Wednesday, July 5, 2006
Announcements:
- RWP1 (Gel Electrophoresis) has been graded and can be picked up
now. Be sure to review the posted
solution to this problem to see what you should have included and
what to consider for future real-world problems.
- I do not have papers from about 15 students, so please let me
know if you submitted a solution and do not see your paper among those
being handed back.
- Exam 1 is scheduled for this Friday, July 7.
- The real-world problem for Exam
1 is now posted. This take-home problem will be worth ~25% of
the points on Exam 1 (the multiple-choice section in class will be the
primary portion). Keep the following in mind when writing up
your solution to this problem:
- Unlike the real-world problems assigned for homework, this
exam
problem must be done individually.
- Remember to justify any claims you make by citing reputable
sources or showing example calculations that validate the statements
you make.
- If you copy information from another source, you must include
a
reference to that source in your work. Failure to give credit for
material that is not your own is an Honor Code violation!
- Remember that you are encouraged to create and solve your own
real-world problem for each exam (worth up to 5 bonus points on the
exam). See the guidelines
posted under the real-world problem webpage for more details.
- Suggestions on how to prepare for
an exam are posted under the resource section of the course
homepage.
- I will remain after class today and tomorrow to answer
questions you may have related to material in Chapters 19-24. You are
encouraged to also take advantage of the regular SI session times as you review and
prepare for the exam.
- If you cannot take the exam in class on Friday, let me know so
that I
can make alternative arrangemetns with you.
Assignments:
- HW23b is due today at midnight.
- HW24b is due tomorrow at midnight.
- The real-world problem for Exam 1
is now posted and is due in class
on Monday.
Chapter 23: Magnetic Flux and Faraday's Law of Induction
23-1: Induced Electromotive Force
A changing magnetic field can produce a
current in a circuit due to an induced
electromotive force.
The magnitude of the induced emf (and
resulting current) depends on the rate
of change of the magnetic flux.
Demo: Induced emf (coil,
magnet, large galvanometer) - Observe that the amount of deflection of
the
galvonometer needle (which also operates on magnetic induction) depends
on how quickly the magnet moves relative to the coil. The
direction of the induced current changes when any one of the following
conditions are reversed: orientation of the magnet, orientation
of the coil, relative motion of magnet and coil. The direction
can be predicted by Lenz's Law
(see below).
23-2: Magnetic Flux
Magnetic flux (like electric flux) is defined as the
number of magnetic field lines that cross a given area.
Phi = BAcos(theta), where theta is the angle between
B and the normal to the area.
Measured in webers: 1 Wb = 1 T-m^2
Example:
The magnetic flux through a 1 m^2
table top where Bearth = 0.6 G at 70 degrees from horizontal is (0.6e-4
T)(1 m^2)cos(20) = 0.06 mWb
23-3: Faraday's Law of Induction
The emf induced by a changing magnetic flux through
a coil of N turns is: emf = -N(dPhi/dt)
Prob.10 -
For a magnetic flux that changes sinusoidally, when is the induced emf
a maximum and minimum?
Prob.16 -
Find the average induced emf for a loop of wire 1.12 m long that
changes shape from a square to a circle in 4.25 s where B = 0.105 T
perpendicular to the plane of the loop.
23-4: Lenz's Law
An induced current flows in the direction that
opposes the change that caused the current. (Think of this
natural attempt to conserve magnetic flux as the action-reaction law
for electromagnetism.)
Demo: Eddy current brake
Demo: Eddy current tube and ramp
Prob.24 -
What is the direction of the current induced in the circuit shown
(Fig.23-31) when the magnetic field increases? Does the top or
bottom plate of the capacitor become positively charged?
Prob.26 -
What emf is induced in a coil that encircles a long current-carrying
wire if the current in the wire is (a) constant, or (b)
increases? What if the wire is still perpendicular to the plane
of the coil but does not pass through its center?
Demo:
Jumping ring
23-5: Mechanical Work and
Electrical Energy
Mechanical work can be converted to electrical
energy by means of a magnetic field.
A conductor of length L that is forced to move with
speed v through a magnetic field B will have an induced emf = BvL.
Prob.29,62
- The emf induced in long conductors moving through weak magnetic
fields can be significant. (Remember the failed NASA experiment to
generate electricity in space using a long wire?)
CQ: 16 -
Describe motion of rod sliding on rails in magnetic field when the
switch is closed.
23-6: Generators and Motors
An electric generator uses mechanical work to
produce electrical energy: emf = NBAwsin(wt)
A motor is basically an electric generator operated
in reverse.
Demo -
simple motor
Prob.36 -
What is the maximum emf for a coil made from 1.6 m of wire wound into a
coil that is 3.2 cm in diameter and rotated at 95 rpm in a 0.070 T
magnetic field? [18 mV]
Prob.37 (assigned
for HW) - Which component of the earth's magnetic field contributes to
the induced emf in a circular coil rotating about a vertical axis?
23-7: Inductance
Self-inductance (or simply inductance, L) is defined
in terms of the emf that opposes the change in current within a
coil: emf = -L(dI/dt)
The SI unit of inductance is the henry: 1 H =
1 V-s/A
The inductance of a solenoid is: L =
uo*n^2*A*length, where n = N/length
Prob.44 -
Find the inductance of a solenoid that has an induced emf of 75 mV when
dI/dt = 2.0 A/s.[38 mH] What will be the induced emf if the
solenoid is stretched to twice its original length? [38 mV]
23-8: RL Circuits
The characteristic time over which current changes
in an RL circuit is: tau = L/R
When the switch is closed in an RL circuit, there is
a large self-induced back-emf due to the sudden change in current, so
the current through the inductor is initially small, but increases
logarithmically to a maximum steady-state value: I = V/R(1 -
e^-tR/L).
Prob.46 -
Find the time constant for the circuit shown in Fig. 23-34. [0.4
ms] What is the current when t = 2*tau? [60 mA] What
is current after a long time? [70 mA]
23-9: Energy Stored in a
Magnetic Field
Energy can be stored in a magnetic field (just like
energy stored in an electric field).
An inductor with current I has energy: U =
(1/2)LI^2
The energy density of a magnetic field is:
u(B) = B^2/(2uo)
Prob.54 -
Find the energy stored in the inductor at t = 0, tau, and infinity.
CQ20 - What
happens to the energy of a solenoid if n is doubled and I is halved?
P.80 - What
is the value of E/B for electric and magnetic fields with the same
energy density? [c]
23-10: Transformers
A transformer uses magnetic induction to convert current and voltage in
one circuit to a different current and voltage in another circuit with
minimal power loss.
The emf in either the primary or secondary
coil is proportional to the number of turns in the coil based on
Faraday's law of induction. Vp/Vs = Np/Ns.
All transformers are fundamentally similar, but
differ in size according to the maximum power that they can handle
without overheating.
Demo:
Transformer with light bulb
Ponderable:
Why is the voltage stepped up from 12 kV to 240 kV for transmission of
electrical energy over long distances?
Applications of magnetic
induction: generators, motors, transformers, audio
speakers, telephone receivers and speakers, read/write heads for
magnetic media (tape recorders, VCR, disk drives), tuning circuits for
wireless EM devices (radios, cell phones, TVs), electric guitar
pickups, MRI, regenerative breaking systems, metal detectors, magnetic
anti-theft
devices, traffic signal loops in pavement, rechargeable toothbrushes.
Concept
Tests
Chapter 24: AC Circuits
24-1: Alternating Voltages and
Currents
An ac generator produces a voltage that varies over
time: V = Vmax*sin(wt)
The voltage read by an AC voltmeter is Vrms =
Vmax/sqrt(2) = 0.71*Vmax
Example:
What is the peak voltage (Vp) for 120 VAC? [170 V] What is
the peak-to-peak voltage (Vpp) for 120 VAC? [340 V]
Prob.7 -
What is Vrms for a square wave?
24-2: Capacitors in AC Circuits
The current through a capacitor depends on the
frequency and is out of phase with the applied voltage.
When the voltage across the capacitor is a maximum
value, the current is zero, so the voltage lags the current by 90 deg.
In a phasor diagram, the voltage of a capacitor is
drawn at an angle that is 90 degrees clockwise from the current phasor.
The current through the capacitor can be found from
I = V/Xc, where Xc = 1/wC is the capacitive reactance.
Prob.14 -
What is Irms for a pure capacitive AC circuit?
24-3: RC Circuits
Impedance is
the overall opposition to the flow of current in a circuit due to
resistance, capacitance, and inductance.
Z = sqrt(R^2 + (XL - Xc)^2)
24-4: Inductors in AC Circuits
The voltage across an inductor results from the
induced emf due to a changing current through the inductor.
The voltage across the inductor is maximum when the
current is a minimum (but maximum slope), so the voltage leads the
current by 90 deg.
In a phasor diagram, the voltage of across an
inductor is drawn at an angle that is 90 degrees counterclockwise from
the current phasor.
Tip: You can remember that V(L)
points to the left since it is on the left side of I.
The current through the inductor can be found from I
= V/XL, where XL = wL is the inductive reactance.
Prob.44 -
What is Irms at high and low frequencies?
24-5: RLC Circuits
Phase angle - remember: ELI the ICE man
Prob.64 - Is
fo more or less than 60 Hz based on the phasor
diagram? What is
the impedance at resonance?
24-6: Resonance in Electrical
Circuits
RLC circuits have natural frequencies, similar to a
pendulum or a mass on a spring.
w = 1/sqrt(LC)
Prob.59 - If
L and C are both doubled, what happens to the resonance frequency?
Demo:
RLC circuit with digital oscilloscope
Concept
Tests - Ch. 21