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Transcript
College
Physics B
Electric
Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
College Physics B - PHY2054C
Magnetic
Fields
Bar Magnets
Horseshoe Magnets
Magnetic Fields
Electromagnetism
Magnetic Fields from
Currents
Current Loop
09/22/2014
My Office Hours:
Tuesday 10:00 AM - Noon
206 Keen Building
College
Physics B
Outline
Electric
Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
Magnetic
Fields
Bar Magnets
Horseshoe Magnets
1 Electric Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
Electromagnetism
Magnetic Fields from
Currents
Current Loop
2 Magnetic Fields
Bar Magnets
Horseshoe Magnets
3 Electromagnetism
Magnetic Fields from Currents
Current Loop
College
Physics B
Resistors in Series
Electric
Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
Magnetic
Fields
Bar Magnets
Horseshoe Magnets
Electromagnetism
Magnetic Fields from
Currents
Current Loop
When current passes through one resistor and then another,
the resistors are said to be in series:
E − I R1 − I R2 = 0
Kirchhoff ′ s Loop Rule
Any number of resistors can be connected in series. The
resistors will be equivalent to a single resistor with:
R equiv = R 1 + R 2 + R 3 + ...
College
Physics B
Review Question 1
Electric
Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
Magnetic
Fields
Bar Magnets
Two light bulbs, A and B, are connected in series to
a constant voltage source. When a wire is connected
across B as shown, bulb A
Horseshoe Magnets
Electromagnetism
Magnetic Fields from
Currents
Current Loop
A burns more brightly.
B burns as brightly.
C burns more dimly.
D goes out.
College
Physics B
Review Question 1
Electric
Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
Magnetic
Fields
Bar Magnets
Two light bulbs, A and B, are connected in series to
a constant voltage source. When a wire is connected
across B as shown, bulb A
Horseshoe Magnets
Electromagnetism
Magnetic Fields from
Currents
Current Loop
A burns more brightly.
B burns as brightly.
C burns more dimly.
D goes out.
College
Physics B
Resistors in Parallel
Electric
Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
Magnetic
Fields
Bar Magnets
Horseshoe Magnets
Electromagnetism
Magnetic Fields from
Currents
Current Loop
Applying the Junction Rule (Kirchhoff ’s Junction Rule)
For path 1, +E − I 1 R 1 = 0
For path 2, +E − I 2 R 2 = 0
The total current is: I 3 = I 1 + I 2 =
E
R1
+
E
R2
= E ( R11 +
1
R2 )
College
Physics B
Electric
Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
Magnetic
Fields
Bar Magnets
Horseshoe Magnets
Electromagnetism
Magnetic Fields from
Currents
Current Loop
Equivalent Resistance - Parallel
College
Physics B
Circuit Analysis
Electric
Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
1
Some complex circuits can be solved by combinations of
series and parallel rules.
2
Other circuits must be analyzed directly by Kirchhoff’s Rules.
Magnetic
Fields
Bar Magnets
Horseshoe Magnets
• Loop Rule: The total change in the electric potential around
Electromagnetism
any closed circuit path must be zero.
Magnetic Fields from
Currents
• Junction Rule: The current entering a circuit junction must
Current Loop
equal the current leaving the junction.
3
Connecting resistors in series always gives a total resistance
larger than the resistance of any of the component resistors.
4
Connecting resistors in parallel always gives a total
resistance smaller than the resistance of any of the
component resistors.
College
Physics B
Ammeters
Electric
Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
Magnetic
Fields
Bar Magnets
Horseshoe Magnets
Electromagnetism
Magnetic Fields from
Currents
Current Loop
An Ammeter is a device that
measures current.
• An ammeter must be connected in series with the
desired circuit branch.
• An ideal ammeter will measure current without changing
its value.
➜ Must have a very low resistance.
College
Physics B
Voltmeters
Electric
Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
Magnetic
Fields
Bar Magnets
Horseshoe Magnets
Electromagnetism
Magnetic Fields from
Currents
Current Loop
A Voltmeter is a device that
measures the voltage across
a circuit element.
• It must be connected in parallel with the element.
• An ideal voltmeter should measure the voltage without
changing its value.
➜ Should have a very high resistance.
College
Physics B
Electric
Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
Magnetic
Fields
Bar Magnets
Horseshoe Magnets
Electromagnetism
Magnetic Fields from
Currents
Current Loop
Superconductivity
At very low temperatures, the
linearity of resistance breaks
down.
• The resistivities of metals
approach a nonzero value
at very low temperatures.
• In some metals, resistivity
drops abruptly and is zero
below a critical
temperature.
• These metals for which
the resistivity goes to
zero are the called
superconductors.
College
Physics B
Superconductivity
Electric
Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
Magnetic
Fields
Bar Magnets
Horseshoe Magnets
Electromagnetism
Magnetic Fields from
Currents
John Robert Schrieffer
Nobel Laureate
Emeritus Professor at Florida State
Current Loop
Bardeen, Cooper, and Schrieffer received the Nobel Prize in
1972 for the development of the theory of superconductivity.
The BCS Theory is one of the greatest discoveries of the 20th
century.
College
Physics B
Outline
Electric
Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
Magnetic
Fields
Bar Magnets
Horseshoe Magnets
1 Electric Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
Electromagnetism
Magnetic Fields from
Currents
Current Loop
2 Magnetic Fields
Bar Magnets
Horseshoe Magnets
3 Electromagnetism
Magnetic Fields from Currents
Current Loop
College
Physics B
Magnetism
Electric
Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
Magnetic
Fields
Bar Magnets
Horseshoe Magnets
Electromagnetism
Magnetic Fields from
Currents
Current Loop
The first observations of magnetic fields involved permanent
magnets. Many ancient cultures discovered natural magnetic
properties of materials.
Permanent magnetic applications include:
• Compass needles
• Speakers
• Computer hard disks
College
Physics B
Electric
Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
Magnetic
Fields
Bar Magnets
Horseshoe Magnets
Electromagnetism
Magnetic Fields from
Currents
Current Loop
Magnetic Poles
College
Physics B
Electric
Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
Magnetic
Fields
Bar Magnets
Magnetic Field Lines
A bar magnet is a permanent
magnet in the shape of a bar.
• The symbol for the
~
magnetic field is B.
Horseshoe Magnets
Electromagnetism
Magnetic Fields from
Currents
Current Loop
• SI unit of the magnetic
field is the Tesla (T )
• The magnetic field lines
can be deduced from the
pattern of the iron filings.
Some properties of the magnetic field:
• The iron filings align parallel to the magnetic field line.
• The magnetic field lines go from the north pole toward
the south pole.
College
Physics B
Electric
Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
Magnetic
Fields
Bar Magnets
Magnetic Field Lines
A bar magnet is a permanent
magnet in the shape of a bar.
• The symbol for the
~
magnetic field is B.
Horseshoe Magnets
Electromagnetism
Magnetic Fields from
Currents
Current Loop
• SI unit of the magnetic
field is the Tesla (T )
• The magnetic field lines
can be deduced from the
pattern of the iron filings.
Some properties of the magnetic field:
• The magnitude of the field decreases as you move
farther from a pole.
• The magnetic field lines form closed loops!
College
Physics B
Magnetic Field Lines
Electric
Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
Magnetic
Fields
Bar Magnets
Horseshoe Magnets
Electromagnetism
Magnetic Fields from
Currents
Current Loop
The magnetic field lines always form
closed loops.
➜ A general property of magnetic
fields, not just bar magnets.
The magnetic poles are analogous
to positive and negative charges.
College
Physics B
Electric
Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
Magnetic
Fields
Bar Magnets
Horseshoe Magnets
Electromagnetism
Magnetic Fields from
Currents
Current Loop
Question 2
Electrical charges and magnetic poles have many similarities,
but one important “difference” is:
A Opposite magnetic poles repel.
B One magnetic pole cannot create magnetic poles in
other materials.
C A magnetic pole cannot be isolated.
D Magnetic poles do not produce magnetic fields.
College
Physics B
Electric
Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
Magnetic
Fields
Bar Magnets
Horseshoe Magnets
Electromagnetism
Magnetic Fields from
Currents
Current Loop
Question 2
Electrical charges and magnetic poles have many similarities,
but one important “difference” is:
A Opposite magnetic poles repel.
B One magnetic pole cannot create magnetic poles in
other materials.
C A magnetic pole cannot be isolated.
D Magnetic poles do not produce magnetic fields.
College
Physics B
Electric
Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
Horseshoe Magnet
Can be made by bending a bar
magnet.
Magnetic
Fields
• There are poles at the ends
Bar Magnets
of the horseshoe magnet.
Horseshoe Magnets
Electromagnetism
Magnetic Fields from
Currents
Current Loop
• The field is largest in the
horseshoe gap.
• The field is directed across
the gap.
➜ iron yoke to strengthen field
College
Physics B
Outline
Electric
Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
Magnetic
Fields
Bar Magnets
Horseshoe Magnets
1 Electric Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
Electromagnetism
Magnetic Fields from
Currents
Current Loop
2 Magnetic Fields
Bar Magnets
Horseshoe Magnets
3 Electromagnetism
Magnetic Fields from Currents
Current Loop
College
Physics B
Electric
Circuits
Connection between Electricity
and Magnetism
Resistors in Series
Resistors in Parallel
Superconductivity
Magnetic
Fields
Sources of Electric Fields Sources of Magnetic Fields
Bar Magnets
Horseshoe Magnets
Electromagnetism
Magnetic Fields from
Currents
Current Loop
Electric Charge
College
Physics B
Electric Fields
Electric
Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
Capacitor
Magnetic
Fields
Bar Magnets
Horseshoe Magnets
Electromagnetism
Magnetic Fields from
Currents
Current Loop
Michael Faraday
(1791 - 1867)
Static Point Charges
College
Physics B
Electric
Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
Magnetic
Fields
Bar Magnets
Horseshoe Magnets
Electromagnetism
Magnetic Fields from
Currents
Current Loop
Faraday’s Cage
College
Physics B
Electric
Circuits
Connection between Electricity
and Magnetism
Resistors in Series
Resistors in Parallel
Superconductivity
Magnetic
Fields
Sources of Electric Fields Sources of Magnetic Fields
Bar Magnets
Horseshoe Magnets
Electromagnetism
Magnetic Fields from
Currents
Current Loop
Electric Charge
Moving Electric Charge
College
Physics B
Electromagnetism
Electric
Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
Christian Oersted
(1777 - 1851)
Magnetic
Fields
Bar Magnets
Horseshoe Magnets
Electromagnetism
Magnetic Fields from
Currents
Current Loop
Field around a currentcarrying wire is fairly weak
College
Physics B
Magnetic Field from Current
Electric
Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
Magnetic
Fields
Moving charges produce magnetic
fields:
Bar Magnets
Horseshoe Magnets
Electromagnetism
Magnetic Fields from
Currents
• An electric current consists
of moving charges, so it will
produce a magnetic field.
Current Loop
• The iron filings show the
magnetic field pattern due
to the current.
College
Physics B
Electric
Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
Magnetic
Fields
Bar Magnets
Horseshoe Magnets
Electromagnetism
Magnetic Fields from
Currents
Question 3
A current in a long, straight wire produces a magnetic field.
The magnetic field lines
A go out from the wire to infinity.
B come in from infinity to the wire.
C form circles that pass through the wire.
Current Loop
D form circles that go around the wire.
College
Physics B
Electric
Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
Magnetic
Fields
Bar Magnets
Horseshoe Magnets
Electromagnetism
Magnetic Fields from
Currents
Question 3
A current in a long, straight wire produces a magnetic field.
The magnetic field lines
A go out from the wire to infinity.
B come in from infinity to the wire.
C form circles that pass through the wire.
Current Loop
D form circles that go around the wire.
College
Physics B
Electric
Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
Magnetic
Fields
Bar Magnets
Question 3
A current in a long, straight wire produces a magnetic field.
The magnetic field lines
D form circles that go around the wire.
Horseshoe Magnets
Electromagnetism
Magnetic Fields from
Currents
Current Loop
Ampère’s Law:
X
B k ∆L = µ0 I enclosed
closed path
B =
µ0 I
2π r
for a straight wire
The constant µ0 is called the
permeability of free space:
µ0 = 4π × 10−7 T · m/A
College
Physics B
Right-Hand Rule
Electric
Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
Magnetic
Fields
Bar Magnets
Horseshoe Magnets
Electromagnetism
Magnetic Fields from
Currents
Current Loop
For a straight wire, the magnetic
field lines form circles:
• The direction of the field is
always tangent to the circles.
• The magnitude of the field
decreases as the distance
from the wire increases.
• The direction of the field is
given by the right-hand rule.
College
Physics B
Right-Hand Rule
Electric
Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
Magnetic
Fields
Bar Magnets
Horseshoe Magnets
Electromagnetism
Magnetic Fields from
Currents
Current Loop
Point the thumb of your ight hand in
the direction of the current:
• Your thumb will be parallel to
the wire.
• Curling the fingers of your right
hand around the wire gives the
direction of the magnetic field.
College
Physics B
Electric
Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
Magnetic
Fields
Bar Magnets
Question 4
Two current-carrying wires are parallel as shown below; the
current is the same in both wires. The current in both wires is
flowing to the right. At a point midway between the wires, the
direction of the net magnetic field is
Horseshoe Magnets
Electromagnetism
Magnetic Fields from
Currents
Current Loop
A to the right →
B to the left ←
C into the screen
D out of the screen
E The field is zero.
•P
College
Physics B
Electric
Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
Magnetic
Fields
Bar Magnets
Question 4
Two current-carrying wires are parallel as shown below; the
current is the same in both wires. The current in both wires is
flowing to the right. At a point midway between the wires, the
direction of the net magnetic field is
Horseshoe Magnets
Electromagnetism
Magnetic Fields from
Currents
Current Loop
A to the right →
B to the left ←
C into the screen
D out of the screen
E The field is zero.
College
Physics B
Plotting Field Lines
Electric
Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
Magnetic
Fields
Bar Magnets
Horseshoe Magnets
Electromagnetism
Magnetic Fields from
Currents
Field lines are three-dimensional.
1
A large dot (•) indicates the tip
of the vector when it points out
of the plane.
2
A cross (×) denotes the tail of
the vector when it points into
the plane.
Current Loop
College
Physics B
Electric
Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
Magnetic
Fields
Bar Magnets
Horseshoe Magnets
Electromagnetism
Magnetic Fields from
Currents
Current Loop
Charges and Magnetic Fields
• The electric current can be modeled as a collection of
positive electric charges.
• The charges would be moving with a velocity parallel to
the current direction.
• The direction of the magnetic field is given by the
right-hand rule.
• A positive charge moving to the left produces the same
magnetic field as a negative charge moving to the right.
Principle of Superposition
The Principle of Superposition states the total magnetic field
produced by two or more different sources is equal to the sum
of the fields produced by each source individually.
College
Physics B
Electric
Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
Magnetic
Fields
Bar Magnets
Horseshoe Magnets
Electromagnetism
Magnetic Fields from
Currents
Current Loop
Current Loop
Treat the loop as many small pieces
of wire:
• Apply the right-hand rule to
find the field from each piece
of wire.
• Applying superposition gives
the overall pattern shown on
the right.
At the center of the loop:
B =
µ0 I
2R
College
Physics B
Electric
Circuits
Resistors in Series
Resistors in Parallel
Superconductivity
Magnetic
Fields
Solenoids
By stacking many loops close together, the field along the axis
is much larger than for a sinle loop.
A helical winding of wire is called a solenoid.
Bar Magnets
Horseshoe Magnets
Electromagnetism
Magnetic Fields from
Currents
Current Loop
➜ More practical than stacking single loops.