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PHYSICS 51: Ch. 27 lectures

PHYSICS 51: Ch. 27 lectures. Homework #8: Magnetic Fields. Read Ch. 27.1 - 27.7 We will talk a bit in class about sections 8 and 9 also Do Exercises : Ch 27, #1, # 16, # 42, #46, #74 Due: Thursday April 3. 2014. First Section Electric Forces Electric Fields Electric Potential

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PHYSICS 51: Ch. 27 lectures

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  1. PHYSICS 51: Ch. 27 lectures

  2. Homework #8: Magnetic Fields • Read Ch. 27.1 - 27.7 • We will talk a bit in class about sections 8 and 9 also • Do Exercises :Ch 27, #1, #16, #42, #46, #74 • Due: Thursday April 3. 2014

  3. First Section Electric Forces Electric Fields Electric Potential Second Section Resistance Capacitance DC Circuits Third Section Magnetic Forces Magnetic Fields Induction Fourth Section AC Circuits Electromagnetic Fields (Waves) Physics 51

  4. Magnetic Fields • Big difference between Electric and Magnetic fields is that there in no magnetic monopole • No simple source of the field (see Maxwell’s Equations) • Magnetic field created by moving charge! • Field interacts with another moving charge • Text Ch 27: How charge reacts to Magnetic field • Text Ch 28: How to create Magnetic field

  5. MAXWELL’S EQUATIONS The relationships between electric and magnetic fields and their sources can be stated compactly in four equations, called Maxwell’s equations. Together they form a complete basis for the relation of E and B fields to their sources. C 2004 Pearson Educational / Addison Wesley

  6. Earth’s magnetic field (Note the N-S polls of magnet!)

  7. Earth’s Magnetic Field • Earth’s magnetic field caused by convection currents in the molten core (we think) • Compass • Invented 2,000 years ago in China, used more for Fung Shui than navigation • Critical to the age of sail and exploration • Magnetic north pole and rotational north pole far apart • Magnetic north pole moves around • Field flips every few thousand years • Provides protection from cosmic rays • Connection between magnetic field and electric currents first observed about 1820 until then thought of as separate subjects

  8. Earth’s Magnetic Field • Earth’s magnetic field caused by convection currents in the molten core (we think) • Compass • Invented 2,000 years ago in China, used more for Fung Shui than navigation • Critical to the age of sail and exploration • Magnetic north pole and rotational north pole far apart • Magnetic north pole moves around • Field flips every few thousand years • Provides protection from cosmic rays • Connection between magnetic field and electric currents first observed about 1820 until then thought of as separate subjects

  9. Magnetic force acting on a moving (+) charge

  10. Example: Force Calculation An proton, with a speed of 1 x 106 m/s enters a region where the magnetic field is into the paper. The field strength is .1 T. What is the pattern of the flight of the proton. What is the rdius of curvature? mp= 1.6 x 10-28 Kg, e = 1.6 x 10-19 C

  11. Particle in Constant Magnetic Field Orbit of a charged particle in a uniform magnetic field is a circle R = m v / q B

  12. Example #2 • An electron comes out of the board at the front of the room. Assume the local magnetic field is up toward the sky. Which direction is the electron bent?

  13. Plan for the day • Moving Charge in Magnetic Field • Mass Spectroscopy • Force on a current in a wire • Audio Speaker • Torque on a loop in a Magnetic Field • DC Electric Motor • Quiz

  14. Fields and forces: Review Electric Field • Charge creates field (E) • Field interacts with different charge causing force Magnetic Field • Moving charge creates field (B) (Ch 28) • Vector field like E • Field interacts with moving charge causing force • Unit of B is T (Tesla) = N/Am • 104 Gauss = 1 T

  15. Magnetic force acting on a moving (+) charge Force is perpendicular to both velocity and field

  16. q v B = q E v = E / B Velocity selector for charged particles uses perpendicular E and B fields, only one velocity goes straight

  17. Mass Spectrometer

  18. Commercial Application of Mass Spectroscopy

  19. I Force on a moving positive charge in a current-carrying conductor: L F = I L x B For vector direction use “RIGHT HAND RULE” I

  20. Right hand rule F = I L x B Magnetic force on a straight wire carrying current Iin a magnetic field B

  21. Example A 10.0 cm segment of wire carries a 5.0A current as shown. It is in a uniform 2.0T magnetic field. What is the magnitude and direction of the force on the wire? What orientation gives a maximum force? B field Wire, 45 degrees to field

  22. A rail gun! F = I L x B

  23. Components of a loudspeaker F = I l x B

  24. Dynamic Loudspeaker Principle A current-carrying wire in a magnetic field experiences a magnetic force perpendicular to the wire.

  25. Loop of current A square loop of wire, 10.0 cm on a side sits in the xy plane. It carries a current I0.0 mA through the loop going clockwise when viewed from above. The loop sits in a constant magnetic field of 0.5T in the +x direction. • What is the magnitude of the net force on the loop • What is the magnitude of the net torque on the loop

  26. Forces on the sides of a current-carrying loop in a uniform magnetic field.This is how a motor works!

  27. Magnetic Moment • Electric Dipole Moment • Definition: p = qd • Torque:  = p x E • Magnetic Dipole Moment • Definition  = niA • Torque  =  x B

  28. Magnetic Moment Right hand rule determines the direction of the magnetic moment () of a current-carrying loop

  29. Torque (m x B) on this solenoid in a uniform magnetic field is into the screen thus rotating the solenoid clockwise

  30. DCElectricMotor

  31. A simple DC motor

  32. Magnetic Moment Right hand rule determines the direction of the magnetic moment () of a current-carrying loop

  33. Torque (m x B) on this solenoid in a uniform magnetic field is into the screen thus rotating the solenoid clockwise

  34. Atomic Magnetic Moments • Electrons and Protons also have magnetic moments (spin) • Zeemann effect is the splitting of and atomic transition based on the energy associated with the electron spin in an magnetic field • Atoms have magnetic moments associated with electron “orbiting” the nucleus • Ferromagnetic Materials have “domains” of aligned magnetic moments • You can expand domains with applied magnetic field • Iron can be made into a permanent magnet

  35. Magnets are aligned magnetic moments Atomic magnetic moments in an iron bar (a) unmagnetized (b) magnetized (c)Torque on a bar magnet in a B field

  36. If the Field is non-uniform you can cause a net force Current loops in a non-uniform B field

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