Physics 2102 Gabriela GonzálezdA A magnetic field can create a en electrical current too! If we define magnetic flux, similar to definition of electric flux, but for an open surface with an edge: B n • Take note of the MINUS sign!! • The induced EMF acts in such a way that it OPPOSES the change in magnetic flux (“Lenz’s Law”). Then a time varying magnetic FLUX creates an induced EMF, and thus an electrical current if the edge is a wire!:• When the N pole approaches the loop, the flux “into” the loop (“downwards”) increases • The loop can “oppose” this change if a current were to flow clockwise, hence creating a magnetic flux “upwards.” • So, the induced EMF is in a direction that makes a current flow clockwise. • If the N pole moves AWAY, the flux “downwards” DECREASES, so the loop has a counter clockwise current!• A non-magnetic (e.g. copper, aluminum) ring is placed near a solenoid. • What happens if: – There is a steady current in the solenoid? – The current in the solenoid is suddenly changed? – The ring has a “cut” in it? – The ring is extremely cold?• Drop a non-magnetic pendulum (copper or aluminum) through an inhomogeneous magnetic field • What do you observe? Why? (Think about energy conservation!) N S Pendulum had kinetic energy What happened to it? Isn’t energy conserved??• The gap between the spark plug in a combustion engine needs an electric field of ~107 V/m in order to ignite the air-fuel mixture. For a typical spark plug gap, one needs to generate a potential difference > 104 V! • But, the typical EMF of a car battery is 12 V. So, how does a spark plug work?? spark 12V The “ignition coil” is a double layer solenoid: • Primary: small number of turns -- 12 V • Secondary: MANY turns -- spark plug http://www.familycar.com/Classroom/ignition.htm • Breaking the circuit changes the current through “primary coil” • Result: LARGE change in flux thru secondary -- large induced EMF!dA • We saw that a time varying magnetic FLUX creates an induced EMF in a wire, exhibited as a current. • Recall that a current flows in a conductor because of electric field. • Hence, a time varying magnetic flux must induce an ELECTRIC FIELD! • Closed electric field lines!!?? No potential!! B n Another of Maxwell’s equations! To decide SIGN of flux, use right hand rule: curl fingers around loop, +flux -- thumb.• The figure shows two circular regions R1 & R2 with radii r1 = 1m & r2 = 2m. In R1, the magnetic field B1 points out of the page. In R2, the magnetic field B2 points into the page. • Both fields are uniform and are DECREASING at the SAME steady rate = 1 T/s. • Calculate the “Faraday” integral for the two paths shown. R1 R2 I II Path I: Path II:• A long solenoid has a circular cross-section of radius R. • The current through the solenoid is increasing at a steady rate di/dt. • Compute the variation of the electric field as a function of the distance r from the axis of the solenoid. R First, let’s look at r < R: Next, let’s look at r > R: magnetic field lines electric field linesr E(r) r = RTwo versions of Faradays’ law: – A varying magnetic flux produces an EMF: – A varying magnetic flux produces an electric
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