Faraday's Law - University of Hawaiifah/272www/272lectures/fall...In Faraday’s Law, we can induce...

15
Faraday's Law dA B B A d B Φ B r r dt d Φ ε B =

Transcript of Faraday's Law - University of Hawaiifah/272www/272lectures/fall...In Faraday’s Law, we can induce...

Page 1: Faraday's Law - University of Hawaiifah/272www/272lectures/fall...In Faraday’s Law, we can induce EMF in the loop when the magnetic flux, Φ B, changes as a function of time. There

Faraday's Law

dA

B B

∫ •≡ AdBΦBrr

dtdΦε B−=

Page 2: Faraday's Law - University of Hawaiifah/272www/272lectures/fall...In Faraday’s Law, we can induce EMF in the loop when the magnetic flux, Φ B, changes as a function of time. There

Faraday’s Law of Induction

dtdAdB

dtd BΦ−=∫ ⋅−=

rrε

Recall the definition of magnetic flux is

Faraday’s Law is the induced EMF in a closed loop equal thenegative of the time derivative of magnetic flux change in the loop,

∫ ⋅=Φ AdBBrr

Constant B field,no induced EMFin loop

changing B field,causes induced EMFin loop

Page 3: Faraday's Law - University of Hawaiifah/272www/272lectures/fall...In Faraday’s Law, we can induce EMF in the loop when the magnetic flux, Φ B, changes as a function of time. There

Getting the sign EMF in Faraday’s Law of Induction

Define the loop and an area vector, A, who magnitude is theArea and whose direction normal to the surface.

The choice of vector A direction defines the direction of EMFwith a right hand rule. Your thumb in A direction and then yourfingers point to positive EMF direction.

A

Page 4: Faraday's Law - University of Hawaiifah/272www/272lectures/fall...In Faraday’s Law, we can induce EMF in the loop when the magnetic flux, Φ B, changes as a function of time. There
Page 5: Faraday's Law - University of Hawaiifah/272www/272lectures/fall...In Faraday’s Law, we can induce EMF in the loop when the magnetic flux, Φ B, changes as a function of time. There

Lenz’s Law – easier way!

Heinrich Friedrich Emil Lenz(1804-1865)

The direction of any magnetic inductioneffect is such as to oppose the cause ofthe effect.

Example if an external magnetic field on a loopis decreasing, the induced current creates a field parallel to the that tends to increase thenet field.

⇒ Convenient method to determine I direction

Example if an external magnetic field on a loopis increasing, the induced current creates a fieldopposite that reduces the net field.

Page 6: Faraday's Law - University of Hawaiifah/272www/272lectures/fall...In Faraday’s Law, we can induce EMF in the loop when the magnetic flux, Φ B, changes as a function of time. There

Incredible shrinking loop: a circular loop of wirewith a magnetic flux is shrinking with time. Inwhich direction is the induced current?

(a) There is none. (b) CW. (c) CCW

X X X X X X

X X X X X X

X X X X X X

X X X X X X

Page 7: Faraday's Law - University of Hawaiifah/272www/272lectures/fall...In Faraday’s Law, we can induce EMF in the loop when the magnetic flux, Φ B, changes as a function of time. There

Determine the direction of current in a – b when

1.) Switch is opened after having been closed for a long time.

(a) No current. (b) left to right. (c) right to left.

2.) The resistance R is decreased while switch remains closed.

(a) No current. (b) left to right. (c) right to left.

Page 8: Faraday's Law - University of Hawaiifah/272www/272lectures/fall...In Faraday’s Law, we can induce EMF in the loop when the magnetic flux, Φ B, changes as a function of time. There

Slide Wire Generator

The area is LS(t) and dS/dt equals velocity of slider

S

BLvSdtdBLBLS

dtdBA

dtd

dABdtdAdB

dtd

dtd

B

−=−=−=−=

−=•−=Φ−= ∫∫rr

ε

Page 9: Faraday's Law - University of Hawaiifah/272www/272lectures/fall...In Faraday’s Law, we can induce EMF in the loop when the magnetic flux, Φ B, changes as a function of time. There

S

BLv=ε

Slide Wire Generator; work and powerwe found

we now ask what ispower dissipated, Pdand power applied, Paassume total resistanceis R, then I=Ɛ/R andPd =I2R=B2L2v2/R

The power applied, Pa=Fv, is the rate of work to the bar to the right against the force, F, which is pointed to the left. F=ILB= (Ɛ/R)LB = B2L2v/R. Thus Pa= Fv = B2L2v2/R = Pd and we find the power put into the moving the bar equals the heat dissipated in the circuit.

⇒ Power needed to move bar = Power dissipated in circuit

Page 10: Faraday's Law - University of Hawaiifah/272www/272lectures/fall...In Faraday’s Law, we can induce EMF in the loop when the magnetic flux, Φ B, changes as a function of time. There

S

Slide Wire Generator; use Lenz’s Law to get I direction

Lenz’s Law saysdirection creates fieldthat opposes changein magnetic flux.

If we pull bar to right, the net magnetic flux in rectangle increasesinto screen, hence the I direction must induce opposite B field which is out of screen and is correct in drawing.

Suppose Lenz’s law were reversed, then I would be reversed and F would go right and the bar would be accelerated to the right, w/o need of external positive work and heat would be dissipated at the same time. This violates Conservation of Energy, so Lenz’s law is correct.

Page 11: Faraday's Law - University of Hawaiifah/272www/272lectures/fall...In Faraday’s Law, we can induce EMF in the loop when the magnetic flux, Φ B, changes as a function of time. There

Motional Electromotive Force

In Faraday’s Law, we can induce EMF in the loop when the magnetic flux, ΦB, changes as a function of time. There are twoCases when ΦB is changing,1) Change the magnetic field (non-constant over time) 2) Change or move the loop in a constant magnetic field

dtdAdB

dtd BΦ−=∫ ⋅−=

rrε

The slide wire generator is an example of #2 and the induction ofEMF via moving parts of the loop is called, motional EMF.

Page 12: Faraday's Law - University of Hawaiifah/272www/272lectures/fall...In Faraday’s Law, we can induce EMF in the loop when the magnetic flux, Φ B, changes as a function of time. There

Alternator Generator Wire loop area A rotates with respect to constant magnetic field.

If the angular frequency is ω, then

and EMF in the loop is

φcosBAAdBB ∫ =•=Φrr

( )tBAB ωcos=Φ

( )tBAdtd

B ωω sin−=Φ

( )tBAdtd

B ωωε sin=Φ−=

Page 13: Faraday's Law - University of Hawaiifah/272www/272lectures/fall...In Faraday’s Law, we can induce EMF in the loop when the magnetic flux, Φ B, changes as a function of time. There

Slide Wire Generator; revisited again

Suppose we move a conducting bar in a constant B field, then a forceFB =q v×B moves + charge up and – charge down. The charge distribution produces an electric field, E, force, FE, and EMF, Ɛ, between a & b. This continues until equilibrium is reached: FE = -FB.

BvqBvq

qF

qF

E BErr

rrrrr

×−=×

−=−

== vBlldEb

a=∫ ⋅=

rrε

In effect the bar motional EMF is an equivalent to a battery EMF

B

EE

Page 14: Faraday's Law - University of Hawaiifah/272www/272lectures/fall...In Faraday’s Law, we can induce EMF in the loop when the magnetic flux, Φ B, changes as a function of time. There

Slide Wire Generator; revisited again

vBlldEb

a

=⋅= ∫rr

ε

If the rod is on the U shaped conductor, the charges don’t build up at the ends but move around the U shaped portion. They produce an electric field in the U shaped circuit. The wire acts as a source of EMF – just like a battery. Called motional electromotive force.

Page 15: Faraday's Law - University of Hawaiifah/272www/272lectures/fall...In Faraday’s Law, we can induce EMF in the loop when the magnetic flux, Φ B, changes as a function of time. There

Direct Current Homopolar Generator invented by Faraday

Rotate a metal disk in a constant perpendicular magnetic field. The charges in the disk when movingreceive a radial force. The causescurrent to flow from center to pointb.

Faraday’s originalapparatus had the diskfixed with a meter and thenhe spun a magnet underthe disk.

2

0 21 BRdrBr

Rωωε == ∫