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Transcript
Eventually transatlantic signals!
From Last Time…
• Electromagnetic waves
Capacitor
banks
Induction
coils
• Charges, current and forces: Coulomb’s law.
Spark gap
• Accelerating charges produce
an electromagnetic wave
• The idea of the electric field.
Today…
Electric fields, magnetic fields, and their
unification
Mon. Feb 20, 2006
Gulgielmo Marconi’s transatlantic transmitter
Phy107 Lecture 14
1
Mon. Feb 20, 2006
Electromagnetic Waves
Phy107 Lecture 14
2
The idea of electric fields
y
z
x
• EM wave made up of
oscillating electric and magnetic fields.
• But what is an electric field?
• Electric and magnetic fields are perpendicular to
propagation direction
• Electric field is a way to describe the force
on a charged particle due to other charges
around it.
• Can travel in empty space
• Force = charge × electric field
f = v/λ
• The direction of the force is the direction of
the electric field.
• A Transverse wave.
v = c = 3 x 108 m/s (186,000 miles/second!)
Mon. Feb 20, 2006
Phy107 Lecture 14
3
Mon. Feb 20, 2006
Question
Phy107 Lecture 14
4
The electric field
Force on this charge…
• Direction of force between two particles of
the same charge (use next slide).
Q2
+
+
F=k
+
Q1Q2
r2
Q1
…due to this charge
!
Force = (Charge) " (Electric field)
+
+
!
Mon. Feb 20, 2006
Phy107 Lecture 14
5
Mon. Feb 20, 2006
Phy107 Lecture 14
6
1
Visualizing the electric field
Why bother?
• Faraday invented the idea of field lines
following the force to
visualize the electric field.
• Why invent fields - why not just use forces?
Local electric field is same
direction as field lines.
Force is parallel or antiparallel
to field lines.
Charged particle will move
along these field lines.
• Think of the EM wave. A spark is an accelerating
current flow, producing the wave.
• The wave continues to propagate
even when the spark is gone.
• No charges anywhere,
but time-varying fields propagate as a wave.
Field lines emanate from
positive charge and terminate
on negative charge.
Mon. Feb 20, 2006
Phy107 Lecture 14
7
Electric field: summary
Mon. Feb 20, 2006
Phy107 Lecture 14
8
But wait… there’s more
• Energy can be stored in the field.
• Presence of electric field means that there
will be a force on a charged particle.
• Energy density proportional to
• This force ( and electric field) can arise from
electric charges (via Coulomb’s law)
(Electric field)2
(Magnetic field)2
• Electromagnetic forces aren’t felt
instantaneously, the propagate at speed of
electromagnetic wave (speed of light)
• Is a way to determine forces on a charged
particle without thinking about the charges
that give rise to the forces.
• Object transfers momentum to the field, which
later transfers it to another object.
Mon. Feb 20, 2006
Phy107 Lecture 14
9
Mon. Feb 20, 2006
Phy107 Lecture 14
10
Magnetism: Permanent magnets
Magnetic forces
• Clearly magnets interact with each other
Opposites
attract
• North Pole
and South Pole
• Sometimes attracting, sometimes repelling
N
• This is the elementary
magnetic particle
N
• Visualized as a bar with positive pole (North) at one
end and negative pole (South) at other.
• Called magnetic dipole
(North pole
and South pole)
S
• These ‘magnetic charges’ cannot be broken apart —
always appear in N-S pairs.
• Poles interact with each
other similar to charges.
• But the magnetic particles are sort of a ‘composite’
positive and negative ‘magnetic charge’.
S
Mon. Feb 20, 2006
S
N
S
S
N
N
Phy107 Lecture 14
11
Mon. Feb 20, 2006
Likes repel
Phy107 Lecture 14
12
2
Magnetic field
Field lines of a magnet
• Similar in spirit to electric field
• Used to determine the ‘orientational’ force on a
magnetic dipole:
– Magnetic field exerts a force on a dipole that aligns it
with magnetic field lines.
– Uniform magnetic field only rotates dipole: doesn’t cause
it to move.
• Static magnetic field
arises from permanent magnets (or currents).
• Field lines indicate
direction of field
• Density indicates
strength of field
• Similar to
electrostatic force,
but force is felt by
magnetic dipole
• But, as electric field, can exist in an EM wave
even without magnetic dipoles.
Mon. Feb 20, 2006
Phy107 Lecture 14
13
Mon. Feb 20, 2006
Surprise!
The Earth is a magnet!
Earth is a
magnetic dipole.
Phy107 Lecture 14
14
Electric current
produces magnetic field
• Current (flow of electric charges )
in wire produces magnetic field.
• That magnetic field aligns compass needle
North magnetic
pole ~ at south
geographic pole
Current
A compass is a
magnetic dipole
Magnetic
field
Compass needle aligns
with local Earth field
Mon. Feb 20, 2006
Phy107 Lecture 14
15
Magnetic field from a current
Mon. Feb 20, 2006
Phy107 Lecture 14
16
Forces between currents
• Which of these pairs of currents will attract
each other?
A. A
B. A & C
C. B
Iron filings align with
magnetic field lines
Mon. Feb 20, 2006
A
Magnetic field loops
around the current.
Phy107 Lecture 14
17
Mon. Feb 20, 2006
B
Phy107 Lecture 14
C
18
3
Magnetic field from a current loop
Solenoid electromagnet
• One loop:
field still loops around the wire.
• Sequence of current
loops can produce
strong magnetic
fields.
• This is an
electromagnet
• Many loops: same effect
Mon. Feb 20, 2006
Phy107 Lecture 14
Mon. Feb 20, 2006
19
Phy107 Lecture 14
Magnetic Field Ranges
Superconducting Magnets
Field Size
• Solenoid as in
conventional
electromagnet.
• But once current is
injected, power
supply turned off,
current and magnetic
field stays forever…
…as long as T < Tc
Example
Phy107 Lecture 14
0.2 T
0.01 T
33 T
0.0001 T
2T
21
0.00003 T
3x10-10 T
Mon. Feb 20, 2006
Phy107 Lecture 14
22
Large scale applications
• Magnetic Resonance
Imaging typically
done at 1.5 T
• Superconducting
magnet to provides
static magnetic field
• Spatial resolution of
positions of tracer
atomic nuclei.
Phy107 Lecture 14
Example
60 T
Magnets for MRI
Mon. Feb 20, 2006
Field Size
0.4 T
850 T
0.5 T
Mon. Feb 20, 2006
20
Superconducting
magnet
Plasma confinement
torus
Proposed ITER
fusion test reactor
23
Mon. Feb 20, 2006
Phy107 Lecture 14
24
4
Faraday’s law of induction
Time-varying magnetic field
• Up to this point,
electric and magnetic fields constant in time
Faraday’s law:
– time-varying magnetic field
produces electric field
• Constant electric current
produces constant magnetic field.
– Strength of electric field proportional
to how fast magnetic field changes.
• Constant magnetic field
produces… nothing in particular!
In this experiment:
• Magnetic field is largest close to the
bar magnet, drops off farther away.
• But changing the magnetic field in time
produces… an electric field!
• Moving magnet toward coil causes
magnetic field through coil to
increase with time, producing
electric field
• This effect is called induction.
Mon. Feb 20, 2006
Phy107 Lecture 14
• Since coil is conducting, this electric
field produces a current in the wire
of the coil and through the meter.
25
Mon. Feb 20, 2006
One step further: Lenz’s law
• This induced current produces a magnetic field,
which interacts with the bar magnet just as another bar
magnet would.
• Lenz’s law describes the direction of the induced field
(or equivalently, the direction of the induced currents)
– The induced current circulates in such a way as to generate a
magnetic field that tends to cancel the change in the field.
Phy107 Lecture 14
26
Time-varying electric field
• Can also produce a time-varying magnetic field with a
time-varying current in an electromagnet.
• Faraday’s law: time-varying magnetic field
produces electric field,
electric field produces electric current (in a metal).
• Just as before, the current is induced in such a way that
the resulting magnetic dipole repels the changing flux that
produced the current.
– Causes repulsive force on original moving bar magnet.
• This is the principle of an electromagnetic ‘gun’.
Mon. Feb 20, 2006
Phy107 Lecture 14
27
Mon. Feb 20, 2006
Maxwell’s unification
Phy107 Lecture 14
28
Electromagnetic Waves
• Intimate connection
between electricity and magnetism
Current (up and down)
creates electromagnetic wave
consisting of oscillating electric and magnetic fields
• Time-varying magnetic field
induces an electric field (Faraday’s Law)
• Time-varying electric field generates a
r
magnetic field
r r
1 %B
"#E =$
c %t
r
In vacuum:
r r
1 %E
"#B=
c %t
+
This is the basis of Maxwell’s unification of
electricity and magnetism into Electromagnetism
-
!
Mon. Feb 20, 2006
Phy107 Lecture 14
29
Mon. Feb 20, 2006
Phy107 Lecture 14
30
5
Electromagnetic Waves
y
z
x
• A Transverse wave.
• Electric and magnetic fields are perpendicular to
propagation direction
• Can travel in empty space
f = v/λ
v = c = 3 x 108 m/s (186,000 miles/second!)
Mon. Feb 20, 2006
Phy107 Lecture 14
31
6