W09D2: Faraday’s Law Today’s Reading Assignment Course Notes: Sections 10.1-10.6 1 Outline Faraday’s Law Applications of Faraday’s Law Problem Solving Experiment 3: Faraday’s Law 2 Faraday’s Law of Induction dΦ B ∝ I induced dt Changing magnetic flux induces a current 3 1 Demonstration: Induction and Simulation of Induction 4 Demo: Electromagnetic Induction http://web.mit.edu/viz/EM/visualizations/faraday/faradaysLaw/faradayapp/faradayapp.htm 5 Demonstration: Magnet Falling Through Plastic Tube and Aluminum Tube 6 2 Demonstration: Jumping Ring An aluminum ring jumps into the air when the solenoid beneath it is energized 7 What is Going On? This is a dramatic example of Faraday’s Law and Lenz’s Law: When current is turned on through the solenoid the created magnetic field tries to permeate the conducting aluminum ring, currents are induced in the ring to try to keep this from happening, and the ring is repelled upwards. 8 Magnetic Flux Thru Wire Loop Analogous to Electric Flux (Gauss’ Law) (1) Uniform B Φ B = B⊥ A = B Ac o sθ = B ⋅ A (2) Non-Uniform B Φ B = ∫∫ B ⋅ d A S 9 3 Concept Question: Loop in Uniform Field While a rectangular wire loop is pulled upward though a uniform magnetic field B field penetrating its bottom half, as shown, there is 1. a current in the loop. 2. no current in the loop. 3. I do not understand the concepts of current and magnetic field. 4. I understand the concepts of current and magnetic field but am not sure of the answer. 10 Concept Q.: Loop in Uniform Field While a rectangular wire loop is pulled sideways though a uniform magnetic field B field penetrating its bottom half, as shown, there is 1. a current in the loop. 2. no current in the loop. 3. I do not understand the concepts of current and magnetic field. 4. I understand the concepts of current and magnetic field but am not sure of the answer. 11 Electromotive Force (EMF) ε = ∫ E ⋅ d s closd path Looks like electric potential. It’s a “driving force” for current If a conducting closed path is present for charge carriers then the electric field exerts forces on charge carriers producing and induced current ε = IR 12 4 Minus Sign? Lenz’s Law ε = − dΦ B dt Induced EMF is in direction that opposes the change in flux that caused it 13 Sign Conventions: Right Hand Rule d E⋅ds = − B⋅dA ∫∫ dt open surface closed path ∫ Integration direction clockwise for line integral requires that unit normal points into page for open surface integral Magnetic flux positive into page, negative out of page 14 : Sign Conventions: Right Hand Rule d E⋅ds = − B⋅dA ∫∫ dt open surface closed path ∫ Integration direction counterclockwise for line integral requires that unit normal points out of page for open surface integral Magnetic flux positive out of page, negative into page : 15 5 Concept Question: Loop The magnetic field through a wire loop is pointed upwards and increasing with time. The induced current in the coil is 1. Clockwise as seen from the top 2. Counterclockwise 16 Concept Question: Moving Loop A circuit in the form of a rectangular piece of wire is pulled away from a long wire carrying current I in the direction shown in the sketch. The induced current in the rectangular circuit is 1. Clockwise 2. Counterclockwise 3. Neither, the current is zero 17 Concept Question: Faraday’s Law: Loop A coil moves up from underneath a magnet with its north pole pointing upward. The current in the coil and the force on the coil: 1. 2. 3. 4. Current clockwise; force up Current counterclockwise; force up Current clockwise; force down Current counterclockwise; force down 18 6 Faraday’s Law Problem Solving 19 Ways to Induce EMF ε=− d BAcosθ dt ( ) Quantities which can vary with time: • Magnitude of B • Area A enclosed by the loop • Angle between B and normal vector to loop 20 Problem: Changing Area Conducting rod pulled along two conducting rails in a uniform magnetic field B at constant velocity v 1. 2. 3. 4. 5. Find the direction of induced current. Find the direction of resultant force. What is the magnitude of EMF? What is the magnitude of current? What is the external power supplied to move at constant v? That is, calculate Fext dot v. 6. What is the Joule heating rate in the circuit, I2R, and how does it relate to the answer in (5)? 21 7 Faraday’s Law of Induction If C is a stationary closed curve and S is a surface spanning C then d E ⋅ d s = − C∫ dt B ⋅ d A ∫∫ S The changing magnetic flux through S induces a non-electrostatic electric field whose line integral around C is non-zero 22 Problem: Calculating Induced Electric Field Consider a uniform magnetic field which points into the page and is confined to a circular region with radius R. Suppose the magnitude increases with time, i.e. dB/dt > 0. Find the magnitude and direction of the induced electric field in the regions (i) r < R, and (ii) r > R. (iii) Plot the magnitude of the electric field as a function r. 23 Experiment 3: Faraday’s Law of Induction 24 8