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Class 9
Physics 106
Learning
Outcomes
Class 9
More Circuit Analysis and Magnetic Fields
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
Physics 106
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
Winter 2017
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Learning Outcomes
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Last time we learned about:
I
Resitivity
I
How resistivity changes with temperature
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
I
Series and parallel circuits with resistors
The Magnetic
Field
I
Kirchhoff’s Laws
The Lorentz
Force
Learning Outcomes
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Today we will discuss:
I
Examples of Series-Parallel Reduction
I
Magnetic Fields
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
I
Series RC Circuits and Time Constants
The Magnetic
Field
I
Using Kirchhoff’s Rules
The Lorentz
Force
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Series-Parallel Reduction
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
Problem-Solving Strategy
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
I
Combine all resistors in series
Virtual Circuit
I
Combine all resistors in parallel
Kirchhoff’s Rules
I
Sketch the new circuit after each step
RC Circuits
I
Continue until one resistor remains
The Magnetic
Field
I
Find the voltage and currents step by step back to
the beginning
The Lorentz
Force
An RC Circuit Example
Equivalent Resistance − Complex Circuit
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
Equivalent Resistance -Complex Circuit
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
Equivalent Resistance -Complex Circuit
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
Find all the currents, voltages, and powers
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
Virtual Circuit
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
You can construct your own circuits and measure
voltages and currents by going to the "Resources" Tab
and then look for the Resistor Network Virtual Lab.
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
Kirchhoff’s Rules
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
I
Junction Rule
I
I
The sum of the currents entering any junction must
equal the sum of the currents leaving that junction
Loop Rule
I The sum of the potential differences across all
the elements around any closed circuit loop
must be zero
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
Applying Kirchhoff’s Rules
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
1.Mark each junction.
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
2. Label all currents - between each pair of
junctions. Choose a direction - it doesn’t
have to be right!
Here there are 6 currents.
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
2. Label all currents - between each pair of
junctions. Choose a direction - it doesn’t
have to be right!
Here there are 6 currents.
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
3. Number of junction equations: If there
are N junctions, there are N − 1 junction
equations.
Here there are 4 junctions, so there are 3
junction equations.
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
Class 9
4. Write the junction equations:
Current in = Current out.
Physics 106
Learning
Outcomes
A. I3 + I6 = I1
B. I1 = I4 + I2
C. I2 = I5 + I6
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
5. Number of loop equations = Number of
currents − Number of junction equations.
Here: 6−3=3, so we need 3 loops.
A. I3 + I6 = I1
B. I1 = I4 + I2
C. I2 = I5 + I6
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
6. At least one loop must cover every
circuit element.
Class 9
Physics 106
Learning
Outcomes
A. I3 + I6 = I1
B. I1 = I4 + I2
C. I2 = I5 + I6
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
7. Put a plus or minus on every resistor
(side current goes in is +) and battery (+ is
positive terminal).
A. I3 + I6 = I1
B. I1 = I4 + I2
C. I2 = I5 + I6
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
Class 9
8. Write the loop equations.
Physics 106
A. I3 + I6 = I1
B. I1 = I4 + I2
C. I2 = I5 + I6
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
1: +6 − 2I3 − 1I1 − 4I4 = 0
2: −3I6 + 2I3 − 6 + 6I5 − 7I6 = 0
3: −6I5 + 4I4 − 5I2 = 0
8. Write the loop equations.
Class 9
Physics 106
When you go around the loop, ignore the current arrows!
Follow the loop in the direction of the loop arrow!
A. I3 + I6 = I1
B. I1 = I4 + I2
C. I2 = I5 + I6
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
1: +6 − 2I3 − 1I1 − 4I4 = 0
2: −3I6 + 2I3 − 6 + 6I5 − 7I6 = 0
3: −6I5 + 4I4 − 5I2 = 0
9. Solve the system of equations using
your favorite method.
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
A. I3 + I6 = I1
B. I1 = I4 + I2
C. I2 = I5 + I6
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
1: +6 − 2I3 − 1I1 − 4I4 = 0
2: −3I6 + 2I3 − 6 + 6I5 − 7I6 = 0
3: −6I5 + 4I4 − 5I2 = 0
The Lorentz
Force
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
RC Circuits
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
A Charging RC Circuit
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
I
When the
circuit is
closed, the
capacitor starts
to charge.
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
A Charging RC Circuit
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
I
The capacitor
continues to
charge until it
reaches its
maximum
charge,
Q = CV .
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
A Charging RC Circuit
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
I
Once the
capacitor is
fully charged,
the current in
the circuit is
zero.
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
A Charging RC Circuit
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
I
The larger the
resistance, the
longer it takes
to charge
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
A Charging RC Circuit
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
I
The larger the
capacitance,
the longer it
takes to charge
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
Charging a Capacitor in an RC Circuit
Class 9
Physics 106
Learning
Outcomes
I
The charge on the
capacitor is q(t) =
Q(1 − e−t/τ )
where τ = RC is
the time constant.
I
At t = 0, the
charge is 0.
I
As t gets large, q
goes to Q = C .
I
When t = τ ,
q = Q(1 − e) =
0.632Q
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
A Discharging RC Circuit
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
I
A charged
capacitor is
discharged
through a
resistor.
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
A Discharging RC Circuit
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
I
Initially the
voltage across
the capacitor is
V = Q/C.
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
Discharging a Capacitor in an RC Circuit
Class 9
Physics 106
I
I
I
I
The charge
decreases in time
as q(t) = Qe−t/τ
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
At t = 0, the
charge is
Q = CV .
Virtual Circuit
As t gets large,
the charge goes
to 0.
The Magnetic
Field
At t = τ , the
charge decreases
to 0.368Q.
(0.368=1-0.632)
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Lorentz
Force
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
An RC Circuit Example
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
An RC Circuit Example
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
I
I
A 10 Ω resistor and a 30 µF capacitor are connected
in series with a 12 V battery and a switch.
What is the final charge on the capacitor?
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
I
Q = CV = 360µF
The Lorentz
Force
An RC Circuit Example
Class 9
Physics 106
Learning
Outcomes
I
A 10 Ω resistor and a 30 µF capacitor are connected
in series with a 12 V battery and a switch.
I
How long does it take after the switch is closed for
the capacitor to reach 50% of its final charge?
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
An RC Circuit Example
Class 9
Physics 106
Learning
Outcomes
I
A 10 Ω resistor and a 30 µF capacitor are connected
in series with a 12 V battery and a switch.
I
How long does it take after the switch is closed for
the capacitor to reach 50% of its final charge?
Series-Parallel
Reduction with
Resistors
Example
q(t) = Q(1 − e−t/τ )
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
An RC Circuit Example
Class 9
Physics 106
Learning
Outcomes
I
A 10 Ω resistor and a 30 µF capacitor are connected
in series with a 12 V battery and a switch.
I
How long does it take after the switch is closed for
the capacitor to reach 50% of its final charge?
Series-Parallel
Reduction with
Resistors
Example
q(t) = Q(1 − e−t/τ )
q(t1/2 ) = Q /2 = Q(1 − e−t1/2 /τ )
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
An RC Circuit Example
Class 9
Physics 106
Learning
Outcomes
I
A 10 Ω resistor and a 30 µF capacitor are connected
in series with a 12 V battery and a switch.
I
How long does it take after the switch is closed for
the capacitor to reach 50% of its final charge?
Series-Parallel
Reduction with
Resistors
Example
q(t) = Q(1 − e−t/τ )
Q /2 = Q(1 − e−t1/2 /τ )
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
An RC Circuit Example
Class 9
Physics 106
Learning
Outcomes
I
A 10 Ω resistor and a 30 µF capacitor are connected
in series with a 12 V battery and a switch.
I
How long does it take after the switch is closed for
the capacitor to reach 50% of its final charge?
Series-Parallel
Reduction with
Resistors
Example
q(t) = Q(1 − e−t/τ )
1/2 = (1 − e−t1/2 /τ )
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
An RC Circuit Example
Class 9
Physics 106
Learning
Outcomes
I
A 10 Ω resistor and a 30 µF capacitor are connected
in series with a 12 V battery and a switch.
I
How long does it take after the switch is closed for
the capacitor to reach 50% of its final charge?
Series-Parallel
Reduction with
Resistors
Example
q(t) = Q(1 − e−t/τ )
1/2 = (1 − e−t1/2 /τ )
e−t1/2 /τ = (1/2)
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
An RC Circuit Example
Class 9
Physics 106
Learning
Outcomes
I
A 10 Ω resistor and a 30 µF capacitor are connected
in series with a 12 V battery and a switch.
I
How long does it take after the switch is closed for
the capacitor to reach 50% of its final charge?
Series-Parallel
Reduction with
Resistors
Example
q(t) = Q(1 − e−t/τ )
1/2 = (1 − e−t1/2 /τ )
1/e−t1/2 /τ = 1/(1/2)
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
An RC Circuit Example
Class 9
Physics 106
Learning
Outcomes
I
A 10 Ω resistor and a 30 µF capacitor are connected
in series with a 12 V battery and a switch.
I
How long does it take after the switch is closed for
the capacitor to reach 50% of its final charge?
Series-Parallel
Reduction with
Resistors
Example
q(t) = Q(1 − e−t/τ )
1/2 = (1 − e−t1/2 /τ )
1/e−t1/2 /τ = 1/(1/2)
e+t1/2 /τ = 2
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
An RC Circuit Example
Class 9
Physics 106
Learning
Outcomes
I
A 10 Ω resistor and a 30 µF capacitor are connected
in series with a 12 V battery and a switch.
I
How long does it take after the switch is closed for
the capacitor to reach 50% of its final charge?
Series-Parallel
Reduction with
Resistors
Example
q(t) = Q(1 − e−t/τ )
1/2 = (1 − e−t1/2 /τ )
1/e−t1/2 /τ = 1/(1/2)
e+t1/2 /τ = 2
ln(e+t1/2 /τ ) = ln(2)
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
An RC Circuit Example
Class 9
Physics 106
Learning
Outcomes
I
A 10 Ω resistor and a 30 µF capacitor are connected
in series with a 12 V battery and a switch.
I
How long does it take after the switch is closed for
the capacitor to reach 50% of its final charge?
Series-Parallel
Reduction with
Resistors
Example
q(t) = Q(1 − e−t/τ )
1/2 = (1 − e−t1/2 /τ )
1/e−t1/2 /τ = 1/(1/2)
e+t1/2 /τ = 2
ln(e+t1/2 /τ ) = ln(2)
t1/2 = τ ln(2)
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
An RC Circuit Example
Class 9
Physics 106
Learning
Outcomes
I
A 10 Ω resistor and a 30 µF capacitor are connected
in series with a 12 V battery and a switch.
I
How long does it take after the switch is closed for
the capacitor to reach 50% of its final charge?
Series-Parallel
Reduction with
Resistors
Example
q(t) = Q(1 − e−t/τ )
1/2 = (1 − e−t1/2 /τ )
1/e−t1/2 /τ = 1/(1/2)
e+t1/2 /τ = 2
ln(e+t1/2 /τ ) = ln(2)
t1/2 = τ ln(2) = R × C × ln(2) = 208µs
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
The Magnetic Field
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
Magnetic Fields
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
I
I
I
Moving charges produces magnetic fields in addition
to electric fields.
To feel a magnetic force, a test charge must also be
moving.
Magnetic fields are used to describe the Coulomb
force when charges are in motion.
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
Magnetic Fields and Wires
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
I
I
I
Moving electrons in wires produce magnetic fields,
whereas stationary charges do not.
Wires therefore produce magnetic fields.
This was first observed by Hans Christian Oersted in
1820.
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
Magnets
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
I
I
I
Magnetite or loadstone is a naturally occurring
magnet.
From ancient times, people used magnetite as a
compass.
The magnetic field in permanent magnets is caused
by electrons moving in atoms.
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
Magnets
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
I
I
I
Magnets have north poles and south poles.
Like poles repel each other and unlike poles attract
each other
Magnetic poles cannot be isolated
I
I
If a permanent magnetic is cut in half repeatedly, you
will still have a north and a south pole
Some physicists believe magnetic "monopoles"
should exist, but none have yet been found
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
Magnetic Fields
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
I
I
~
A vector field, we write it as B
That means that at every point in space we can find
~
a magnitude and direction for B.
I
Its direction at a point is the direction the north pole
of a compass needle points.
I
Magnetic field lines can be used much like electric
field lines.
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
Magnetic Field Lines
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
I
A compass can be used to show the direction of the
magnetic field lines.
Earth’s Magnetic Field
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
I
The north pole of a magnet is the "north-seeking"
pole
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
I
That means the magnetic pole near the Earth’s north
geographic pole is actually a south magnetic pole.
The Magnetic
Field
The Lorentz
Force
Earth’s Magnetic Field
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
I
The Earth’s
magnetic field
is similar to that
of a huge bar
magnet deep in
the Earth’s
interior.
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
Units of Magnetic Field
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
I
The SI unit of magnetic field is the Tesla (T)
I
Another commonly used unit is a Gauss(G)
I
1 T = 104 G
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
A Few Typical B Values
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
I
I
I
Conventional laboratory magnets
Up to 25000 G or 2.5 T
Superconducting magnets
Up to 300000 G or 30 T
Earth’s magnetic field
0.5 G or 5 x 10−5 T
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
The Lorentz or
Magnetic Force
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
The Electric Force (a Quick Review)
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
~ E = qE
~
F
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
I
The magnitude of the electric force on a test charge
depends on
I
I
I
The test charge (q)
The electric field (E)
The direction of the force depends on:
I
The direction of the electric field
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
The Magnetic Force
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
I
The magnitude of the magnetic force on a test
charge depends on:
I
I
I
I
The test charge, q
The magnetic field, B
The velocity of the test charge, v
The angle between the magnetic field and the test
charge, θ
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
The Magnetic Force
Class 9
Physics 106
Learning
Outcomes
I
First consider the magnetic field vector and the
velocity vector
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
The Magnetic Force
Class 9
Physics 106
I
Call the angle between the vectors θ
I
The magnitude of the force is
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
F = qvB sin θ
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
The Magnetic Force
Class 9
Physics 106
Learning
Outcomes
I
F = qvB sin θ
I
If the test charge moves in the direction of the
field,there is no force.
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
The Magnetic Force
Class 9
Physics 106
Learning
Outcomes
I
F = qvB sin θ
I
If the test charge moves opposite the direction of the
field,there is no force.
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
The Magnetic Force
Class 9
Physics 106
Learning
Outcomes
I
F = qvB sin θ
I
The force is largest when the velocity and B field are
perpendicular.
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
The Magnetic Force
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
I
The direction of the magnetic force on a test charge
depends on:
I
I
~
The magnetic field vector, B
The velocity vector, ~v
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
The Magnetic Force
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
I
The direction of the magnetic force on a test charge
depends on:
I
I
~
The magnetic field vector, B
The velocity vector, ~v
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
The Magnetic Force
Class 9
Physics 106
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
I
The direction of the magnetic force on a test charge
depends on:
I
I
~
The magnetic field vector, B
The velocity vector, ~v
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
The Magnetic Force
Class 9
Physics 106
Learning
Outcomes
I
Two vectors must always lie in a single plane.
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
The Magnetic Force
Class 9
Physics 106
Learning
Outcomes
I
The direction of the magnetic force is perpendicular
to this plane.
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
The Magnetic Force
Class 9
Physics 106
I
But there are two directions perpendicular to a plane.
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
The Magnetic Force
Class 9
Physics 106
I
We select the correct choice by using the "right-hand
rule."
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
Right Hand Rule #1
Class 9
Physics 106
I
Place your fingers in
the direction of ~v .
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
Right Hand Rule #1
Class 9
Physics 106
I
I
Place your fingers in
the direction of ~v .
Curl your fingers into
the direction of the
~
magnetic field, B.
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
Right Hand Rule #1
Class 9
Physics 106
I
I
I
Place your fingers in
the direction of ~v .
Curl your fingers into
the direction of the
~
magnetic field, B.
Your thumb points in
the direction of the
~ , on a
force, F
positive charge
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
Right Hand Rule #1
Class 9
Physics 106
I
I
I
I
Place your fingers in
the direction of ~v .
Curl your fingers into
the direction of the
~
magnetic field, B.
Your thumb points in
the direction of the
~ , on a
force, F
positive charge
If the charge is
negative, the force is
opposite that
determined by the
right hand rule.
Learning
Outcomes
Series-Parallel
Reduction with
Resistors
Example
Virtual Circuit
Kirchhoff’s Rules
RC Circuits
An RC Circuit Example
The Magnetic
Field
The Lorentz
Force
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