B for a Long, Straight Conductor, Special Case. If the conductor is an infinitely long, straight wire, θ 1 = 0 and θ 2 = π The field becomes
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1 B for a Long, Straight Conductor, Special Case If the conductor is an infinitely long, straight wire, θ 1 = 0 and θ 2 = π The field becomes μ I B = o 2πa
2 B for a Curved Wire Segment Find the field at point O due to the wire segment I and R are constants B = μ o I 4πR θ θ will be in radians
3 B for a Circular Loop of Wire Consider the previous result, with θ = 2π μ I I 2 I o μo μo B = θ = π = 4πR 4πR 2R This is the field at the center of the loop
4 B for a Circular Current Loop The loop has a radius of R and carries a steady current of I Find B at point P B x = 2 μ I R 2 o ( x + R )
5 Comparison of Loops Consider the field at the center of the current loop At this special point, x = 0 Then, B x μ I R μ I R = = 2 x 2 2 o o ( x + R ) This is exactly the same result as from the curved wire
6 Magnetic Field Lines for a Loop Figure (a) shows the magnetic field lines surrounding a current loop Figure (b) shows the field lines in the iron filings Figure (c) compares the field lines to that of a bar magnet
7 Magnetic Force Between Two Parallel Conductors Two parallel wires each carry a steady current The field B 2 due to the current in wire 2 exerts a force on wire 1 of F 1 = I 1 l B 2
8 Active Figure 30.8 (SLIDESHOW MODE ONLY)
9 Magnetic Force Between Two Parallel Conductors, cont. Substituting the equation for B 2 gives F I I 2πa μ o = l Parallel conductors carrying currents in the same direction attract each other Parallel conductors carrying current in opposite directions repel each other
10 Magnetic Force Between Two Parallel Conductors, final The result is often expressed as the magnetic force between the two wires, F B This can also be given as the force per unit length: F l B = μo I I 2πa 1 2
11 Definition of the Ampere The force between two parallel wires can be used to define the ampere When the magnitude of the force per unit length between two long parallel wires that carry identical currents and are separated by 1 m is 2 x 10-7 N/m, the current in each wire is defined to be 1 A
12 Definition of the Coulomb The SI unit of charge, the coulomb, is defined in terms of the ampere When a conductor carries a steady current of 1 A, the quantity of charge that flows through a cross section of the conductor in 1 s is 1 C
13 Magnetic Field of a Wire A compass can be used to detect the magnetic field When there is no current in the wire, there is no field due to the current The compass needles all point toward the Earth s north pole Due to the Earth s magnetic field
14 Magnetic Field of a Wire, 2 Here the wire carries a strong current The compass needles deflect in a direction tangent to the circle This shows the direction of the magnetic field produced by the wire
15 Active Figure 30.9 (SLIDESHOW MODE ONLY)
16 Magnetic Field of a Wire, 3 The circular magnetic field around the wire is shown by the iron filings
17 Ampere s Law The product of B. ds can be evaluated for small length elements ds on the circular path defined by the compass needles for the long straight wire Ampere s law states that the line integral of B. ds around any closed path equals μ o I where I is the total steady current passing through any surface bounded by the closed path. ds μ o Ñ B = I
18 Ampere s Law, cont. Ampere s law describes the creation of magnetic fields by all continuous current configurations Most useful for this course if the current configuration has a high degree of symmetry Put the thumb of your right hand in the direction of the current through the amperian loop and your fingers curl in the direction you should integrate around the loop
19 Field Due to a Long Straight Wire From Ampere s Law Want to calculate the magnetic field at a distance r from the center of a wire carrying a steady current I The current is uniformly distributed through the cross section of the wire
20 Field Due to a Long Straight Wire Results From Ampere s Law Outside of the wire, r > R Ñ B d s = B( 2πr ) = μo I μo I B = 2πr Inside the wire, we need I, the current inside the amperian circle 2 r Ñ B d s = B( 2 πr ) = μo I' I' = I 2 R μo I B= r 2 2πR
21 Field Due to a Long Straight Wire Results Summary The field is proportional to r inside the wire The field varies as 1/r outside the wire Both equations are equal at r = R
22 Magnetic Field of a Toroid Find the field at a point at distance r from the center of the toroid The toroid has N turns of wire Ñ B d s = B( 2πr ) = μon I μon I B = 2πr
23 Magnetic Field of an Infinite Sheet Assume a thin, infinitely large sheet Carries a current of linear current density J s The current is in the y direction J s represents the current per unit length along the z direction
24 Ideal Solenoid Characteristics An ideal solenoid is approached when: the turns are closely spaced the length is much greater than the radius of the turns
25 Magnetic Flux The magnetic flux associated with a magnetic field is defined in a way similar to electric flux Consider an area element da on an arbitrarily shaped surface
26 Magnetic Flux, cont. The magnetic field in this element is B da is a vector that is perpendicular to the surface da has a magnitude equal to the area da The magnetic flux Φ B is Φ B = B d A The unit of magnetic flux is T. m 2 = Wb Wb is a weber
27 Magnetic Flux Through a Plane, 1 A special case is when a plane of area A makes an angle θ with da The magnetic flux is Φ B = BA cos θ In this case, the field is parallel to the plane and Φ = 0
28 Gauss Law in Magnetism Magnetic fields do not begin or end at any point The number of lines entering a surface equals the number of lines leaving the surface Gauss law in magnetism says: B Ñ d A = 0
29 Displacement Current Ampere s law in the original form is valid only if any electric fields present are constant in time Maxwell modified the law to include timesaving electric fields Maxwell added an additional term which includes a factor called the displacement current, I d
30 Displacement Current, cont. The displacement current is not the current in the conductor Conduction current will be used to refer to current carried by a wire or other conductor The displacement current is defined as dφe Id = εo dt Φ E = E. da is the electric flux and ε o is the permittivity of free space
31 Ampere s Law General Form Also known as the Ampere-Maxwell law dφ B ( I I ) E d s = μo + d = μo I+ μoεo dt
32 Ampere s Law General Form, Example The electric flux through S 2 is EA A is the area of the capacitor plates E is the electric field between the plates If q is the charge on the plate at any time, Φ E = EA = q/ε o
33 Ampere s Law General Form, Example, cont. Therefore, the displacement current is dφe dq Id = εo = dt dt The displacement current is the same as the conduction current through S 1 The displacement current on S 2 is the source of the magnetic field on the surface boundary
34 Ampere-Maxwell Law, final Magnetic fields are produced both by conduction currents and by time-varying electric fields This theoretical work by Maxwell contributed to major advances in the understanding of electromagnetism
35 Magnetic Moments In general, any current loop has a magnetic field and thus has a magnetic dipole moment This includes atomic-level current loops described in some models of the atom This will help explain why some materials exhibit strong magnetic properties
36 Magnetic Moments Classical Atom The electrons move in circular orbits The orbiting electron constitutes a tiny current loop The magnetic moment of the electron is associated with this orbital motion L is the angular momentum µ is magnetic moment
37 Magnetic Moments Classical Atom, 2 This model assumes the electron moves with constant speed v in a circular orbit of radius r travels a distance 2πr in a time interval T The orbital speed is v = 2πr T
38 Magnetic Moments Classical Atom, 3 The current is The magnetic moment is I e = = T ev 2πr 1 μ = I A= evr 2 The magnetic moment can also be expressed in terms of the angular momentum e μ = L 2m e
39 Magnetic Moments Classical Atom, final The magnetic moment of the electron is proportional to its orbital angular momentum The vectors L and µ point in opposite directions Quantum physics indicates that angular momentum is quantized
40 Magnetic Moments of Multiple Electrons In most substances, the magnetic moment of one electron is canceled by that of another electron orbiting in the same direction The net result is that the magnetic effect produced by the orbital motion of the electrons is either zero or very small
41 Electron Spin Electrons (and other particles) have an intrinsic property called spin that also contributes to their magnetic moment The electron is not physically spinning It has an intrinsic angular momentum as if it were spinning Spin angular momentum is actually a relativistic effect
42 Electron Spin, cont. The classical model of electron spin is the electron spinning on its axis The magnitude of the spin angular momentum is 3 S = h 2 η is Planck s constant
43 Electron Spin and Magnetic Moment The magnetic moment characteristically associated with the spin of an electron has the value μ spin = eh m 2 e This combination of constants is called the Bohr magneton μ B = 9.27 x J/T
44 Electron Magnetic Moment, final The total magnetic moment of an atom is the vector sum of the orbital and spin magnetic moments Some examples are given in the table at right The magnetic moment of a proton or neutron is much smaller than that of an electron and can usually be neglected
45 Magnetization Vector The magnetic state of a substance is described by a quantity called the magnetization vector, M The magnitude of the vector is defined as the magnetic moment per unit volume of the substance The magnetization vector is related to the magnetic field by B m = μ o M When a substance is placed in an magnetic field, the total magnetic field is B = B o + μ o M
46 Magnetic Field Strength The magnetic field strength, H, is the magnetic moment per unit volume due to currents H is defined as B o /μ o The total magnetic field in a region can be expressed as B = μ o (H + M) H and M have the same units SI units are amperes per meter
47 Classification of Magnetic Substances Paramagnetic and ferromagnetic materials are made of atoms that have permanent magnetic moments Diamagnetic materials are those made of atoms that do not have permanent magnetic moments
48 Magnetic Susceptibility The dimensionless factor Χ can be considered a measure of how susceptible a material is to being magnetized M = X H For paramagnetic substances, X is positive and M is in the same direction as H For diamagnetic substances, X is negative and M is opposite H
49 Table of Susceptibilities
50 Magnetic Permeability The total magnetic field can be expressed as B = μ o (H + M) = μ o (1 + X)H = μ m H μ m is called the magnetic permeability of the substance and is related to the susceptibility by μ m = μ o (1 + X)
51 Classifying Materials by Permeability Materials can be classified by how their permeability compares with the permeability of free space (μ o ) Paramagnetic: μ m > μ o Diamagnetic: μ m < μ o Because X is very small for paramagnetic and diamagnetic substances, μ m ~ μ o for those substances
52 Ferromagnetic Materials For a ferromagnetic material, M is not a linear function of H The value of μ m is not only a characteristic of the substance, but depends on the previous state of the substance and the process it underwent as it moved from its previous state to its present state
53 Ferromagnetic Materials, cont Some examples of ferromagnetic materials are: iron cobalt nickel gadolinium dysprosium They contain permanent atomic magnetic moments that tend to align parallel to each other even in a weak external magnetic field
54 Domains All ferromagnetic materials are made up of microscopic regions called domains The domain is an area within which all magnetic moments are aligned The boundaries between various domains having different orientations are called domain walls
55 Domains, Unmagnetized Material The magnetic moments in the domains are randomly aligned The net magnetic moment is zero
56 Domains, External Field Applied A sample is placed in an external magnetic field The size of the domains with magnetic moments aligned with the field grows The sample is magnetized
57 Magnetization Curve The total field increases with increasing current (O to a) As the external field increases, more domains are aligned and H reaches a maximum at point a
58 Magnetization Curve, cont At point a, the material is approaching saturation Saturation is when all magnetic moments are aligned If the current is reduced to 0, the external field is eliminated The curve follows the path from a to b At point b, B is not zero even though the external field B o = 0
59 Magnetization Curve, final B total is not zero because there is magnetism due to the alignment of the domains The material is said to have a remanent magnetization If the current is reversed, the magnetic moments reorient until the field is zero Increasing this reverse current will cause the material to be magnetized in the opposite direction
60 Magnetic Hysteresis This effect is called magnetic hysteresis It shows that the magnetization of a ferromagnetic substance depends on the history of the substance as well as on the magnetic field applied The closed loop on the graph is referred to as a hysteresis loop Its shape and size depend on the properties of the ferromagnetic substance and on the strength of the maximum applied field
61 Example Hysteresis Curves Curve (a) is for a hard ferromagnetic material The width of the curve indicates a great amount of remanent magnetism They cannot be easily demagnetized by an external field Curve (b) is for a soft ferromagnetic material These materials are easily magnetized and demagnetized
62 More About Magnetization Curves The area enclosed by a magnetization curve represents the energy input required to take the material through the hysteresis cycle When the magnetization cycle is repeated, dissipative processes within the material due to realignment of the magnetic moments result in an increase in internal energy This is made evident by an increase in the temperature of the substance
63 Curie Temperature The Curie temperature is the critical temperature above which a ferromagnetic material loses its residual magnetism and becomes paramagnetic Above the Curie temperature, the thermal agitation is great enough to cause a random orientation of the moments
64 Domains, External Field Applied, cont. The material is placed in a stronger field The domains not aligned with the field become very small When the external field is removed, the material may retain a net magnetization in the direction of the original field
65 Table of Some Curie Temperatures
66 Curie s Law Curie s law gives the relationship between the applied magnetic field and the absolute temperature of a paramagnetic material: o M C T = B C is called Curie s constant
67 Diamagnetism When an external magnetic field is applied to a diamagnetic substance, a weak magnetic moment is induced in the direction opposite the applied field Diamagnetic substances are weakly repelled by a magnet
68 Meissner Effect Certain types of superconductors also exhibit perfect diamagnetism This is called the Meissner effect If a permanent magnet is brought near a superconductor, the two objects repel each other
69 Earth s Magnetic Field The Earth s magnetic field resembles that achieved by burying a huge bar magnet deep in the Earth s interior The Earth s south magnetic pole is located near the north geographic pole The Earth s north magnetic pole is located near the south geographic pole
70 Dip Angle of Earth s Magnetic Field If a compass is free to rotate vertically as well as horizontally, it points to the Earth s surface The angle between the horizontal and the direction of the magnetic field is called the dip angle The farther north the device is moved, the farther from horizontal the compass needle would be The compass needle would be horizontal at the equator and the dip angle would be 0 The compass needle would point straight down at the south magnetic pole and the dip angle would be 90
71 More About the Earth s Magnetic Poles The dip angle of 90 is found at a point just north of Hudson Bay in Canada This is considered to be the location of the south magnetic pole The magnetic and geographic poles are not in the same exact location The difference between true north, at the geographic north pole, and magnetic north is called the magnetic declination The amount of declination varies by location on the Earth s surface
72 Earth s Magnetic Declination
73 Source of the Earth s Magnetic Field There cannot be large masses of permanently magnetized materials since the high temperatures of the core prevent materials from retaining permanent magnetization The most likely source of the Earth s magnetic field is believed to be convection currents in the liquid part of the core There is also evidence that the planet s magnetic field is related to its rate of rotation
74 Reversals of the Earth s Magnetic Field The direction of the Earth s magnetic field reverses every few million years Evidence of these reversals are found in basalts resulting from volcanic activity The origin of the reversals is not understood
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