phy13 lesson 1 magnetism
DESCRIPTION
magnetismphysicsTRANSCRIPT
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MAGNETIC FIELD ANDMAGNETIC FORCES
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MAGNETISM: Properties of Magnets
1. If a permanent bar magnet is free to rotate, one end would point north – this is the north pole or N-pole.
2. Like poles of two magnets repel and unlike poles attract.
to northpole
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3. If a permanent bar magnet is cut, it forms two smaller magnets each with its own N and S poles.*
*A magnetic monopole has not been observed in nature.
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THE EARTH AS A MAGNET
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The Earth's magnetic field is caused by electric currents in the liquid outer core.
magnetic inclination – angle of the magnetic field line with the surface of the earth.
Earth's magnetic field is tilted with respect to the planet's spin axis by about 11°.
The magnetic field is near horizontal at the equator and vertical at the poles.
The magnetic field of the earth ranges from 30T to 60 T.
magnetic declination – the deviation of the magnetic axis from the geographic axis.
THE EARTH AS A MAGNET
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MAGNETISM AND ELECTRICITY
Hans Christian Oersted (1777-1851) Danish physicist and chemist who “accidentally” discovered the relationship between electricity and magnetism.
In 1820, Oersted discovered that the needle of a magnetic compass is deflected by a current-carrying conductor.
In 1824, Michael Faraday discovered that a moving magnet near a conducting loop produces current in the loop.
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A moving charge or current creates a magnetic field in the surrounding space (in addition to its electric field).
The magnetic field exerts a magnetic force on any other moving charge or current that is present in the field.
Magnetic field is a vector field, the direction of which is the direction which the N-pole of a compass needle tends to point.
For a permanent magnet, the magnetic field points out of its N-pole and into its S-pole.
MAGNETIC FIELD ( B )
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EXPERIMENTAL OBSERVATIONS ON MAGNETIC FORCE ON MOVING ELECTRIC CHARGES.
A charged particle at rest experiences no magnetic force.
4. The magnetic force F is always perpendicular to both B and v.
1. The magnitude of the magnetic force F is directly proportional to the charge q.
F |q |2. The magnitude of the magnetic force F is directly
proportional to the magnitude of the magnetic field B.
F B3. The magnitude of the magnetic force F is directly proportional to the particle’s velocity v.
F v
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MAGNETIC FORCES ON MOVING CHARGES
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THE RIGHT-HAND RULE
V
B
F
The thumb points to the direction of the charged particle’s velocity v.
The index finger points to the direction of the magnetic field B.
The middle finger points to the direction of the magnetic force acting on the charge F.
directions of vectors:
xaway from observer:
toward the observer:
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MAGNETIC FORCES ON MOVING CHARGES
BvqF ||
sin|| BvqF
BvqF
units of B:
)(111 TteslaAm
N
C
N
sm
teslaGgauss 410)(1
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Example 1. A beam of protons ( q = 1.6 x 10-19 C ) moves at 3.0 x 10 5 m/s through a uniform magnetic field with a magnitude 2.0 T that is directed along the +z-axis. The velocity of each proton lies in the xz-plane at an angle of 30o to the +z-axis. Find the magnitude and direction of the force on a proton.
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Example 1. A beam of protons ( q = 1.6 x 10-19 C ) moves at 3.0 x 10 5 m/s through a uniform magnetic field with a magnitude 2.0 T that is directed along the +z-axis. The velocity of each proton lies in the xz-plane at an angle of 30o to the +z-axis. Find the magnitude and direction of the force on a proton.
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Example 1. A beam of protons ( q = 1.6 x 10-19 C ) moves at 3.0 x 10 5 m/s through a uniform magnetic field with a magnitude 2.0 T that is directed along the +z-axis. The velocity of each proton lies in the xz-plane at an angle of 30o to the +z-axis. Find the magnitude and direction of the force on a proton.
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MAGNETIC FIELD LINES
Magnetic field lines show the direction of the magnetic field at any point in the field.
• the line through any point is tangent to the magnetic field vector.• where field lines are close together, the magnetic field magnitude is greater.
• magnetic field lines never intersect.
• the direction of the magnetic field points away from N- pole and toward S-pole.
• magnetic field lines have no ends.
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MAGNETIC FIELD LINES
(a) C-shaped magnet
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MAGNETIC FIELD LINES
(b) Straight Wire
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MAGNETIC FIELD LINES
(c) Coil (d) Solenoid
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MAGNETIC FLUX (B)magnetic flux – is a measure of the amount of magnetic field passing through a given surface.
Consider a surface area A divided into area elements dA. Determine the component of the magnetic field perpendicular to the area element.
AdBd B
dABd B cos
The magnetic flux on the area element is
where is the angle between B and the area vector A.
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MAGNETIC FLUX (B)
AdBB cosBdAB
The magnetic flux for the whole area is
For a regularly-shaped area: cosBAB
Maximum magnetic flux: BAB unit: )(2 WbweberTm
AB B
Magnetic Flux Density – another term for magnetic field.
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GAUSS’S LAW FOR MAGNETISM
0dAB
The total magnetic flux through a closed surface is zero.
(for any closed surface )
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MOTION OF CHARGED PARTICLES IN A MAGNETIC FIELD
LCENTRIPETAMAGNETIC FF
R
mvqvB
2
qB
mvR
Radius of circular orbit in magnetic field:
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MAGNETIC FORCE ON A CURRENT-CARRYING CONDUCTOR
sinBvqF
sinBt
lqF
sinBlt
qF
I
I
sinBlIF
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MAGNETIC FORCE ON A STRAIGHT CONDUCTOR
I
I
sinBlIF
BlIF
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Example 2. A straight horizontal copper rod carries a current of 50.0 A from west to east in a region between the poles of a large electromagnet. In this region, there is a horizontal magnetic field in the direction 45o NE with a magnitude of 1.20 T. Find the magnitude and direction of the force on a 1.00-m section of the rod.
sinBlIF 45sin)20.1)(00.1)(50( TmAF
upwardNF ,4.42
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sinBdlIdF
MAGNETIC FORCE ON A CONDUCTOR
BldIFd
For any conductor (straight or not), divide it into infinitesimal segments dl.
sinBdlIF
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Example 3. Find the total magnetic force on a composite conductor carrying a current I (see figure below).
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0 BlIF A
jILBBLIF B
semicircle portion (FC ):
BdlIdF
BRdIdF
cosBRdIdFx
sinBRdIdFy
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0cos0
dRBIFx
0sin dRBIFy
IRBRBIFy 2)]0cos()cos[(
jIRBF C 2
jIRBjILBFFFF CBA 20
jRLIBF )2(
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B is eastward.
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(a)
x
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(b)
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MAGNETIC TORQUE Consider a wire loop carrying a current I inside a
uniform magnetic field of magnitude B.
BIL
W
axis
Fx
F
B
F
Ix
F
W/2 W/2
axis
Fr 22 WF
2)(2 WILB
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MAGNETIC TORQUE
B
F
Ix
F
W/2 W/2
axis 2)(2 WILB
LWIB)(
BIA
If the current loop has N number of turns
NBIA
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MAGNETIC TORQUE
BIAmax
When the magnetic field and the area vector are perpendicular, the magnetic torque is maximum.
B
F
Ix
F
W/2 W/2
A
B
F
I
x
F
A
sin2
W sinBIA
If the angle between the magnetic field and the area vector is , the magnetic torque is
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MAGNETIC MOMENT
AI
The product IA is called the magnetic moment (which is a vector whose direction is that of the area vector).
sinB
B
B
F
I
x
F
sin2
W
Magnetic torque tends to rotate the loop in the direction of decreasing .
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ELECTRIC MOTOR
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ANSWER: 0.024 T, +y direction
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ANSWERS: (a) 0.030 T, +j(b) 0.017 T, -j