1 / 15

Faraday's Law: Induced EMF, Flux Change, Lenz’s Law, Proof, Examples

Learn about Faraday's Law of induction, including the induction of EMF, the change in flux, Lenz's Law, and proof. Explore examples of induced current and EMF calculations.

vaughanm
Télécharger la présentation

Faraday's Law: Induced EMF, Flux Change, Lenz’s Law, Proof, Examples

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. DF ε = - N D t DF ε = - (N = number of turns) D t An emf (ε) is induced in a conducting loop whenever the magnetic flux () is changing. Faraday’s Law Notes: 1) /t = rate of change of flux 2) Induced emf causes induced current in the loop 3) Induced current causes its own magnetic field 4) This new B-field direction opposes the change in the original one. This part is called Lenz’s Law. 5) If there are multiple loops (Solenoid): Flux linking coil = 3 5 2 4

  2. Faraday’s Law Change in Flux Induced emf Time for Change Lenz’s Law Number of Turns

  3. Dt B v x Dx Proof 1 At t = 0 Fo = BA = BLx L After Dt F = Fo + DF F = BLx + BLDx DF = BLDx DF = BL(vDt)

  4. L q F v Force on charge v Proof 2 Work done by force EMF

  5. B F = Ee L F = Bev + • A rod of length L moves perpendicular to a field B at speed v. • Using the Slap hand rule means electrons pushed to front • F = Bqv (here q = e) • As more electrons get pushed to front an electric field grows • Electric force (F=Eq) will balance magnetic force • Eq = Bqv • Let E = ε / L (assume the rod is a capacitor ~ E=V/d) + - - Eq = Bqv (ℇ/L) q = Bqv ℇ/L = Bv ℇ = BLv ℇ = BLv Proof 3

  6. Magnetic flux will change if the angle between the loop and the field changes:

  7. Magnetic flux will change if the area of the loop changes:

  8. x x x x x x x x x x x x x x x x 20 cm B = 2.0 T 20 cm 3. The wire loop has a resistance of 20 m. If its area is reduced to zero in a time of .20 s, find the magnitude and direction of the induced current.

  9. 1. A 9.6-cm-diameter circular loop of wire is in a 1.10-T magnetic field. The loop is removed from the field in 0.15 s. What is the average induced emf? 2. A 10.2-cm-diameter wire coil is initially oriented so that its plane is perpendicular to a magnetic field of 0.63 T pointing up. During the course of 0.15 s, the field is changed to one of 0.25 T pointing down. What is the average induced emf in the coil?

  10. 3. The moving rod is 12.0 cm long and is pulled at a speed of 15.0 cm/s. If the magnetic field is 0.800 T, calculate (a) the emf developed in the rod. (b) the electric field felt by electrons in the rod.

  11. 4. The moving rod is 13.2 cm long and generates an emf of 120 mV while moving in a 0.90-T magnetic field. (a) What is its speed? (b) What is the electric field in the rod?

  12. 5. The rod moves with a speed of 1.6 m/s is 30.0 cm long, and has a resistance of 2.5 W. The magnetic field is 0.35 T, and the resistance of the U-shaped conductor is 25 W at a given instant. Calculate (a) the induced emf, (b) the current in the U-shaped conductor (c) the external force needed to keep the rod’s velocity constant at that instant.

  13. 6. A square loop 24.0 cm on a side has a resistance of 5.20 Ω. It is initially in a 0.665-T magnetic field, with its plane perpendicular to B but is removed from the field in 40.0 ms. Calculate the electric energy dissipated in this process.

More Related