Reading Quiz 4 - University of Florida · PHY2054: Chapter 20 15 Reading Quiz 4 ÎFaraday’s law...
Transcript of Reading Quiz 4 - University of Florida · PHY2054: Chapter 20 15 Reading Quiz 4 ÎFaraday’s law...
15PHY2054: Chapter 20
Reading Quiz 4Faraday’s law says that1. an emf is induced in a loop when it moves through an electric
field2. the induced emf produces a current whose magnetic field
opposes the original change3. the induced emf is proportional to the rate of change of magnetic
flux
Faraday’s law
16PHY2054: Chapter 20
ConcepTest: Lenz’s Law If a North pole moves towards the loop from above the page, in what direction is the induced current?
(a) clockwise (b) counter-clockwise (c) no induced current
Must counter flux change indownward direction with upward B field
17PHY2054: Chapter 20
ConcepTest: Induced Currents A wire loop is being pulled through a uniform magnetic field. What is the direction of the induced current?
(a) clockwise (b) counter-clockwise (c) no induced current
x x x x x x x x x x x x xx x x x x x x x x x x x xx x x x x x x x x x x x xx x x x x x x x x x x x xx x x x x x x x x x x x xx x x x x x x x x x x x xx x x x x x x x x x x x x
No change in flux, no induced current
18PHY2054: Chapter 20
ConcepTest: Induced Currents
In the cases above, what is the direction of the induced current?
x x x x x x x x x x x x x x x x x x x x x x x x xx x x x x x x x x x x x x x x x x x x x x x x x xx x x x x x x x x x x x x x x x x x x x x x x x xx x x x x x x x x x x x x x x x x x x x x x x x xx x x x x x x x x x x x x x x x x x x x x x x x xx x x x x x x x x x x x x x x x x x x x x x x x xx x x x x x x x x x x x x x x x x x x x x x x x xx x x x x x x x x x x x x x x x x x x x x x x x x
1
2
Counterclockwise None
19PHY2054: Chapter 20
ConcepTest: Lenz’s Law If a coil is shrinking in a B field pointing into the page, in what direction is the induced current?
(a) clockwise (b) counter-clockwise (c) no induced current
Downward flux is decreasing,so need to create downwardB field
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Induced currents A circular loop in the plane of the paper lies in a 3.0 T magnetic field pointing into the paper. The loop’s diameter changes from 100 cm to 60 cm in 0.5 s
What is the magnitude of the average induced emf?What is the direction of the induced current?If the coil resistance is 0.05Ω , what is the average induced current?
Direction = clockwise (Lenz’s law)
Current = 3.016 / 0.05 = 60.3 A
( )2 20.3 0.53.0 3.016 Volts
0.5BV
t
π −ΔΦ= = × =
Δ
21PHY2054: Chapter 20
ConcepTest: Induced Currents A wire loop is pulled away from a current-carrying wire. What is the direction of the induced current in the loop?
(a) clockwise (b) counter-clockwise (c) no induced current
I
Downward flux through loopdecreases, so need to createdownward field
22PHY2054: Chapter 20
ConcepTest: Induced Currents A wire loop is moved in the direction of the current. What is the direction of the induced current in the loop?
(a) clockwise (b) counter-clockwise (c) no induced current
I
Flux does not change whenmoved along wire
23PHY2054: Chapter 20
ConcepTest: Lenz’s Law If the B field pointing out of the page suddenly drops to zero, in what direction is the induced current?
(a) clockwise (b) counter-clockwise (c) no induced current
If a coil is rotated as shown, in a B field pointing to the left, in what direction is the induced current?
(a) clockwise (b) counter-clockwise (c) no induced current
Upward flux through loopdecreases, so need to createupward field
Flux into loop is increasing, soneed to create field out of loop
24PHY2054: Chapter 20
ConcepTest: Induced CurrentsWire #1 (length L) forms a one-turn loop, and a bar magnet is dropped through. Wire #2 (length 2L) forms a two-turn loop, and the same magnet is dropped through. Compare the magnitude of the induced currents in these two cases.
(a) I1 = 2 I2
(b) I2 = 2 I1
(c) I1 = I2 ≠ 0(d) I1 = I2 = 0(e) Depends on the strength of the magnetic field
Voltage doubles, but R alsodoubles, leaving current the same
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Motional EMFConsider a conducting rod moving on metal rails in a uniform magnetic field:
( ) ( )ε Φ= = = =Bd d BA d BLx dxBL
dt dt dt dt
x
x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x x xx x x x x x x x x
v L ε = BLv
Current will flow counter-clockwise in this “circuit”. Why?
26PHY2054: Chapter 20
Force and Motional EMFPull conducting rod out of B field
Current is clockwise. Why?
Current within B field causes force
Force opposes pull (RHR)Also follows from Lenz’s law
We must pull with this forceto maintain constant velocity
ε= =
BLviR R
2 2= =
B L vF iLBR
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Power and Motional EMFForce required to pull loop:
Power required to pull loop:
Energy dissipation through resistance
Same as pulling power! So power is dissipated as heatKinetic energy is constant, so energy has to go somewhereRod heats up as you pull it
2 2= =
B L vF iLBR
2 2 2= =
B L vP FvR
2 2 2 22 ⎛ ⎞= = =⎜ ⎟
⎝ ⎠BLv B L vP i R R
R R
28PHY2054: Chapter 20
ExamplePull a 30cm x 30cm conducting loop of aluminum through a 2T B field at 30cm/sec. Assume it is 1cm thick.
Circumference = 120cm = 1.2m, cross sectional area = 10-4 m2
R = ρL/A = 2.75 x 10-8 * 1.2 / 10-4 = 3.3 x 10-4 Ω
EMF
Current
Force
Power
2 0.3 0.3 0.18Vε = = × × =BLv
4/ 0.18 / 3.3 10 545Aε −= = × =i R
2 98W= =P i RAbout 0.330 C per sec(from specific heat, density)
545 0.3 2 327 NF iLB= = × × = 74 lbs!
29PHY2054: Chapter 20
Electric GeneratorsRotate a loop of wire in a uniform magnetic field:
changing θ ⇒ changing flux ⇒ induced emfΦB = B A cos θ = B A cos(ωt)
Rotation: θ = ωt
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Electric GeneratorsFlux is changing in a sinusoidal manner
Leads to an alternating emf (AC generator)
cos( ) sin( )Bd d tN NBA NBA tdt dt
ω ω ωε Φ= = =
This is how electricity is generated
Water or steam (mechanical power) turns the blades of a turbine which rotates a loop
Mechanical power converted to electrical power
31PHY2054: Chapter 20
ConcepTest: GeneratorsA generator has a coil of wire rotating in a magnetic field. If the B field stays constant and the area of the coil remains constant, but the rotation rate increases, how is the maximum output voltage of the generator affected?
(a) Increases (b) Decreases (c) Stays the same(d) Varies sinusoidally
sin( )ω ωε = NBA t
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Induction in Stationary CircuitSwitch closed (or opened)
Current induced in coil B (direction shown is for closing)
Steady state current in coil ANo current induced in coil B
A
B
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Self - InductanceConsider a single isolated coil:
Current (red) starts to flow clockwise due to the batteryBut the buildup of current leads to changing flux in loopInduced emf (green) opposes the change
d diN Ldt dt
ε Φ=− =−
L is the self-inductanceunits = “Henry (H)”
induced emf
This is a self-induced emf (also called “back” emf)
12V
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Inductance of SolenoidTotal flux (length l)
( )( ) 20μΦ = =BN nl B A n A li
0μ=B in
20
Bd di diN n Al Ldt dt dt
με Φ= − = − = −
20L n Alμ=
To make large inductance:Lots of windingsBig areaLong
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LR CircuitsInductance and resistor in series with battery of EMF V
Start with no initial current in circuitClose switch at t = 0Current is initially 0 (initial increasecauses voltage drop across inductor)
Find i(t)Resistor: ΔVR = RiInductor: ΔVL = L di/dtUse back emf of inductor
VR
L
( ) /LV V V Ldi dti tR R−Δ −
= =
36PHY2054: Chapter 20
Analysis of LR CircuitGeneral solution
( )( )// 1 −= − tR Li V R e
Final current (maximum)
Rise from 0 withtime constant τ = L / R
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L-R Circuits (2)Switch off battery: Find i(t) if current starts at i0
/0
tR Li i e−= Exponential fall to 0 withtime constant τ = L / R
Initial current (maximum)
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Exponential Behaviorτ = L/R is the “characteristic time” of any RL circuit
Only t / τ is meaningful, just like for RC circuit
t = τCurrent falls to 1/e = 37% of maximum valueCurrent rises to 63% of maximum value
t =2τCurrent falls to 1/e2 = 13.5% of maximum valueCurrent rises to 86.5% of maximum value
t =3τCurrent falls to 1/e3 = 5% of maximum valueCurrent rises to 95% of maximum value
t =5τCurrent falls to 1/e5 = 0.7% of maximum valueCurrent rises to 99.3% of maximum value
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ConcepTest: Generators and MotorsA current begins to flow in a wire loop placed in a magnetic field as shown. What does the loop do?
(a) moves to the right (b) moves up (c) rotates around horizontal axis(d) rotates around vertical axis(e) moves out of the page
This is how a motor works !!
B
40PHY2054: Chapter 20
Current is supplied from an external source of emf (battery or power supply)
Forces act to rotate the wire loop
A motor is essentially a generator operated in reverse!
Electric Motors
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MotorForces act to rotate the loop towards the vertical.
When loop is vertical, current switches sign and the forces reverse, in order to keep the loop in rotation.
This is why alternating current is necessary for a motor to operate.
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Motors Generators
Electrical ⇒ mechanical energy Mechanical ⇒ electrical energy
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Reading Quiz 5A generator is a device that:
a) transforms mechanical into electrical energyb) transforms electrical into mechanical energyc) transforms low voltage to high voltage
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Energy of an InductorEnergy is stored in inductor when current flows through it
Energy is stored in the B field
Similar to energy in charged capacitor
Energy is stored in the E field (between plates)
212LU Li=
221
22CqU CVC
= =
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Energy of SolenoidRecall B field of solenoid (current i, n turns per meter)
Inductance of solenoid
Energy of solenoid can be written in terms of B field and volume (V = lA)
0B niμ=
( )( )0 20
B nl niANL n Ali i
μμΦ
= = =
( )2 2
2 21 102 2
0 02LB BU Li n lA Al
nμ
μ μ⎛ ⎞
= = =⎜ ⎟⎝ ⎠
0B BA niAμΦ = =
Energy densityof B field
Volume
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Energy of Solenoid (2)Typical MRI magnet
B = 0.5 – 1.5 TR = 0.25 m, l = 2.5 m
Assume B = 1 T typically
This is a lot of energyNeeds to be held in by strong materials
2 30.5mV Al R lπ= = ≅
( )2 2
70
1 0.5 200 kJ2 2 4 10BBU Vμ π −= = ≈
× ×
47
Energy Density (contd)Typical solid held together ≈ 1eV/(10- 10)3 ≈ 1.6 x 1011 J/m3
In pressure units ≈ 106 Atm
In magnetic field units ≈ B2/2μo B ≈ 700T
These are limits of magnetic fields
In reality, the material strength is capped sooner than a Mega atmosphere (by a factor of 100).
Therefore the limiting field is 60-70T, an estimate.
Perhaps 100T, but be careful.. Tread very carefully..
Magnet Lab (National High Magnetic Field Laboratory) in Tallahassee runs magnets at up to 50T or more.
PHY2054: Chapter 20
48PHY2054: Chapter 20
Gigajoule Magnet at CERNCMS experiment at CERN
p-p collisions at world’s highest energy in 2007Hope to discover new particles, find the origin of mass and new fundamental forces
Compact Muon Solenoid
50PHY2054: Chapter 20
CMS Experiment MagnetLarge central solenoid magnet to study particle production
B = 4T, R = 3.15 m, l = 12.5 mUB = 2.6 x 109 J = 2.6 gigajoules!!
http://www.spacedaily.com/news/energy-tech-04b.html
( )( )2 2
27
0
4 3.15 12.52 2 4 10BBU Al πμ π −= = ×
× ×
51PHY2054: Chapter 20
CMS Articles and PicturesHome page
http://cmsinfo.cern.ch/Welcome.html/
Pictures of detectorhttp://cmsinfo.cern.ch/Welcome.html/CMSdetectorInfo/CMSdetectorInfo.htmlhttp://cmsinfo.cern.ch/Welcome.html/CMSmedia/CMSmedia.html
Interesting article on solenoid, with pictureshttp://cmsinfo.cern.ch/Welcome.html/CMSdocuments/MagnetBrochure/MagnetBrochure.pdf
Other documents & pictures about CMShttp://cmsinfo.cern.ch/Welcome.html/CMSdocuments/CMSdocuments.html