Electricity: Electromagnetism
Electromagnetism: Problem Set Overview
We are planning 12 problem sets on the topic of Electromagnetism. Most problems are multipart problems requiring an extensive analysis. The problems target your ability to apply concepts of elctric circuits and magnetic fields in order to analyze situations in which a moving charge induces a magnetic effect or a magnetic field induces a current in a wire.
The Origin of Magnetic Fields and Forces
Magnetic fields are produced by certain elements in nature. There are 4 levels of scale from smallest to largest that the element must satisfy for the object to display a magnetic field around it: 1) particle, 2) atom, 3) crystal structure, 4) domain.
 Charged Particle:
Electrons orbiting the nucleus are tiny magnets due to their motion and a quantum property called spin. It gives the particle a tiny magnetic field called a magnetic moment. In a broader sense, spin is an essential property influencing the ordering of electrons and nuclei in atoms and molecules. The spin state can be either up or down. Protons also have the magnetic property of spin, but it is about 1000 times less in magnitude compared to the electron’s spin.
 Atom:
Atoms have many electrons orbiting the nucleus that fill orbitals. Electrons in a specific orbital pair up and in general, each electron pair consists of an up and a down spin characterisitc that cancels out any overall magnetic effect. Therefore, atoms with halffilled outer shells have the best chance of being effectively magnetic.
 Crystal Structure:
Many elements form solids with atoms arranged in a crystal structure. This is defined as a particular repeating arrangement of atoms (molecules or ions) throughout the element. The atoms will arrange in a way that requires the lowest amount of energy, making it the most stable. In most of these arrangements the magnetic fields will be minimized.
 Domain:
Materials are made of sections of atoms with magnetic fields aligned. These sections are called domains. When one particular domain direction dominates the material, it will exhibit the physical characteristic of magnetism on a large scale.
Analyzing the periodic table and considering these 4 conditions, only iron, cobalt, and nickel are naturally occuring magnets at room temperature.
Any object able to create a magnetic field has polarity, producing north and south poles. Bar magnets create magnetic fields by having opposite poles (north and south) as shown at right. The direction of the field is the direction the north pole of a compass needle points at that location.
If 2 poles are sufficiently small and far apart, they can be considered point magnetic charges. The force between 2 magnetic points is much like the Coulomb Force Law between charges and Newton’s Universal Law of Gravity between masses:
where p_{1} and p_{2} are the magnitudes of the magnetic charges.
SI unit: Ampere•meter
In this case,
where µ = 4•π x 10^{7} T•m/A
and is the permeability of the intervening medium.
SI unit: Tesla•meter/Ampere
There is rarely a scenario where this is the case since monopoles don’t exist in nature. Complicated calculations have been developed for more common situations such as the force between 2 nearby magnetized surfaces, 2 nearby bar magnets, or 2 nearby cylindrical magnets. These situations are beyond the scope of these problems. A more common and useful way to produce a magnetic field is to set up a current in a wire. This magnetic field is observed since the current can put a force on a nearby magnet or moving charge.
There is disagreement about whether the Magnetic Field is fundamental to nature since the magnetic field can be viewed as an Electric Field in a certain frame of reference. This is like the “centrifugal” force and “Coriolis” force in that these forces are only observed in a specific (noninertial) frame of reference.
Claim 1: The magnetic field is not fundamental and that can be seen when investigating the magnetic field created by a current. Let’s look at how a charge is affected by the current in a wire in the table below
from the frame of reference of the charged particle outside the wire.
Case I: If the charged particle is not moving the equal number of protons and moving electrons equally spaced in the wire produce a net electric field of 0, thereby not affecting any nonmoving charged particles.
Case II & III: If the charged particle is moving parallel to the current then the concept of Special Relativity becomes relevant. In relative motion between the charged particle and the charges in the wire, the charge and quantum spin of any of the particles does not change (invariant). But what can change due to the relative motion between the charged particle and the charges in the wire (
from the frame of reference of the charged particle) is space (length, distance, area, volume) among other physical characteristics.
Consider the following cases in the frame of reference of the positively charge particle:



Claim 2: The Magnetic Field is fundamental as best stated by Dr. Christopher S. Baird of West Texas A&M University below:
The correct statement is that electric fields and magnetic fields are both fundamental, both are real, and both are part of one unified entity: the electromagnetic field. Depending on what reference frame you are in, a particular electromagnetic field will look more electric and less magnetic, or more magnetic and less electric. However, this does not change the fact that they are both fundamental and both part of the same unified entity. A purely electric field as viewed in one inertial frame is part electric and part magnetic in all other reference frames. Similarly, a purely magnetic field as viewed in one inertial frame is part electric and part magnetic in all other reference frames. The magnetic field is not just a relativistic version of the electric field, and the electric field is not just a relativistic version of the magnetic field. Rather, the unified electromagnetic field is innately and selfconsistently relativistic.
Though the generation of the magnetic field at the atomic level is complex we can analyze and make use of the behavior at the human scale and in the human frame of reference. The outcomes that we are concerned with are the following:
 A current (moving charge) in a wire produces a magnetic field around the wire.
 A stationary charged particle is not affected by a magnetic field.
 A moving charged particle feels a force from a magnetic field.






The Magnetic Field Definition due to a Magnetic Force
It is found experimentally that the strength of the magnetic force on a moving charged particle is proportional to the magnitude of the charge, q , the magnitude of the velocity v, the strength of the external magnetic field, B, and the sine of the angle, Θ, between the direction of v and B as shown at right. This can be written as a cross product between v and B:
This expression is rearranged to define the magnitude of the magnetic field as the following:
SI unit: Tesla
The direction of the magnetic field is determined by the righthand rule as shown in the diagram.
The Magnetic Force on a Current in a Wire
The magnitude of the force from a magnetic field on a current in a wire can be analyzed by rewriting the equation for Force from the reference frame of a point in the wire where L is the length of the wire, Δq/Δt is the charge flow and B is the magnetic field as shown at right as follows:
where I is the current in the wire and the direction is determined by the righthand rule between conventional current, I, and magnetic field, B.
The Magnetic Force on the Current in a Loop
The previous result can be used to analyze the force on a current in the shape of a rectangular loop as shown at right.
The current in the top and bottom sides of the loop is parallel to the Bfield so the force from
F = a*I X B = a*I•*B*sin(0°) = 0
The current in the left and right sides of the loop is perpendicular to the Bfield so the result from F = b*I X B is
F = b*I•*B*sin(90°) = b*I*B
The direction is obtained from the righthand rule for cross products. The resulting forces are shown below from the eye’s view looking at the edge of the loop from the end position:
Since the forces do not go through the center of the loop a torque is produced that causes the loop to rotate about the center axis. The edge view reveals that the angle between the plane of the loop and the Bfield, α, changes over time as shown below right.
The torque at any loop position about the center axis due to one force will be τ = r X F. Since r = a/2, F = b*I*B from above, and there are 2 identical forces, the net torque will be
When the loop is horizontal Θ = 90°, making the net Torque value a maximum of τ_{max} = a*b*I*B.
A Magnetic Force Outcome; Hall Effect
When a flow of electrons moves through a wire in a magnetic field the charges are separated in the wire by the righthand rule of F = q*v X B, where v is the drift velocity shown at right. This force on the electrons moves the negative charges to the bottom leaving positive charges near the top. This charge separation then sets up an Efield directed downward (called the Hall field) that puts a force on the moving electrons upward. Establishing equilbrium between these 2 forces prduces the following relationship:
F_{net} = 0 = q*E_{Hall}  q*v_{drift}*B
and rearranging gives
E_{Hall} = v_{drift}*B
From previous studies regarding separation of charge due to parallel plates the Potential Difference across the wire can be calculated by using ΔV = E*d. In this case, that Potential Difference is called the Hall emf:
ε_{Hall} = E_{Hall}*d = v_{drift}*B*d
A Magnetic Force Outcome; Mass Spectrometry:
A flow of ions can be accelerated to a velocity, v, and sent through a set of parallel plates as shown at right. Opposing forces from the Efield and Bfield are established with only ions having a certain velocity going straight through (F_{net} = 0) due to the relationship:
q*E = q*v*B_{1}
and rearranging gives
v = E / B_{1}.
These ions then enter another area having a magnetic field where they experince Uniform Circular Motion. Newton’s 2^{nd} Law gives the following result:
F = q*v*B_{2} = m•v^{2} / r
Rearranging gives
and substituting for v gives
This result can be used to measure the mass of the ion.
The Magnetic Field Determined using Ampere’s Law
In electrostatics a charge that feels a force in an electric field also produces an electric field. In the same way a moving charge in a wire that feels a force from a Bfield also generates a Bfield of its own. This Bfield can be determined using calculus and Ampere’s Law for moving charges
The result for the current in the wire at right using Ampere’s Law is the following:
where µ_{o} = 4•π•10^{7} T*m/A
I_{enclosed} is is the current in the wire, and
r is the distance from the wire to the location of interest.
The Magnetic Field created by the Current in a Solenoid
A long coil of wire consisting of many loops is called a solenoid as shown at right. Applying the righthand rule to determine Bfield lines when a current is sent through the wire gives the result that the Bfield is reinforced in the center of the coil and not reinforced between the individual coils or immediately outside the coils.
A solenoid acts like a bar magnet in that when current flows it has a north pole and a south pole, depending on the direction of the current. If the solenoid is very long in comparison to its diameter and the coils are tightly packed together, the field inside a solenoid is very nearly uniform in both direction and strength.
A solenoid cut in half with current shown in the coils is shown below.
Ampere’s Law
can be used on a section of coils on one side of the solenoid as shown above using the dotted rectangle (N=4 loops) to determine the magnitude of the Bfield. The closed surface must be analyzed on all sides. Sides 23 and 41 are perpendicular to the Bfield so no contribution will occur due to the dot product giving a cos (90˚) = 0. Side 34 has such a small Bfield due to canceling effects from all coils so it will not contribute. The only side needing to be evaluated is side 12. The result is the following:
B * L = µ_{o} * I_{enc}
where I_{enc} = N* I,
µ_{o} = 4•π•10^{7} T*m/A, and
L is the length of the rectangle.
Therefore, the Bfield produced by any solenoid can be calculated by using
where n = N / L, the number of loops per unit length.
The Magnetic Field created by the Current in a Toroid
A long coil of wire consisting of many loops bent into the shape of a circle is called a toroid as shown at right. Ampere’s Law
can be applied to the 3 pathways shown. Since there is no current inside Path 1 the Bfield there is 0. Since the current flows into and out of the screen as shown at bottom right inside Path 3 the total current is 0 so the Bfield there is 0.
Only in Path 2 do you get a current in one direction that qualifies for I_{enc} as part of Ampere’s Law. The result for Path 2 then will be the following:
B*2*π*r = µ_{o} * N * I
where N*I is the number of loops times the current.
The magnetic field is uniform within the toroid if the radius of the center of the ring, r, is large relative to the width of the ring. Solving for the Bfield magnitude then gives
where n = N / 2 π r, the number of loops per unit length.
The Magnetic Flux
In the 1800’s Michael Faraday used the setup above to perform the following experiments:
Because of the brief occurences of current in the secondary coil, it was concluded that a changing magnetic field in the ring produced an electric field in the secondary coil as though a source of potential difference [referred to as an induced emf (electromotive force)] was connected to it for a short period of time.
To study this phenomenon, the Magnetic Flux, Φ_{B}, that is a measure of the strength of the magnetic field, B, passing through a specific crosssectional area, A, is defined. It can be written as
Φ_{B} = B_{perpendicular} * A = B*A*cos Θ
SI unit: Weber (Wb)
B_{perpendicular} is the component of B perpendicular to the plane of the loop as shown at right.
Faraday’s Law of Induction
It has been determined that an emf (electromotive force) is induced in a circuit whn the magnetic flux through the circuit changes with time. The relationship between the change in flux and the emf is referred to as Faraday’s law of Magnetic Induction and written as follows:
where N would be the number of tightly wound loops that experience the change in magnetic flux, ΔΦ_{B}, during the time interval, Δt. The negative sign is used to determine the polarity of the induced emf. This is determined using Lenz’s Law stated as follows:
Lenz’s Law: The current caused by the induced emf travels in the direction that creates a magnetic field with flux opposing the change in the original flux through the circuit.
The creation of an emf due to a decreasing Bfield is described in the table below:
The creation of an emf due to an increasing Bfield is described in the table below:
The creation of an emf due to a moving conductor and/or changing area in a magnetic field is called Motional emf. Let’s look at 2 scenarios below.
Scenario 1:Moving conductor:
Conducting bar moving in a magnetic field as shown at right. A force due to the motion of charged particles is exerted on the charges in the bar,
F = q*v X B, causing a separation of charge by forcing negative electrons to move to the bottom of the bar according to the righthand rule. This sets up an electric field pointing downwards in the conductor. Charge stops moving in thhe bar when the force due to the electric field matches the opposing force due to the magnetic field. Therefore,
F_{e} = F_{B}, and with substitution becomes
q*E = q*v*B, giving
E = v*B.
Like the capacitor, the potential difference (in this case the
emf) set up by the separation of charge for the uniform electric field is
E*L, so that the emf is the following:
ε = B*L*v .
Scenario 2: Changing Area:
Consider a conducting bar experiencing an applied force, F_{a}, to the right in a magnetic field as shown at right. A force due to the motion of charged particles is exerted on the charges in the bar, F = q*v X B, causing a counterclockwise conventional current in the closed conductive pathway by the dotted red lines. The continual movement of the charge upwards in the moving bar causes the bar to experience a force, F_{B}, to the left due to F = q*v X B, applying the righthand rule.
Therefore, an induced emf will be set up to oppose this increasing area and can be calculated using a change in Magnetic Flux. Consider the change in area shown at right with the bar covering a distance, Δx,in a time of Δt. Using Faraday’s Law of Induction
where N= 1 becomes
and since ΔA = L*Δx,
and since v = Δx/Δt, then the magnitude of the emf is: ε = B*L*v .
Equation Summary
Habits of an Effective ProblemSolver
An effective problem solver by habit approaches a physics problem in a manner that reflects a collection of disciplined habits. While not every effective problem solver employs the same approach, they all have habits which they share in common. These habits are described briefly here. Effective problemsolvers ...
 ...read the problem carefully and develops a mental picture of the physical situation. If needed, they sketch a simple diagram of the physical situation to help visualize it.
 ...identify the known and unknown quantities in an organized manner, often times recording them on the diagram itself. They equate given values to the symbols used to represent the corresponding quantity (e.g., F = 0.025 N, E = 4.50x10^{6} N/C, q = ???).
 ...plot a strategy for solving for the unknown quantity. The strategy will typically center around the use of physics equations and is heavily dependent upon an understanding of physics principles.
 ...identify the appropriate formula(s) to use, often times writing them down. Where needed, they perform the needed conversion of quantities into the proper unit.
 ...perform substitutions and algebraic manipulations in order to solve for the unknown quantity.
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