Chapter 27 sources of the magnetic field
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Chapter 27 Sources of the magnetic field. Point Object Force. Point Object Field. Force Equation. Differential Field. Are B, dB radial?. Do B, dB have 1/r 2 dependence?. Magnetic field of point charges. Magnitude ~ 1/r 2. Constants.

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Chapter 27 Sources of the magnetic field

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Chapter 27 sources of the magnetic field

Chapter 27 Sources of the magnetic field

Point

Object

Force

Point

Object

Field

Force

Equation

Differential

Field

Are B, dB radial?

Do B, dB have 1/r2 dependence?


Magnetic field of point charges

Magnetic field of point charges

Magnitude ~ 1/r2

Constants

mo = permeability of free space = 4p x 10-7 N/A2

Direction


Right hand rule

Right Hand Rule


Cross product review

Cross product review


Chapter 27 sources of the magnetic field

q = 4.5 mC

  • What is the direction of the Magnetic Field at the origin?

  • What is the magnitude of the magnetic field at the origin?

  • What if the charge was orbiting the origin?

-3.2 x 10-14 T


Biot savart law set up

Biot-Savart Law – Set-Up

  • The magnetic field is dB at some point P

  • The length element is dl

  • The wire is carrying a steady current of I


Biot savart law

Biot-Savart Law

Permeability of free space

For a long Wire:

ds


Magnetic field of a long wire

Magnetic field of a long wire


Magnetic field due to a straight wire

Magnetic field due to a straight wire

Compare with:


Force between two parallel wires

Force between two parallel wires

R


Force between two parallel wires1

Force between two parallel wires

If the currents are in the same direction, the force is attractive.

If the currents are in the opposite direction, the force is repulsive.


Historical definition of the ampere

Historical definition of the Ampere

If 2 long parallel wires 1.0 m apart have the same current in them and the force per unit length on each wire is 2.0 x 10-7 N/m, the current is 1.0 Ampere

Historical definition of the Coulomb

If the current is 1.0 Ampere, then 1.0 Coulomb is the amount of charge passing through a cross section in 1 second.


B for a curved wire segment

B for a Curved Wire Segment

  • Find the field at point O due to the wire segment

  • I and R are constants

    q will be in radians


Chapter 27 sources of the magnetic field

5.Determine the magnetic field at a point P located a distance x from the corner of an infinitely long wire bent at a right angle, as shown in Figure P30.5. The wire carries a steady current I.

7. The segment of wire in Figure P30.7 carries a current of I = 5.00 A, where the radius of the circular arc is R = 3.00 cm. Determine the magnitude and direction of the magnetic field at the origin.

10. A very long straight wire carries current I. In the middle of the wire a right-angle bend is made. The bend forms an arc of a circle of radius r, as shown in Figure P30.10. Determine the magnetic field at the center of the arc.


Magnetic field due to a current loop

Magnetic field due to a current loop

The perpendicular components cancel by symmetry.


Helmholtz coils

Helmholtz Coils

One Coil:

R

Two Coils:

R

At x~R/2


Magnetic field due to a current loop1

Magnetic field due to a current loop

At the center:

Magnetic dipole moment vector for a single loop:

When x>>R:


Comparison to an electric dipole

Comparison to an electric dipole

-q

+

q

Biot-Savart Law:


Chapter 27 sources of the magnetic field

  • Two long, parallel conductors, separated by 10.0 cm, carry currents in the same direction. The first wire carries current I1 = 5.00 A and the second carries I2 = 8.00 A. (a) What is the magnitude of the magnetic field created by I1 at the location of I2? (b) What is the force per unit length exerted by I1 on I2? (c) What is the magnitude of the magnetic field created by I2 at the location of I1? (d) What is the force per length exerted by I2 on I1?

18.Two long, parallel wires are attracted to each other by a force per unit length of 320 μN/m when they are separated by a vertical distance of 0.500 m. The current in the upper wire is 20.0 A to the right. Determine the location of the line in the plane of the two wires along which the total magnetic field is zero.

63. Two long, parallel conductors carry currents in the same direction as shown in Figure P30.63. Conductor A carries a current of 150 A and is held firmly in position. Conductor B carries a current IB and is allowed to slide freely up and down (parallel to A) between a set of nonconducting guides. If the mass per unit length of conductor B is 0.100 g/cm, what value of current IB will result in equilibrium when the distance between the two conductors is 2.50 cm?


Introduction to ampere s law

Introduction to Ampere’s Law

Recall the definition of electric potential:

What is the value of the integral over a closed path for any electric field?

Let’s try the same thing for a magnetic field around a current carrying wire.


Ampere s law

Ampere’s Law

  • The integral is around any closed path

  • The current is that passing through the surface bounded by the path

  • Like Gauss’s Law, useful in finding fields for highly symmetric problems

This result has been shown experimentally to be true in general


Applying ampere s law

Select a surface

Try to imagine a surface where the electric field is constant everywhere. This is accomplished if the surface is equidistant from the charge.

Try to find a surface such that the electric field and the normal to the surface are either perpendicular or parallel.

Determine the charge inside the surface

If necessary, break the integral up into pieces and sum the results.

Select a path

Try to imagine a path where the magnetic field is constant everywhere. This is accomplished if the surface is equidistant from the charge.

Try to find a path such that the magnetic field and the path are either perpendicular or parallel.

Determine the current inside the surface

If necessary, break the integral up into pieces and sum the results.

Applying Ampere’s Law


Example magnetic field inside a wire

Example: Magnetic field inside a wire


Example solenoid

Example: Solenoid


Example solenoid1

Example: Solenoid

0

0

small


Example toroid

Example: Toroid

Inside:

Outside:


Chapter 27 sources of the magnetic field

21.Four long, parallel conductors carry equal currents of I = 5.00 A. Figure P30.21 is an end view of the conductors. The current direction is into the page at points A and B (indicated by the crosses) and out of the page at C and D (indicated by the dots). Calculate the magnitude and direction of the magnetic field at point P, located at the center of the square of edge length 0.200 m.

29. A long cylindrical conductor of radius R carries a current I as shown in Figure P30.29. The current density J, however, is not uniform over the cross section of the conductor but is a function of the radius according to J = br, where b is a constant. Find an expression for the magnetic field B (a) at a distance r1 < R and (b) at a distance r2 > R, measured from the axis.

24. The magnetic field 40.0 cm away from a long straight wire carrying current 2.00 A is 1.00 μT. (a) At what distance is it 0.100 μT? (b) What If? At one instant, the two conductors in a long household extension cord carry equal 2.00-A currents in opposite directions. The two wires are 3.00 mm apart. Find the magnetic field 40.0 cm away from the middle of the straight cord, in the plane of the two wires. (c) At what distance is it one tenth as large? (d) The center wire in a coaxial cable carries current 2.00 A in one direction and the sheath around it carries current 2.00 A in the opposite direction. What magnetic field does the cable create at points outside?


Magnetic flux

Magnetic Flux

  • 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 FB is

  • The unit of magnetic flux is T.m2 = Wb

    • Wb is a weber


Gauss law in magnetism

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:


Displacement current

Displacement Current

  • Ampere’s law in the original form is valid only if any electric fields present are constant in time

  • Maxwell added an additional term which includes a factor called the displacement current, Id

  • 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


Ampere s law general form

Ampere’s Law – General Form

  • Also known as the Ampere-Maxwell law

  • Magnetic fields are produced both by conduction currents and by time-varying electric fields


Material magnetism

Material Magnetism

Empty core magnetic field

  • Ferromagnetic – Fe, Co, Ni - susceptability is large and positive

  • Paramagnetic – Al, Mg – susceptability is small and positive

  • Dimagnetic – Cu, Au, Ag, Pb – suceptabiltiy is small and negative

Magnetic field in the solenoid changes due to the tendency of the dipoles to align and strengthen the field

susceptability


Magnetization vector

Magnetization Vector

  • Defined to describe what is happening in the material as a result of the external applied field.


Dielectrics

Dielectrics

  • A dielectric is a nonconducting material that, when placed between the plates of a capacitor, increases the capacitance

    • Materials with Dipoles that can align with an external electric Field. Dielectrics include rubber, plastic, and waxed paper

-

-

+ +

-

+ +

+

-

-

+

-

k is the Dielectric Constant

Measure of the degree of dipole alignment in the material


Ferromagnetism

Ferromagnetism

  • Domains

  • Curie Temperature

  • Hysteresis

Dipoles are random

at higher temperatures

Curie’s Law


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