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A. Manalaysay – PHY2054, Fall 2004 CHAPTER 19 This chapter’s an introduction to magnetic fields. Magnetic fields are similar (but a little more complicated) than electric fields. You’re familiar with a bar magnet probably; magnetic field lines point out of a north pole and into a south pole. The Earth’s magnetic field at the surface points north, geographically (i.e. away from Antarctica). But this means the field lines point out of Antarctica, which means that is where the magnetic north pole is. If this is confusing, look at page 589 of your book for a diagram. Magnetic fields can produce a force on a charged particle: ---Magnetic force on a charged particle (magnitude only) “q” is the charge, “v” is the velocity, “B” is the magnetic field, and “ ” is the angle between the magnetic field and the velocity. To find the direction of the magnetic force, use the Right-Hand-Rule: with your right hand, hold your fingers straight and in the direction of the B-field, your thumb in the direction of the velocity. The direction your palm faces is the direction of the force. Magnetic fields produce a force on a current-carrying wire: ---Magnetic force on a current-carrying wire (magnitude only) “B” is the magnetic field, “I” is the current, “L” is the length of the wire, and “ ” is the angle between the magnetic field and the current. The direction of this force is again found by using the Right-Hand-Rule, except now you put your thumb in the direction of the current. A loop of current in a uniform magnetic field experiences a torque: ---Torque on loop(s) of wire “N” is the number of loops (or coils), “A” is the area of the loop, and “ ” is the angle between the B-field and the normal to the loop. This confuses most people. If a charged particle moves under only the influence of a magnetic field, it travels in circular paths (or helical paths—see the figure on page 599). The radius of this circle is: ---Radius of a charged particle’s path in a magnetic field Wires produce magnetic fields themselves: ---Magnetic field produced by a long, straight wire , “I” is the current in the wire, “r” is the distance from/to the wire. Ampere’s Law: basically the equivalent of Gauss’s Law for currents and B-fields. ---Ampere’s Law, simply says add up the pieces around a closed loop. “I” is the total current enclosed by the loop. ---Force between two parallel, current-carrying wires (magnitude only) ---Magnetic field inside a solenoid; it’s uniform everywhere inside. Look at page 605 to see what a solenoid is. “n” is the number of turns per unit length (basically n=N/L).