Title: Using the
1Using the Clicker
- If you have a clicker now, and did not do this
last time, please enter your ID in your clicker. - First, turn on your clicker by sliding the power
switch, on the left, up. Next, store your student
number in the clicker. You only have to do this
once. - Press the button to enter the setup menu.
- Press the up arrow button to get to ID
- Press the big green arrow key
- Press the T button, then the up arrow to get a U
- Enter the rest of your BU ID.
- Press the big green arrow key.
2Magnetic flux
3Magnetic flux
- Magnetic flux is a measure of the number of
magnetic field lines passing through something,
such as a loop. If we define the area of the loop
as a vector, with its direction perpendicular to
the plane of the loop, the magnetic flux is given
by - where ? is the angle between the magnetic field
and the area vector. - The unit of magnetic flux is the weber. 1 Wb 1
T m2.
4Magnetic flux
- The more field lines pass through an area, the
larger the flux. - Lots of flux. No flux.
- Some flux.
5Magnetic flux from a bar magnet
- A bar magnet passes from right to left through a
loop of wire. Flux is positive when the field
lines pass one way through the loop, and negative
when they go in the opposite direction. What, if
anything, is wrong with the graph of magnetic
flux for this situation? - There's nothing wrong
- with it.
- 2. There is something
- wrong with it (you
- specify what it is)
6Observations with a magnet, coil, and galvanometer
- Lets make a few observations, using a magnet
near a coil connected to a galvanometer (a
sensitive current meter). The magnets north pole
points at the coil.
Situation Predict what the galvanometer needle does. What the needle actually does.
The magnet is moved toward the coil. No basis for prediction.
The magnet is moved away from the coil.
The magnet is moved toward the coil again, but more slowly.
The magnet is held at rest near the coil.
The magnet is held at rest and the coil is moved toward the magnet.
7Observations with a magnet, coil, and galvanometer
- Lets make a few observations, using a magnet
near a coil connected to a galvanometer (a
sensitive current meter). The magnets north pole
points at the coil.
Situation Predict what the galvanometer needle does. What the needle actually does.
The magnet is moved toward the coil. No basis for prediction. Needle deflects to the left.
The magnet is moved away from the coil.
The magnet is moved toward the coil again, but more slowly.
The magnet is held at rest near the coil.
The magnet is held at rest and the coil is moved toward the magnet.
8Observations with a magnet, coil, and galvanometer
- Lets make a few observations, using a magnet
near a coil connected to a galvanometer (a
sensitive current meter). The magnets north pole
points at the coil.
Situation Predict what the galvanometer needle does. What the needle actually does.
The magnet is moved toward the coil. No basis for prediction. Needle deflects to the left.
The magnet is moved away from the coil. Opposite to the above.
The magnet is moved toward the coil again, but more slowly.
The magnet is held at rest near the coil.
The magnet is held at rest and the coil is moved toward the magnet.
9Observations with a magnet, coil, and galvanometer
- Lets make a few observations, using a magnet
near a coil connected to a galvanometer (a
sensitive current meter). The magnets north pole
points at the coil.
Situation Predict what the galvanometer needle does. What the needle actually does.
The magnet is moved toward the coil. No basis for prediction. Needle deflects to the left.
The magnet is moved away from the coil. Opposite to the above. Needle deflects to the right.
The magnet is moved toward the coil again, but more slowly.
The magnet is held at rest near the coil.
The magnet is held at rest and the coil is moved toward the magnet.
10Observations with a magnet, coil, and galvanometer
- Lets make a few observations, using a magnet
near a coil connected to a galvanometer (a
sensitive current meter). The magnets north pole
points at the coil.
Situation Predict what the galvanometer needle does. What the needle actually does.
The magnet is moved toward the coil. No basis for prediction. Needle deflects to the left.
The magnet is moved away from the coil. Opposite to the above. Needle deflects to the right.
The magnet is moved toward the coil again, but more slowly. Same as the first case, but needle deflects less.
The magnet is held at rest near the coil.
The magnet is held at rest and the coil is moved toward the magnet.
11Observations with a magnet, coil, and galvanometer
- Lets make a few observations, using a magnet
near a coil connected to a galvanometer (a
sensitive current meter). The magnets north pole
points at the coil.
Situation Predict what the galvanometer needle does. What the needle actually does.
The magnet is moved toward the coil. No basis for prediction. Needle deflects to the left.
The magnet is moved away from the coil. Opposite to the above. Needle deflects to the right.
The magnet is moved toward the coil again, but more slowly. Same as the first case, but needle deflects less. Needle deflects a little bit to the left.
The magnet is held at rest near the coil.
The magnet is held at rest and the coil is moved toward the magnet.
12Observations with a magnet, coil, and galvanometer
- Lets make a few observations, using a magnet
near a coil connected to a galvanometer (a
sensitive current meter). The magnets north pole
points at the coil.
Situation Predict what the galvanometer needle does. What the needle actually does.
The magnet is moved toward the coil. No basis for prediction. Needle deflects to the left.
The magnet is moved away from the coil. Opposite to the above. Needle deflects to the right.
The magnet is moved toward the coil again, but more slowly. Same as the first case, but needle deflects less. Needle deflects a little bit to the left.
The magnet is held at rest near the coil. ??
The magnet is held at rest and the coil is moved toward the magnet.
13Observations with a magnet, coil, and galvanometer
- Lets make a few observations, using a magnet
near a coil connected to a galvanometer (a
sensitive current meter). The magnets north pole
points at the coil.
Situation Predict what the galvanometer needle does. What the needle actually does.
The magnet is moved toward the coil. No basis for prediction. Needle deflects to the left.
The magnet is moved away from the coil. Opposite to the above. Needle deflects to the right.
The magnet is moved toward the coil again, but more slowly. Same as the first case, but needle deflects less. Needle deflects a little bit to the left.
The magnet is held at rest near the coil. ?? Nothing!
The magnet is held at rest and the coil is moved toward the magnet.
14Observations with a magnet, coil, and galvanometer
- Lets make a few observations, using a magnet
near a coil connected to a galvanometer (a
sensitive current meter). The magnets north pole
points at the coil.
Situation Predict what the galvanometer needle does. What the needle actually does.
The magnet is moved toward the coil. No basis for prediction. Needle deflects to the left.
The magnet is moved away from the coil. Opposite to the above. Needle deflects to the right.
The magnet is moved toward the coil again, but more slowly. Same as the first case, but needle deflects less. Needle deflects a little bit to the left.
The magnet is held at rest near the coil. ?? Nothing!
The magnet is held at rest and the coil is moved toward the magnet. Same as the first case.
15Observations with a magnet, coil, and galvanometer
- Lets make a few observations, using a magnet
near a coil connected to a galvanometer (a
sensitive current meter). The magnets north pole
points at the coil.
Situation Predict what the galvanometer needle does. What the needle actually does.
The magnet is moved toward the coil. No basis for prediction. Needle deflects to the left.
The magnet is moved away from the coil. Opposite to the above. Needle deflects to the right.
The magnet is moved toward the coil again, but more slowly. Same as the first case, but needle deflects less. Needle deflects a little bit to the left.
The magnet is held at rest near the coil. ?? Nothing!
The magnet is held at rest and the coil is moved toward the magnet. Same as the first case. Needle deflects to the left.
16Observations with a magnet, coil, and galvanometer
- Lets make a few more observations.
Situation Predict what the galvanometer needle does. What the needle actually does.
The magnet is reversed, so the south pole points at the coil. The magnet is moved toward the coil.
The magnet is moved away from the coil.
The magnet is taken to the other end of the coil, and the north pole is closer to the coil. The magnet is moved toward the coil.
The magnet is moved away from the coil.
The magnet is rotated back and forth near the end of the coil
17Observations with a magnet, coil, and galvanometer
- Lets make a few more observations.
Situation Predict what the galvanometer needle does. What the needle actually does.
The magnet is reversed, so the south pole points at the coil. The magnet is moved toward the coil. Opposite to when the north pole was pointed at the coil.
The magnet is moved away from the coil.
The magnet is taken to the other end of the coil, and the north pole is closer to the coil. The magnet is moved toward the coil.
The magnet is moved away from the coil.
The magnet is rotated back and forth near the end of the coil
18Observations with a magnet, coil, and galvanometer
- Lets make a few more observations.
Situation Predict what the galvanometer needle does. What the needle actually does.
The magnet is reversed, so the south pole points at the coil. The magnet is moved toward the coil. Opposite to when the north pole was pointed at the coil. The needle deflects to the right.
The magnet is moved away from the coil.
The magnet is taken to the other end of the coil, and the north pole is closer to the coil. The magnet is moved toward the coil.
The magnet is moved away from the coil.
The magnet is rotated back and forth near the end of the coil
19Observations with a magnet, coil, and galvanometer
- Lets make a few more observations.
Situation Predict what the galvanometer needle does. What the needle actually does.
The magnet is reversed, so the south pole points at the coil. The magnet is moved toward the coil. Opposite to when the north pole was pointed at the coil. The needle deflects to the right.
The magnet is moved away from the coil. Opposite to the above.
The magnet is taken to the other end of the coil, and the north pole is closer to the coil. The magnet is moved toward the coil.
The magnet is moved away from the coil.
The magnet is rotated back and forth near the end of the coil
20Observations with a magnet, coil, and galvanometer
- Lets make a few more observations.
Situation Predict what the galvanometer needle does. What the needle actually does.
The magnet is reversed, so the south pole points at the coil. The magnet is moved toward the coil. Opposite to when the north pole was pointed at the coil. The needle deflects to the right.
The magnet is moved away from the coil. Opposite to the above. The needle goes left.
The magnet is taken to the other end of the coil, and the north pole is closer to the coil. The magnet is moved toward the coil.
The magnet is moved away from the coil.
The magnet is rotated back and forth near the end of the coil
21Observations with a magnet, coil, and galvanometer
- Lets make a few more observations.
Situation Predict what the galvanometer needle does. What the needle actually does.
The magnet is reversed, so the south pole points at the coil. The magnet is moved toward the coil. Opposite to when the north pole was pointed at the coil. The needle deflects to the right.
The magnet is moved away from the coil. Opposite to the above. The needle goes left.
The magnet is taken to the other end of the coil, and the north pole is closer to the coil. The magnet is moved toward the coil. Same as the south pole at the other end?
The magnet is moved away from the coil.
The magnet is rotated back and forth near the end of the coil
22Observations with a magnet, coil, and galvanometer
- Lets make a few more observations.
Situation Predict what the galvanometer needle does. What the needle actually does.
The magnet is reversed, so the south pole points at the coil. The magnet is moved toward the coil. Opposite to when the north pole was pointed at the coil. The needle deflects to the right.
The magnet is moved away from the coil. Opposite to the above. The needle goes left.
The magnet is taken to the other end of the coil, and the north pole is closer to the coil. The magnet is moved toward the coil. Same as the south pole at the other end? The needle deflects to the right.
The magnet is moved away from the coil.
The magnet is rotated back and forth near the end of the coil
23Observations with a magnet, coil, and galvanometer
- Lets make a few more observations.
Situation Predict what the galvanometer needle does. What the needle actually does.
The magnet is reversed, so the south pole points at the coil. The magnet is moved toward the coil. Opposite to when the north pole was pointed at the coil. The needle deflects to the right.
The magnet is moved away from the coil. Opposite to the above. The needle goes left.
The magnet is taken to the other end of the coil, and the north pole is closer to the coil. The magnet is moved toward the coil. Same as the south pole at the other end? The needle deflects to the right.
The magnet is moved away from the coil. Opposite to the previous.
The magnet is rotated back and forth near the end of the coil
24Observations with a magnet, coil, and galvanometer
- Lets make a few more observations.
Situation Predict what the galvanometer needle does. What the needle actually does.
The magnet is reversed, so the south pole points at the coil. The magnet is moved toward the coil. Opposite to when the north pole was pointed at the coil. The needle deflects to the right.
The magnet is moved away from the coil. Opposite to the above. The needle goes left.
The magnet is taken to the other end of the coil, and the north pole is closer to the coil. The magnet is moved toward the coil. Same as the south pole at the other end? The needle deflects to the right.
The magnet is moved away from the coil. Opposite to the previous. The needle goes left.
The magnet is rotated back and forth near the end of the coil
25Observations with a magnet, coil, and galvanometer
- Lets make a few more observations.
Situation Predict what the galvanometer needle does. What the needle actually does.
The magnet is reversed, so the south pole points at the coil. The magnet is moved toward the coil. Opposite to when the north pole was pointed at the coil. The needle deflects to the right.
The magnet is moved away from the coil. Opposite to the above. The needle goes left.
The magnet is taken to the other end of the coil, and the north pole is closer to the coil. The magnet is moved toward the coil. Same as the south pole at the other end? The needle deflects to the right.
The magnet is moved away from the coil. Opposite to the previous. The needle goes left.
The magnet is rotated back and forth near the end of the coil The needle goes back and forth, too.
26Observations with a magnet, coil, and galvanometer
- Lets make a few more observations.
Situation Predict what the galvanometer needle does. What the needle actually does.
The magnet is reversed, so the south pole points at the coil. The magnet is moved toward the coil. Opposite to when the north pole was pointed at the coil. The needle deflects to the right.
The magnet is moved away from the coil. Opposite to the above. The needle goes left.
The magnet is taken to the other end of the coil, and the north pole is closer to the coil. The magnet is moved toward the coil. Same as the south pole at the other end? The needle deflects to the right.
The magnet is moved away from the coil. Opposite to the previous. The needle goes left.
The magnet is rotated back and forth near the end of the coil The needle goes back and forth, too. What we said.
27Faradays Law
- Faraday's Law ties all of our observations into
one neat package. It says that the voltage
induced in a coil of N turns is given by the rate
of change of the magnetic flux in the coil - Faraday's Law
- This has an incredible number of practical
applications, particularly in the generation and
distribution of electricity. - We call the voltage induced by a changing
magnetic flux an induced emf. This is because
changing magnetic flux acts like a battery in a
coil or loop, which is why there is a current
when there's a complete circuit.
28Graphs of flux and induced emf
- In this situation, a bar magnet is moved at
constant speed v toward a coil until the left end
of the magnet is at the center of the coil. The
magnet is held stationary for 3 seconds, and then
moved to the right away from the coil with a
speed v. -
- What does the graph of magnetic flux as a
function of time look like? Assume positive flux
corresponds to field lines passing through the
coil to the left. - What does the graph of induced emf as a function
of time look like?
29Lenzs Law
- Exposing a coil or loop to a changing magnetic
flux will generate a current if the circuit is
complete. The direction of the current is given
by Lenz's Law - Lenz's Law A changing magnetic flux induces an
emf that produces a current which sets up a
magnetic field that tends to oppose whatever
produced the change. - Coils and loops don't like to change, and they
will try to counteract any changes in magnetic
flux imposed on them. They are not successful -
the change can be made, but the coil or loop
tries to oppose the change while the change is
taking place. This tendency to oppose is why
there is a minus sign in Faraday's Law.
30A pictorial approach to Lenzs Law
- An easy way to approach Lenzs Law situations, to
figure out the direction of an induced current,
it to draw a set of three pictures. - First, some review. In which direction is the
magnetic field inside a loop if the loop has a
counter-clockwise current? What if the current is
clockwise?
31A pictorial approach to Lenzs Law
- An easy way to approach Lenzs Law situations, to
figure out the direction of an induced current,
it to draw a set of three pictures. - First, some review. In which direction is the
magnetic field inside a loop if the loop has a
counter-clockwise current? What if the current is
clockwise?
32A pictorial approach to Lenzs Law
- Example A wire loop in the plane of the page is
in a uniform magnetic field directed into the
page. Over some time interval, the field is
doubled. What direction is the induced current in
the loop while the field is changing? - Step 1 Draw a Before picture, showing the
field passing through the loop before the change
takes place. - Step 2 Draw an After picture, showing the
field passing through the loop after the change. - Step 3 Draw a To Oppose picture, showing the
direction of the field the loop creates to oppose
the change. - Step 4 Use the right-hand rule to determine
which way the induced current goes in the loop to
create that field.
33A pictorial approach to Lenzs Law
- Example A wire loop in the plane of the page is
in a uniform magnetic field directed into the
page. Over some time interval, the field is
doubled. What direction is the induced current in
the loop while the field is changing? - Step 1 Draw a Before picture, showing the
field passing through the loop before the change
takes place.
34A pictorial approach to Lenzs Law
- Example A wire loop in the plane of the page is
in a uniform magnetic field directed into the
page. Over some time interval, the field is
doubled. What direction is the induced current in
the loop while the field is changing? - Step 2 Draw an After picture, showing the
field passing through the loop after the change.
35A pictorial approach to Lenzs Law
- Example A wire loop in the plane of the page is
in a uniform magnetic field directed into the
page. Over some time interval, the field is
doubled. What direction is the induced current in
the loop while the field is changing? - Step 3 Draw a To Oppose picture, showing the
direction of the field the loop creates to oppose
the change. - Step 4 Use the right-hand rule to determine
which way the induced current goes in the loop to
create that field. - One field line is enough for the To Oppose
picture - that's enough to determine the
direction of the induced current.
36Lenzs Law example 1
A wire loop is located near a long straight
current-carrying wire. The current in the wire is
directed to the right. With the current held
constant in the long straight wire, the loop is
moved up, away from the wire. In what direction
is the induced current in the loop? 1. The
induced current is clockwise. 2. The induced
current is counter-clockwise. 3. There is no
induced current.
37Lenzs Law example 1
- The flux through the loop decreases, so the loop
tries to add field lines that are directed out of
the page to oppose the change. The induced
current must go counter-clockwise to produced the
required field.
38Lenzs Law example 2
With the current held constant in the long
straight wire, the loop is moved parallel to the
wire. In what direction is the induced current in
the loop? 1. The induced current is clockwise.
2. The induced current is counter-clockwise. 3.
There is no induced current.
39Lenzs Law example 2
- The flux through the loop is constant, so there
is no change to oppose, and no induced current.
40Lenzs Law example 3
The loop is now placed directly on the wire with
the wire bisecting the loop. If the current in
the wire is increasing, in what direction is the
induced current in the loop? 1. The induced
current is clockwise. 2. The induced current is
counter-clockwise. 3. There is no induced
current.
41Lenzs Law example 3
- The net flux through the loop is always zero, so
there is no change to oppose, and no induced
current.
42Lenzs Law example 4
A loop of wire, in the plane of the page, has an
area of 0.5 m2 and a resistance of R 0.1 O.
There is a uniform magnetic field of B 1.0 T
passing through the loop into the page. In what
direction is the induced current in the loop? 1.
The induced current is clockwise. 2. The induced
current is counter-clockwise. 3. There is no
induced current.
43Lenzs Law example 4
- Nothing is changing, so there is no induced
current.
44Lenzs Law example 4, continued
A loop of wire, in the plane of the page, has an
area of 0.5 m2 and a resistance of R 0.1 O.
There is a uniform magnetic field of B 1.0 T
passing through the loop into the page. Now the
magnetic field is reduced steadily from 1.0 T to
0 over a 10 second period. In what direction is
the induced current in the loop? 1. The induced
current is clockwise. 2. The induced current is
counter-clockwise. 3. There is no induced
current.
45Lenzs Law example 4, continued
- The pictorial method tells us that the field from
the loop must be into the page, requiring a
clockwise current.
46Lenzs Law example 4, continued
- A loop of wire, in the plane of the page, has an
area of 0.5 m2 and a resistance of R 0.1 O.
There is a uniform magnetic field of B 1.0 T
passing through the loop into the page. Now the
magnetic field is reduced steadily from 1.0 T to
0 over a 10 second period. In what direction is
the induced current in the loop? - What is the magnitude of the induced current in
the loop?
47Lenzs Law example 4, continued
- A 0.5 m2 R 0.1 O Bi 1.0 T
- Now the magnetic field is reduced steadily from
1.0 T to 0 over a 10 second period. - First, apply Faradays law to find the induced
emf (voltage)
48Lenzs Law example 4, continued
- A 0.5 m2 R 0.1 O Bi 1.0 T
- Second, apply Ohms law to find the current
49Lenzs Law example 4, continued
- If we'd kept the magnetic field constant, what
other ways could we have induced the same current
(magnitude and direction) in the loop?
50Lenzs Law example 4, continued
- If we'd kept the magnetic field constant, what
other ways could we have induced the same current
(magnitude and direction) in the loop? - By changing the field we reduced the flux to zero
over a 10 second period. Two other ways to do
that are - reduce the area to zero over a 10 second interval
- rotate the loop by 90 over a 10 second interval
51Lenzs Law example 4, continued
- What if, instead of reducing the field to zero in
10 seconds, we reduced it to zero in 2 seconds?
Would anything change? Would anything stay the
same?
52Lenzs Law example 4, continued
- What if, instead of reducing the field to zero in
10 seconds, we reduced it to zero in 2 seconds?
Would anything change? Would anything stay the
same? - The current would still be clockwise, but it
would be 5 times as large. So, we'd get five
times the current for 1/5 of the time. The
product of current and time would be the same,
but that represents the total charge. The same
total charge flows every time.
53Graphs of flux and induced current
- A square conducting loop moves at a constant
velocity of 1 m/s to the right. At t 0, its
right side is at x -6 m. A region of uniform
magnetic field directed into the page is located
between x -4 m and x 0. A second region of
uniform magnetic field directed out of the page
is located between x 0 and x 4 m. The field
in the two regions has the same magnitude and the
field is zero everywhere else. Assume the
velocity of the loop is constant throughout its
motion. Simulation
54Graphs of flux and induced current
- A square conducting loop moves at a constant
velocity of 1 m/s to the right. At t 0, its
right side is at x -6 m. A region of uniform
magnetic field directed into the page is located
between x -4 m and x 0. A second region of
uniform magnetic field directed out of the page
is located between x 0 and x 4 m. Plot graphs
of the magnetic flux through the loop, and the
induced current in the loop, as a function of
time. Define into the page as positive for flux,
and clockwise to be positive for current.
55The flux graph
- Remember that flux is a measure of the number of
field lines passing through the loop, with
positive for, in this case, field lines into the
page.
56The graph of induced current
- What is the connection between the graphs?
57The graph of induced current
- What is the connection between the graphs? The
current graph is proportional to the negative
slope of the flux graph.
58Whiteboard