the wire and two are perpendicular as shown.
Part A
What is the magnitude, , of the net force on the loop?
Hint A.4 Find the force on the section of the loop closest to the wire
Hint not displayed
Hint A.5 Find the magnetic field due to the wire
Hint not displayed
Express the force in terms of , , , , and .
ANSWER: =
Correct
Part B
The magnetic moment of a current loop is defined as the vector whose magnitude equals the area of the
loop times the magnitude of the current flowing in it ( ), and whose direction is perpendicular to the
plane in which the current flows. Find the magnitude, , of the force on the loop from Part A in terms of the
magnitude of its magnetic moment.
Express in terms of , , , , and .
ANSWER: =
Correct
The direction of the net force would be reversed if the direction of the current in either the wire or theloop were reversed. The general result is that "like currents" (i.e., currents in the same direction)attract each other (or, more correctly, cause the wires to attract each other), whereas oppositelydirected currents repel. Here, since the like currents were closer to each other than the unlike ones,the net force was attractive. The corresponding situation for an electric dipole is shown in the figurebelow.
Setting in the previous expression yields the magnetic field for a semi-infinite wire:
,
which is in fact just half the value of the magnetic field due to an infinitely long wire. This differenceresults from the point chosen being close to one of the ends of the wire. Such "end effects" fornoninfinite wires always change the magneic field near that point.
Magnetic Field of a Current-Carrying WireFind the magnetic field a distance from the center of a long wire that has radius and carries a uniformcurrent per unit area in the positive z direction.
Part A
First find the magnetic field, , outside the wire (i.e., when the distance is greater than ).
From the Biot-Savart law, it can be calculated that the magnitude of the magnetic field due to a long straightwire is given by
,
where ( ) is the permeability constant, is the current in the wire, and is the
distance from the wire to the location at which the magnitude of the magnetic field is being calculated.
The same result can be obtained from Ampere's law as well.
The direction of vector can be found using the right-hand rule. (Take care in applying the right-hand rule.
Many students mistakenly use their left hand while applying the right-hand rule since those who use their righthand for writing sometimes automatically use their "pencil-free hand" to determine the direction of .)
In this problem, you will be asked to calculate the magnetic field due to a set of two wires with antiparallelcurrents as shown in the diagram . Each of the wirescarries a current of magnitude . The current in wire
1 is directed out of the page and that in wire 2 isdirected into the page. The distance between thewires is . The x axis is perpendicular to the line
connecting the wires and is equidistant from thewires.As you answer the questions posed here, try to lookfor a pattern in your answers.
Part A
Which of the vectors best represents the direction of the magnetic field created at point K (see the diagramin the problem introduction) by wire 1 alone?
Enter the number of the vector with the appropriate direction.
Find the magnitude of the magnetic field created at point K by wire 1.
Express your answer in terms of , , and appropriate constants.
ANSWER: =
Correct
Of course, because point K is equidistant from the wires.
Part E
Find the magnitude of the net magnetic field created at point K by both wires.
Express your answer in terms of , , and appropriate constants.
ANSWER: =
Correct
This result is fairly obvious because of the symmetry of the problem: At point K, the two wires eachcontribute equally to the magnetic field. At points L and M you should also consider the symmetry ofthe problem. However, be careful! The vectors will add up in a more complex way.
Part F
Point L is located a distance from the midpoint between the two wires. Find the magnitude of the
magnetic field created at point L by wire 1.
Hint F.1 How to approach the problem
Use the distances provided and the Pythagorean Theorem to find the distance between wire 1 and pointL.
Express your answer in terms of , , and appropriate constants.
Point L is located a distance from the midpoint between the two wires. Find the magnitude of the net
magnetic field created at point L by both wires.
Hint G.1 How to approach the problem
Sketch a detailed diagram with all angles marked; draw vectors and ; then add them using the
parallelogram rule.
Hint G.2 Find the direction of the magnetic field due to wire 1
Which of the vectors best represents the direction of the magnetic field created at point L (see thediagram in the problem introduction) by wire 1 alone?
Enter the number of the vector with the appropriate direction.
Hint G.4 Find the direction of the net magnetic field
Which of the vectors best represents the direction of the net magnetic field created at point L by bothwires?
Enter the number of the vector with the appropriate direction.
ANSWER: Answer not displayed
Hint G.5 Angle between magnetic field due to wire 1 and the x axis
Use the distances provided and your knowledge of right angle triangle trigonometry to find the anglebetween the magnetic field due to wire 1 at point L and the x axis.
Hint G.6 Find the angle between magnetic field due to wire 1 and the x axis
Use the distances provided and your knowledge of right angle triangle trigonometry to find the angle
between the magnetic field due to wire 1 at point L and the x axis.
Express your answer numerically, in degrees.
ANSWER: = Answer not displayed
Hint G.7 Net magnetic field
Consider the symmetry of the magnetic field at point L due to wire 1 and the magnetic field due to wire 2.You should note that the y components of these two vectors are of equal magnitude but are opposite in
direction. Therefore they will cancel when added together, leaving you only to worry about the xcomponents. Find the x component of the magnetic field at point L due to wire 1 by using the magnitudeof the vector (found in Part F) and the angle between the x axis and the magnetic field vector (found inthe previous hint). Because of symmetry, the x component of the magnetic field at point L due to wire 2 isthe same size. To find the net magnetic field at point L you need to add together the x components of themagnetic field at point L due to wire 1 and of the magnetic field due to wire 2.
Express your answer in terms of , , and appropriate constants.
ANSWER: =
All attempts used; correct answer displayed
Part H
Point M is located a distance from the midpoint between the two wires. Find the magnitude of the
magnetic field created at point M by wire 1.
Express your answer in terms of , , and appropriate constants.
ANSWER:
=
Correct
Part I
Find the magnitude of the net magnetic field created at point M by both wires.
Hint I.1 How to approach the problem
Hint not displayed
Hint I.2 Find the direction of the magnetic field due to wire 1
Hint not displayed
Hint I.3 Find the direction of the net magnetic field
Hint not displayed
Hint I.4 Angle between magnetic field due to wire 1 and the x axis
Hint not displayed
Hint I.5 Find the angle between magnetic field due to wire 1 and the x axis
Express your answer in terms of , , and appropriate constants.
ANSWER: =
All attempts used; correct answer displayed
Part J
Finally, consider point X (not shown in the diagram) located on the x axis very far away in the positive xdirection. Which of the vectors best represents the direction of the magnetic field created at point X by wire1 alone?
Enter the number of the vector with the appropriate direction.
ANSWER: 1Correct
Part K
Which of the vectors best represents the direction of the magnetic field created at point X by wire 2 alone?
Enter the number of the vector with the appropriate direction.
As you can see, at a very large distance, the individual magnetic fields (and the correspondingmagnetic field lines) created by the wires are directed nearly opposite to each other, thus ensuring thatthe net magnetic field is very, very small even compared to the magnitudes of the individual magneticfields, which are also relatively small at a large distance from the wires. Thus, at a large distance, themagnetic fields due to the two wires almost cancel each other out! (That is, if point X is very far fromeach wire, then the ratio is very close to zero.)
Another way to think of this is as follows: If you are really far from the wires, then it's hard to tell themapart. It would seem as if the current were traveling up and down, almost along the same line, therebyappearing much the same as a single wire with almost no net current (because the up and downcurrents almost cancel each other), and therefore almost no magnetic field. Note that this only worksfor points very far from the wires; otherwsie it's easy to tell that the wires are separated and thecurrents don't cancel, since they are going up and down at different locations.It comes as no surprise then that one way to eliminate unnecessary magnetic fields in electric circuitsis to twist together the wires carrying equal currents in opposite directions.
± Magnetic Field from Current Segments
Learning Goal: To apply the Biot-Savart law to find the magnetic field produced on the z axis from currentelements in the xy plane.
In this problem you are to find the magnetic field component along the z axis that results from various currentelements in the xy plane (i.e., at ).
The field at a point due to a current-carrying wire is given by the Biot-Savart law,
,
where and , and the integral is done over the current-carrying wire. Evaluating the vector
integral will typically involve the following steps:Choose a convenient coordinate system--typically rectangular, say with coordinate axes , , and .Write in terms of the coordinate variables and directions ( , , etc.). To do this, you must find
and . Again, finding the cross product can be done either
geometrically (by finding the direction of the cross product vector first, then checking for cancellations fromany other portion of the wire, and then finding the magnitude or relevant component) oralgebraically (by using , etc.).
Evaluate the integral for the component(s) of interest.In this problem, you will focus on the second of these steps and find the integrand for several differentcurrent elements. You may use either of the two methods suggested for doing this.
Express the magnitude of the magnetic force in terms of , , , , and .
ANSWER: =
Correct
Part C
Assuming that the charges are moving nonrelativistically ( ), what can you say about the relationshipbetween the magnitudes of the magnetic and electrostatic forces?
Hint C.1 How to approach the problem
Hint not displayed
ANSWER: The magnitude of the magnetic force is greater than the magnitude of theelectric force.
The magnitude of the electric force is greater than the magnitude of themagnetic force.
Both forces have the same magnitude.
Correct
This result holds quite generally: Magnetic forces between moving charges are much smaller thanelectric forces as long as the speeds of the charges are nonrelativistic.
Magnetic Field at the Center of a Wire LoopA piece of wire is bent to form a circle with radius . It has a steady current flowing through it in a
counterclockwise direction as seen from the top (looking in the negative direction).
What is , the z component of at the center (i.e., ) of the loop?
Hint A.1 Specify the integrand
Hint not displayed
Hint A.2 Perform the integration
Hint not displayed
Express your answer in terms of , , and constants like and .
ANSWER: =
Correct
Magnetic Field due to Semicircular WiresA loop of wire is in the shape of two concentric semicircles as shown.The inner circle has radius ; the outer circle hasradius . A current flows clockwise through the outer
wire and counterclockwise through the inner wire.
Part A
What is the magnitude, , of the magnetic field at the center of the semicircles?
Hint A.1 What physical principle to use
Hint not displayed
Hint A.2 Compute the field due to the inner semicircle
Hint A.3 Direction of the field due to the inner semicircle
Hint not displayed
Hint A.4 Compute the field due to the straight wire segments
Hint not displayed
Express in terms of any or all of the following: , , , and .
ANSWER: =
Correct
To see whether and makes sense, think of the scaling of different quantities. The
size of the current element scales as the radius, whereas the power of in the denominator is 2 (andequals the radius also, in this case). So over all, you would expect the magnetic field to scale as1/radius. Note that such an argument works only because the field due to each point is in the samedirection, so you are doing a much simpler integral.
Part B
What is the direction of the magnetic field at the center of the semicircles?
ANSWER: into the screen
out of the screen
Correct
Magnetic Field near a Moving ChargeA particle with positive charge is moving with speed along the z axis toward positive . At the time of thisproblem it is located at the origin, . Your task is to find the magnetic field at various locations in
the three-dimensional space around the moving charge.
Which of the following expressions gives the magnetic field at the point due to the moving charge?
A.
B.
C.
D.
ANSWER: A only
B only
C only
D only
both A and B
both C and D
both A and C
both B and D
Correct
The main point here is that the r-dependence is really . The results from using in the
numerator rather than the unit vector .
A second point is that the order of the cross product must be such that the right-hand rule works: Ifyour right thumb is along the direction of the current, , your fingers must curl along the direction of
the magnetic field.
Part B
Find the magnetic field at the point .
Hint B.1 Find the magnetic field direction
Hint not displayed
Express your answer in terms of , , , and , and use , , and for the three unit vectors.
Express your answer in terms of , , , , and , and use , , and for the three unit
vectors.
ANSWER: =
Correct
Part D
Find the magnetic field at the point .
Hint D.1 Evaluate the cross product
Hint not displayed
Hint D.2 Find the distance from the charge
Hint not displayed
Express your answer in terms of , , , , , and , and use , , and for the three unit
vectors.
ANSWER:
=
Correct
Part E
The field found in this problem for a moving charge is the same as the field from a current element of length carrying current provided that the quantity is replaced by which quantity?
Learning Goal: To understand the origin of the torque on a current loop due to the magnetic forces on thecurrent-carrying wires.
This problem will show you how to calculate the torque on a magnetic dipole in a uniform magnetic field. Westart with a rectangular current loop, the shape of which allows us to calculate the Lorentz forces explicitly.Then we generalize our result. Even if you already know the general formula to solve this problem, you mightfind it instructive to discover where it comes from.
Part A
A current flows in a plane rectangular current loop with height and horizontal sides . The loop is
placed into a uniform magnetic field in such a way that the sides of length are perpendicular to ,
and there is an angle between the sides of length
and .
Calculate , the magnitude of the torque about thevertical axis of the current loop due to the interactionof the current through the loop with the magneticfield.
Hint A.1 How to approach the problem
Hint not displayed
Hint A.2 Forces on the parts of the loop that have length
Hint not displayed
Hint A.3 Force on a current-carrying wire in a magnetic field
Hint A.5 Forces on the parts of the loop that have length
Hint not displayed
Express the magnitude of the torque in terms of the given variables. You will need a trigonomericfunction [e.g., or ]. Use for the magnitude of the magnetic field.
ANSWER: =
Correct
Part B
Give a more general expression for the magnitude of the torque . Rewrite the answer found in Part A interms of the magnitude of the magnetic dipole moment of the current loop . Define the angle between thevector perpendicular to the plane of the coil and the magnetic field to be , noting that this angle is the
complement of angle in Part A.
Hint B.1 Definition of the magnetic dipole moment
Hint not displayed
Give your answer in terms of the magnetic moment , magnetic field , and .
ANSWER: =
Correct
The more general vector form of this expression is.
Part C
A current flows around a plane circular loop of radius , giving the loop a magnetic dipole moment of
magnitude . The loop is placed in a uniform magnetic field , with an angle between the direction of
the field lines and the magnetic dipole moment as shown in the figure. Find an expression for the magnitudeof the torque on the current loop.
Express the torque explicitly in terms of , , , , and (where and are the magnitudes of
the respective vector quantities). Do not use . You will need a trigonomeric function [e.g..
or ].
ANSWER: =
Correct
± Magnetic Force on a Current-Carrying Wire
Learning Goal: To understand the magnetic force on a straight current-carrying wire in a uniform magneticfield.
Magnetic fields exert forces on moving charged particles, whether those charges are moving independently orare confined to a current-carrying wire. The magnetic force on an individual moving charged particle
depends on its velocity and charge . In the case of a current-carrying wire, many charged particles aresimultaneously in motion, so the magnetic force depends on the total current and the length of the wire .
The size of the magnetic force on a straight wire of length carrying current in a uniform magnetic field
with strength is
.
Here is the angle between the direction of the current (along the wire) and the direction of the magnetic
field. Hence refers to the component of the magnetic field that is perpendicular to the wire, . Thus
this equation can also be written as .
The direction of the magnetic force on the wire can be described using a "right-hand rule." This will bediscussed after Part B.
Part A
Consider a wire of length = 0.30 that runs north-south on a horizontal surface. There is a current of
= 0.50 flowing north in the wire. (The rest of the circuit, which actually delivers this current, is not
shown.) The Earth's magnetic field at this location has a magnitude of 0.50 (or, in SI units,) and points north and 38 degrees down from the horizontal, toward the ground. What is
the size of the magnetic force on the wire due to the Earth's magnetic field? In considering the agreementof units, recall that .
Express your answer in newtons to twosignificant figures.
ANSWER: 4.6×10−6
Correct
Because the Earth's magnetic field is quite modest, this force is so small that it might be hard todetect.
Part B
Now assume that a strong, uniform magnetic field of size 0.55 pointing straight down is applied. What is
the size of the magnetic force on the wire due to this applied magnetic field? Ignore the effect of the Earth'smagnetic field.
Hint B.1 Determining the angle theta
Hint not displayed
Express your answer in newtons to two significant figures.
ANSWER: 8.3×10−2
Correct
This force would be noticeable if the wire were of light weight.
The direction of the magnetic force is perpendicular to both the direction of the current flow and the directionof the magnetic field. Here is a "right-hand rule" to help you determine the direction of the magnetic force.Straighten the fingers of your right hand and pointthem in the direction of the current.Rotate your arm until you can bend your fingers topoint in the direction of the magnetic field.Your thumb now points in the direction of themagnetic force acting on the wire.
Notice that whenever the current in the wire and the magnetic field point in the same direction ( )
or in opposite directions ( ), the sine of is zero, so there is no magnetic force exerted on the
wire. This is consistent with the earlier statement that it is the component of the magnetic field that isperpendicular to the direction of the current that produces the magnetic force.Also notice that for these two special values of (when the current is flowing parallel to or antiparallel
to the magnetic field) the steps listed for the right-hand rule suggest a unique direction for the magneticforce. This is another clue that the magnetic force is zero.
A Conductor Moving in a Magnetic FieldA metal cube with sides of length is moving at velocity across a uniform magnetic field .
The cube is oriented so that four of its edges are parallel to its direction of motion (i.e., the normal vector oftwo faces are parallel to the direction of motion).
Part A
Find , the electric field inside the cube.
Hint A.1 Net force on charges in a conductor
Hint not displayed
Hint A.2 Find the magnetic force magnitude
Hint not displayed
Hint A.3 Find the magnetic force direction
Hint not displayed
Hint A.4 Determine the force due to the electric field
Express the electric field in terms of , , and unit vectors ( , , and/or ).
ANSWER: =
Correct
Now, instead of electrons, suppose that the free charges have positive charge . Examples include "holes"in semiconductors and positive ions in liquids, each of which act as "conductors" for their free charges.
Part B
If one replaces the conducting cube with one that has positive charge carriers, in what direction does theinduced electric field point?
ANSWER:
Correct
The direction of the electric field stays the same regardless of the sign of the charges that are free tomove in the conductor.Mathematically, you can see that this must be true since the expression you derived for the electricfield is independent of .Physically, this is because the force due to the magnetic field changes sign as well and causes positivecharges to move in the direction (as opposed to pushing negative charges in the direction).
Therefore the result is always the same: positive charges on the side and negative charges on
the side. Because the electric field goes from positive to negative charges will always point in
the direction (given the original directions of and ).
A Thomson ExperimentIn the late 19th century, great interest was directed toward the study of electrical discharges in gases and thenature of so-called cathode rays. One remarkable series of experiments with cathode rays, conducted by J.J. Thomson around 1897, led to the discovery of the electron.With the idea that cathode rays were charged particles, Thomson used a cathode-ray tube to measure theratio of charge to mass, , of these particles, repeating the measurements with different cathode
materials and different residual gases in the tube.
Part A
What is the most significant conclusion that Thomson was able to draw from his measurements?
ANSWER: He found a different value of for different cathode materials.
He found the same value of for different cathode materials.
From measurements of he was able to calculate the charge of an
electron.
From measurements of he was able to calculate the mass of an electron.
Correct
That the quantity was independent of the material provided clear evidence that the particles
comprising the cathode rays were, in fact, a common constituent of matter.
Imagine that you set up an apparatus to reproduce Thomson's experiment, as shown in the figure . In anhighly evacuated glass tube, a beam of electrons,each moving with speed , passes between twoparallel plates and strikes a screen at a distance
from the end of the plates.First, you observe the point where the beam strikesthe screen when there is no electric field between theplates. Then, you observe the point where the beamstrikes the screen when a uniform electric field ofmagnitude is established between the plates. Call
the distance between these two points .
Part B
What is the distance between the two points that you observe? Assume that the plates have length ,
and use and for the charge and the mass of the electrons, respectively.
Hint B.1 How to approach the problem
Hint not displayed
Hint B.2 Find the deflection at the end of the plates
Hint not displayed
Hint B.3 Find the deflection in the field-free region
Now imagine that you place your entire apparatus inside a region of magnetic field of magnitude . The
magnetic field is perpendicular to and directed
straight into the plane of the figure. You adjust thevalue of so that no deflection is observed on the
screen.What is the speed of the electrons in this case?
Hint C.1 How to approach the problem
Hint not displayed
Hint C.2 Find the magnetic force exerted on the electrons
Hint not displayed
Hint C.3 Find the electric force exerted on the electrons
Hint not displayed
Express your answer in terms of and .
ANSWER:
=Correct
Part D
In your experiment, you measure a total deflection of 4.12 when an electric field of is
established between the plates (with no magnetic field present). When you add the magnetic field asdescribed in Part C, to what value do you have to adjust its magnitude to observe no deflection?
Assume that the plates are 6.00 long and that the distance between them and the screen is 12.0 .
Now suppose you carry out a second Thomson experiment with a different beam that contains two types ofparticles. In particular, both types have the same mass as an electron, but one has charge and theother has charge . As in the previous experiment, initially only the electric field is imposed and the
deflection of the beam is observed as a spot on the screen; then, in the second phase of the experiment,one attempts to tune the magnetic field to exactly cancel the effect of the electric field.What would you observe on the screen during this experiment?
ANSWER: Two off-centered spots in both the first and the second phases of theexperiment
Two off-centered spots in the first phase of the experiment; one centered spotin the second phase of the experiment
Two off-centered spots in the first phase of the experiment; one centered andone off-centered spot in the second phase of the experiment
One off-centered spot in the first phase of the experiment; one centered andone off-centered spot in the second phase of the experiment
One off-centered spot in the first phase of the experiment; two off-centeredspots in the second phase of the experiment
One off-centered spot in both the first and the second phases of theexperiment
Correct
In the first phase of the experiment, when only the electric field is present, the particles with charge are deflected exactly as the electrons, whereas the particles with charge experience a greater
force and suffer a larger deflection. Hence, two distinct spots will be observed on the screen.In the second phase of the experiment, when a magnetic field is added, only one spot will be observedon the screen because the balance of the electric force and the magnetic force does not depend on thecharge of the particles. Thus, when the magnetic field is tuned to cancel the effect of the electric force,the beam of particles, regardless of the magnitude of their charge, will pass through the platesundeflected.
Charged Particles Moving in a Magnetic Field Ranking Task
Five equal-mass particles (A–E) enter a region of uniform magnetic field directed into the page. They followthe trajectories illustrated in the figure.
Rank from largest to smallest. To rank items as equivalent, overlap them.
ANSWER:
View Correct
Interaction of a Current Loop with a Magnetic FieldThe effects due to the interaction of a current-carrying loop with a magnetic field have many applications,some as common as the electric motor. This problem illustrates the basic principles of this interaction.
Consider a current that flows in a plane rectangular current loop with height = 4.00 and horizontal
Hint D.1 Find the direction of the forces on the parts of the loop that have length
Hint not displayed
Hint D.2 Find the direction of the forces on the parts of the loop that have length
Hint not displayed
ANSWER: Yes, the net torque acting on the loop is negative and tends to rotate the loopin the direction of decreasing angle (clockwise).
Yes, the net torque acting on the loop is positive and tends to rotate the loopin the direction of increasing angle (counterclockwise).
No, the net torque acting on the loop is zero and the loop is in equilibrium.
No, the net force acting on the loop is zero and the loop is in equilibrium.
Correct
Depending on the initial position of the loop relative to , the direction of rotation of the loop will be
different. If initially , then the net torque acting on the loop will cause the loop to rotate in
the counterclockwise direction. If instead, , then the net torque will rotate the loop in the
opposite direction.
Mass SpectrometerJ. J. Thomson is best known for his discoveries about the nature of cathode rays. Another importantcontribution of his was the invention, together with one of his students, of the mass spectrometer. The ratio ofmass to (positive) charge of an ion may be accurately determined in a mass spectrometer. In essence,the spectrometer consists of two regions: one that accelerates the ion through a potential and a second
that measures its radius of curvature in a perpendicular magnetic field.The ion begins at potential and is accelerated
toward zero potential. When the particle exits theregion with the electric field it will have obtained aspeed .
By sending atoms of various elements through a mass spectrometer, Thomson's student, FrancisAston, discovered that some elements actually contained atoms with several different masses. Atomsof the same element with different masses can only be explained by the existence of a third subatomicparticle in addition to protons and electrons: the neutron.
Motion of Electrons in a Magnetic FieldAn electron of mass and charge is moving through a uniform magnetic field in vacuum.
At the origin, it has velocity , where
and . A screen is mounted perpendicular
to the x axis at a distance from the origin.
Throughout, you can assume that the effect of gravityis negligible.
Part A
First, suppose . Find the y coordinate of the point at which the electron strikes the screen.
Hint A.1 Forces acting on electron
Hint not displayed
Hint A.2 Two-dimensional kinematics
Hint not displayed
Express your answer in terms of and the velocity components and .
ANSWER:
=
Correct
Part B
Now suppose , and another electron is projected in the same manner. Which of the following is the
most accurate qualitative description of the electron's motion once it enters the region of nonzero magneticfield?
ANSWER: The electron decelerates before coming to a halt and turning around whilealways moving along a straight line.
The electron's motion will be unaffected. (It will continue moving in a straightline with the same constant velocity.)
The electron moves in a circle in the xy plane.
The electron moves along a helical path about an axis parallel to the field lineswith constant radius and constant velocity in the x direction.
Correct
Part C
The motion of the electron can be broken down into two parts: 1. constant motion in the x direction plus 2. aperiodic part, the projection of which in the yz plane is circular. Find the angular velocity of the electronassociated with the circular component of its motion.
Hint C.1 Use Newton's 2nd law to determine the force
Hint not displayed
Hint C.2 Find the magnitude of the Lorentz force
Hint not displayed
Hint C.3 Express in terms of
Hint not displayed
Hint C.4 Express the acceleration in terms of
Hint not displayed
Express the magnitude of the angular velocity in terms of , the magnitude of the electric charge
, and other known quantities.
ANSWER:
=
Correct
A DC MotorA shunt-wound DC motor with the field coils and rotor connected in parallel (see the figure) operates from a135 DC power line. The resistance of the field
Express your answer in degrees to three significant figures.
ANSWER: 90Correct
Notice that the dot product of the velocity and the force is zero. This will always be the case. Since, must be perpendicular to both and . This result is important because it implies that
magnetic fields can only change the direction of a charged particle's velocity, not its speed.
Score Summary:Your score on this assignment is 91.3%.You received 91.33 out of a possible total of 100 points.