Title: Magnetic Field
1Magnetic Field
- A magnetic field is a region in which a body with
magnetic properties experiences a force.
2Sources of Magnetic Field
- Magnetic fields are produced by electric
currents, which can be macroscopic currents in
wires, or microscope currents associated with
electrons in atomic orbits.
3Magnetic Field Lines
- A magnetic field is visualised using magnetic
lines of force which are imaginary lines such
that the tangent at any point gives the direction
of the magnetic field at that point.
4Magnetic Flux Pattern
5The Earths Magnetic Field
- The Earth's magnetic field appears to come from a
giant bar magnet, but with its south pole located
up near the Earth's north pole.
6Properties of Magnetic Field Lines
- Magnetic lines of force never intersect.
- By convention, magnetic lines of force point from
north to south outside a magnet (and from south
to north inside a magnet). - Field lines converge where the magnetic force is
strong, and spread out where it is weak. (Number
of lines per unit area is proportional to the
magnetic field strength.)
7Magnetic flux pattern due to current in a
straight wire at right angles to a uniform field
Net flux is greater on this side of the wire
Net flux is lesser on this side of the wire
8Flemings Left Hand Rule
- If you point your left forefinger in the
direction of the magnetic field, and your second
finger in the direction of the current flow, then
your thumb will point naturally in the direction
of the resulting force!
9Force on a current-carrying conductor
- The direction of magnetic force always
perpendicular to the direction of the magnetic
field and the direction of current passing
through the conductor.
10Magnetic Flux Density
- The magnetic flux density is defined as the force
per unit length per unit current acting on a
current-carrying conductor at right angle to the
field lines.
Unit tesla (T) or gauss (G), 1 G
10-4 T or weber/m2
11Typical Values of the magnetic flux density
12Magnetic Field Measurements
- Using a current balance (d.c.)
- Using a search coil (a.c.)
- Using a Hall probe (d.c.)
13Magnetic flux density due to a straight wire
- Experiments show that the magnetic flux density
at a point near a long straight wire is
r
P ?
- TThis relationship is valid as long as r, the
perpendicular distance to the wire, is much less
than the distance to the ends of the wire.
14Calculation of B near a wire
Where ?o is called the permeability of free
space.
Permeability is a measure of the effect of a
material on the magnetic field by the material.
15Magnetic Field due to a Solenoid
- The magnetic field is strongest at the centre of
the solenoid and becomes weaker outside.
16Magnetic Flux Density due to a Solenoid
- Experiments show that the magnetic flux density
inside a solenoid is
and
So we have
or
where
17Variation of magnetic flux density along the axis
of a solenoid
- B is independent of the shape or area of the
cross-section of the solenoid. - At a point at the end of the solenoid,
18Magnetic Flux Density due to Some
Current-carrying conductors(1)
19Magnetic Flux density due to Some
Current-carrying Conductors (2)
20Force on a moving charge in a magnetic field
- The force on a moving charge is proportional to
the component of the magnetic field perpendicular
to the direction of the velocity of the charge
and is in a direction perpendicular to both the
velocity and the field.
http//webphysics.davidson.edu/physlet_resources/b
u_semester2/c12_force.html
21Right Hand Rule
- Direction of force on a positive charge given by
the right hand rule.
22Free Charging Moving in a Uniform Magnetic Field
- If the motion is exactly at right angles to a
uniform field, the path is turned into a circle.
- In general, with the motion inclined to the
field, the path is helix round the lines of
force.
23Mass Spectrometer
- The mass spectrometer is used to measure the
masses of atoms.
- Ions will follow a straight line path in this
region.
- Ions follow a circular path in this region.
24Aurora Borealis (Northern Lights)
- Charged ions approach the Earth from the Sun (the
solar wind and are drawn toward the poles,
sometimes causing a phenomenon called the aurora
borealis.
25Causes of Aurora Borealis
- The charged particles from the sun approaching
the Earth are captured by the magnetic field of
the Earth. - Such particles follow the field lines toward the
poles. - The high concentration of charged particles
ionizes the air and recombining of electrons with
atoms emits light.
http//www.exploratorium.edu/learning_studio/auror
as/selfguide1.html
26Hall Effect
- When a current carrying conductor is held firmly
in a magnetic field, the field exerts a sideways
force on the charges moving in the conductor. - A buildup of charge at the sides of the conductor
produces a measurable voltage between the two
sides of the conductor.
- The presence of this measurable transverse
voltage is called the Hall effect.
27Hall Voltage
- The transverse voltage builds up until the
electric field it produces exerts an electric
force on the moving charges that equal and
opposite to the magnetic force. - The transverse voltage produced is called the
Hall voltage.
28Charge Carriers in the Hall Effect
- The Hall voltage has a different polarity for
positive and negative charge carriers. - That is, the Hall voltage can reveal the sign of
the charge carriers.
29Hall Probe
- Basically the Hall probe is a small piece of
semiconductor layer.
- Four leads are connected to the midpoints of
opposite sides.
- When control current IC is flowing through the
semiconductor and magnetic field B is applied,
the resultant Hall voltage VH can be measured on
the sides of the layer.
30Force between two parallel current-carrying
straight wires (1)
- Parallel wires with current flowing in the same
direction, attract each other. - Parallel wires with current flowing in the
opposite direction, repel each other.
31Force between two parallel current-carrying
straight wires (2)
- Note that the force exerted on I2 by I1 is equal
but opposite to the force exerted on I1 by I2.
32Definition of the ampere
- The ampere is the constant current which, if
maintained in two parallel conductors of infinite
length, of negligible cross-section, and placed
one metre apart in a vacuum, would produce
between these conductors force of 2 x 10-7 N per
metre of length.