Chapter 22 Magnetism.

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Presentation transcript:

Chapter 22 Magnetism

MAGNETISM Arguable the oldest subject in Physics: ancient Greeks (near the City of Magnesia) and Chinese realized certain strange stones attracted iron. Around 1600, William Gilbert proposed that the Earth itself is A gigantic magnet. For a long time, people knew only one source of magnetism from Iron. In 1821, a Danish physicist, Oersted noticed that an electrical wire carrying current made the near-by compass reorient.  First clue of inter-relation between electricity and Magnetism. Ampere, Faraday established the nature of electricity and magnetism (all from their experimental observations).

Magnets Poles of a magnet are the ends where objects are most strongly attracted Two poles, called north and south Like poles repel each other and unlike poles attract each other Similar to electric charges Magnetic poles cannot be isolated If a permanent magnetic is cut in half repeatedly, you will still have a north and a south pole This differs from electric charges There is some theoretical basis for monopoles, but none have been detected

More About Magnetism An unmagnetized piece of iron can be magnetized by stroking it with a magnet Somewhat like stroking an object to charge an object Magnetism can be induced If a piece of iron, for example, is placed near a strong permanent magnet, it will become magnetized

S N S N S N S N

Magnetic field cannot be defined as E-field, Magnets exist in pairs of N-S poles. A theoretical prediction says that it is possible to have magnetic mono-poles but they have not been observed!! Magnetic field cannot be defined as E-field, FE = qE FB = qBB

Magnetic Fields A vector quantity Symbolized by B Direction is given by the direction a north pole of a compass needle points in that location Magnetic field lines can be used to show how the field lines, as traced out by a compass, would look

Magnetic Field Lines, sketch A compass can be used to show the direction of the magnetic field lines (a) A sketch of the magnetic field lines (b)

Magnetic Field Lines, Bar Magnet Iron filings are used to show the pattern of the magnetic field lines The direction of the field is the direction a north pole would point

Magnetic Field Lines, Unlike Poles Iron filings are used to show the pattern of the magnetic field lines The direction of the field is the direction a north pole would point Compare to the electric field produced by an electric dipole

Magnetic Field Lines, Like Poles Iron filings are used to show the pattern of the magnetic field lines The direction of the field is the direction a north pole would point Compare to the electric field produced by like charges

Magnetic and Electric Fields An electric field surrounds any stationary electric charge A magnetic field surrounds any moving electric charge A magnetic field surrounds any magnetic material

Earth’s Magnetic Field The Earth’s geographic north pole corresponds to a magnetic south pole The Earth’s geographic south pole corresponds to a magnetic north pole Strictly speaking, a north pole should be a “north-seeking” pole and a south pole a “south-seeking” pole

Earth’s Magnetic Field The Earth’s magnetic field resembles that achieved by burying a huge bar magnet deep in the Earth’s interior

S N In unifrom field, no force only torque!!!

Magnetic field can make a closed loop (not with E-field). I X Right-handed cork-screw rule

Magnetic Fields In a magnetic field, a current carrying wire experiences a magnetic force This force has a maximum value when the wire is perpendicularly to the magnetic field lines This force is zero when the wire is along the field lines

Magnetic Fields, cont One can define a magnetic field in terms of the magnetic force exerted on current carrying wire Similar to the way electric fields are defined

Units of Magnetic Field The SI unit of magnetic field is the Tesla (T) Wb is a Weber The cgs unit is a Gauss (G) 1 T = 104 G

B F FB = ILB I Magnetic induction Magnetic flux density Magnetic field (strength) [B] = [F/IL] = Ns/Cm = Tesla *1 Tesla = 104 gauss FB = ILB Length of the section in B-field