w11d3
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W11D3. Magnetic Forces. Reminder. EXAMINATION #3 Wednesday November 9 th. Calendar Thing. Today (Watch for last WA before exam. Sorry about the intensity of these!) Quiz Who wants to present their experimental results? Collected now! - PowerPoint PPT PresentationTRANSCRIPT
W11D3Magnetic Forces
EXAMINATION #3Wednesday
November 9th
Reminder
Calendar Thing Today (Watch for last WA before exam. Sorry about the
intensity of these!) Quiz Who wants to present their experimental results?
Collected now! Some Problems (No Evan Show! He is cutting class today)) Continue with Forces
Next Week Monday - As much of remainder of chapter as possible.
Nothing DIFFICULT from this session will be on exam. Wednesday Exam
Second Hour & Friday … moving along!
FINAL EXAMINATION Monday morning – December 3rd 7:30AM Physical Science Building First Floor Conference Room Location is SECRET!! TWO index cards allowed Calculator Writing Instrument YOU. More
Info Later
In the circuit shown below, the emf of the battery is 7.6 volts. Resistor R1 has a resistance of 33 ohms, resistor R2 has a resistance of 47 ohms, and resistor R3 has a resistance of 57 ohms. A steady current flows through the circuit.a) What is the equivalent resistance of R1 and R2?
(b) What is the equivalent resistance of all the resistors: R1, R2, and R3
(c) What is the conventional current through R3?
Switch S in the figure below is closed at time t = 0, to begin charging an initially uncharged capacitor of capacitance C = 10.0 µF through a resistor of resistance R = 16.0 W . At what time is the electric potential across the capacitor equal to that across the resistor? t = 0.111 ms
In the circuit of the figure below, = 2.0 kV, C = 5.5 µF, R1 = R2 = R3 = 0.63 MΩ. With C completely uncharged, switch S is suddenly closed (at t = 0).
a) At t = 0, what is current i1 in resistor 1? 0.00212 A
(b) At t = 0, what is current i2 in resistor 2? 0.00106 A
(c) At t = 0, what is current i3 in resistor 3? 0.00106 A
Repeat for t = infinity (that is, after many time constants.)
(d) What is current i1? 0.00159 A
(e) What is current i2? 0.00159 A
(f) What is current i3? 0 A
(g) What is the potential difference V2 across resistor 2 at t = 0? 667 V
(h) What is V2 at t = ? 1000 V
(i) Sketch V2 versus t between these two extreme times. (Do this on paper. Your instructor may ask you to turn in this sketch.)
In the figure below, the battery has a potential difference of 10.0 V and the five capacitors each have a capacitance of 16.0 µF.
(a) What is the charge on capacitor 1? 0.00016 C
(b) What is the charge on capacitor 2? 3.2e-05 C
MORE ON FORCESRemember Bil?
Bil
Opposites don’t always attract!FORCES BETWEEN WIRES
The Wire in More Detail – Conventional
:
in the direction of the motion of POSITIVE charge (I).
d
d dd
Lq I t I
vL
F qv B I v B ILBv
vectorI
Vector
F L B
L
B out of plane of the paper
Assume all electrons are moving with the same velocity vd.
L
Think “BIL”
I
We usually calculate force per unit length.
TWO WIRES
0 24
IB
r
Now we can calculate the magnitude of the magnetic force F21 exerted on the lower wire by the field produced by the upper wire:
u sing the right-hand rule with , the direction of the force is up, so that the lower wire is attracted to the upper wire.
IΔL×B
0 121 2
24
IF I L
d
TWO WIRES
B
Let’s Get Dizzy!
+ + + +
+ + + +
+ + + +
+ + + +
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vB
F
+ + + +
+ + + +
+ + + +
+ + + +
+ + + +
vB
F
(B field points into plane of paper.)
Magnetic Force is a centripetal force
Trajectory of Charged Particlesin a Magnetic Field
16
Review of Rotational Motion
atar
at = r tangential accelerationar = v2 / r radial acceleration
The radial acceleration changes the direction of motion,while the tangential acceleration changes the speed.
r s = s / r s = r ds/dt = d/dt r v = r
= angle, = angular speed, = angular acceleration
Uniform Circular Motion
= constant v and ar constant but direction changes
ar = v2/r = 2 rF = mar = mv2/r = m2r
KE = ½ mv2 = ½ mw2r2
v
ar
Radius of a Charged ParticleOrbit in a Magnetic Field
+ + + +
+ + + +
+ + + +
+ + + +
+ + + +
vB
F
r
2 vv
v
mq B
r
mr
qB
Centripetal Magnetic Force Force =
Note: as , the magneticforce does no work!
Fv
Cyclotron Frequency
+ + + +
+ + + +
+ + + +
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vB
F
r
The time taken to complete one orbit is:
qBm
rT
vv
2v
2
mqBf
mqB
Tf
c
2
21
More Circular Type Motion in a Magnetic Field
19
Magnetic Sector - Mass Spectrometer20
vmr
qB
VelocitySelector
How Old is That?? Activity
Low Resolution Mass Spectrum
SIMS
THAT’S ALL THERE IS!Magnetic Forces on Charges