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| Humankind has known about magnetism since before 600 BC. Ancient Greeks discovered lodestone, an ore of iron that is magnetic. When these stones were suspended on a string, they always assumed a North - South orientation. As early as 121 AD, the Chinese knew that a piece of iron could be magnetized by bringing it in close proximity to lodestone. Since lodestone was discovered near the ancient city of Magnesia in Asia Minor, the term given to this phenomena was magnetism. |
| Magnets and Magnetic Fields Any magnet, straight, horeshoe or disc shaped always have two poles, referred to as North and South . |
| The magnetic poles are distinct and cannot be separated into monopoles. Breaking a magnet into two will always result in two, smaller dipoles. |

| We observe both repulsive and attractive forces with magnets. Just as with electric charges, opposite poles attract and like poles repel. |
|
Magnetic field
can be visualized in a manner similar to electric fields. We determine the direction
of the field lines by imagining the direction of force acting on a hypothetical North monopole. We can
see that the field lines would appear to be coming out of the North pole of
the magnet and would be going into the South pole. We used iron filings and a
compass in the lab to help us visualize the field lines and direction.
Remember, the field lines aren't really there. They simply serve as a mental
model to help us understand the action at a distance exhibited by magnets. |
| Two Opposite Poles |
| Two Like Poles |
|
The Magnetic Field Of The Earth |
| Magnetic Declination When you use a compass to orient yourself, remember that the compass points to the magnetic South Pole, not the geographic North. This means that at any point on the earth, there will be an angle formed from two lines drawn from that location, one to geographic North and the other to magnetic South. The angle between these two lines is referred to as the magnetic declination. In New England, the magnetic declination ranges from 15 to 20 degrees west. This means that a compass points west of true North by that angle of declination. |
Magnetic InclinationMagnetic Inclination can be used to get an idea of your latitude. It is measured with a dipping needle. The needle indicates the direction of a cord drawn from the location to magnetic south. The angle measured is the angle between the cord and the horizontal line drawn towards the magnetic South. |
| Earth's magnetic field is continually changing. The poles precess like a spinning top and move a couple of km per year. In the geological record, there is evidence that the earth's magnetic field has reversed itself on numerous occasions. |
|
Electricity and Magnetism Magnetic
Field Around a Wire Conducting Current Up until the
eighteenth century, many people recognized the similarity between electricity
and magnetism, but it wasn't until 1820 that Hans Christian Oersted came upon
evidence making a direct connection between electricity and magnetism. When a
compass was left near a wire, its needle deflected when the wire had current
flowing through it. |
|
The
direction of these field lines can be determined by the 1st right hand rule |
| Magnetic Field Around a Coil of Wire
(Solenoid) If a conductor is wound into a coil, not only will a magnetic field be produced by current, but a definite north and south pole will be produced. We can see why this is by examining one loop of wire and applying the 1st right hand rule. If we grasp the wire and slide our hand around the coil, the direction of the field lines inside of the coil all point in one direction. |
| If we put several coils together we can see a definite North and South Pole. We can determine the location of the North Pole on a solenoid conducting current by applying the 2nd right hand rule. If we grasp the solenoid so our fingers point in the direction of the conventional current, our thumb will point to the North Pole. |
| As we observed with our experiment, the strength of the magnetic field depends upon the current, the radius, the number of coils and the presence or absence of a ferromagnetic core material. |
|
The Nature of Magnetism |
| Presence of Unpaired Electrons | Behavior in Magnetic Field | Examples | |
| Ferromagnetic | several unpaired electrons | strongly attracted to a magnet | Fe, Co, Ni, Gd |
| Paramagnetic | a few unpaired electrons | weakly attracted to a magnet | O2, Mn |
| Diamagnetic | no unpaired electrons | weakly repelled by a magnet | N2 |
| Ferromagnetic
substances like iron can either be magnetized or not. What determines whether
or not a piece of iron is magnetized? In a ferromagnetic substance, there are
groups of atoms whose magnetic poles all line up in the same direction. These
groups are referred to as domains. An unmagnetized piece of iron has domains that are randomly oriented. If you add up the magnetic field of each domain, they "cancel out" because of their random orientation. |
| A magnetized piece of iron has many domains pointing in the same direction. The magnetic field strength of the magnet will increase as the number of domains pointing in the same direction increase. |
This can help us explain a lot about what we observe with magnets. For example: 1) We can make an unmagnetized paper clip magnetized, simply by placing it next to a magnet. The magnetic field of the magnet causes the domains in the paper clip to line up temporarily, allowing it to be magnetized. When the magnet is removed, the domains randomize, and the paper clip loses its magnetism. 2) We can stroke a nonmagnetized steel nail with a magnet and make the nail magnetized. The magnetic field the magnet causes the domains in the nail to line up so that the nail becomes magnetized. 3) An older Canadian Nickel is attracted to a magnet. When it is heated to a very hot temperature, it loses its attraction to the magnet. The thermal energy causes the domains to vibrate and assume a random orientation. 4) A ferromagnetic material used as a core in a solenoid enhances the magnetic field of the solenoid because the domains of the material align with the solenoid's magnetic field. The ability to enhance a solenoids magnetic field is referred to as the magnetic permeability, m. We define the magnetic permeability as the ratio of the magnetic field of the solenoid with the core to the magnetic field of the solenoid with no core. m = Bwith/ Bwithout |
| Interaction
of Magnetic Fields Produced By Conductors In class we observed that magnetic fields produced by conductors interact. When 2 conductors conduct current in the same direction, we observe an attraction. Drawing the magnetic field lines around each conductor illustrates that the field lines from each conductor travel in opposite directions where we observe the most interaction. |
When 2 conductors conduct current in the opposite direction, we observe a repulsion. Drawing the magnetic field lines around each conductor illustrates that the field lines from each conductor travel in the same direction where we observe the most interaction. |
Direction of the Force on a Moving Charge Due to an External Magnetic FieldPicture a wire placed between two magnets. If the wire conducts current, an induced magnetic field resembling concentric circles surrounds the conductor. We can determine the direction of the induced magnetic field by the first right hand rule. We can see that above the conductor the field lines go in the same direction and repel whereas below the conductor, the field lines go in opposite directions and attract. The net force will be downward. |
We can develop a third right hand rule that helps us determine the direction of the force. 1) Our fingers point in the direction of the external magnetic field. 2) Our thumb points in the direction of the current (positive charge) 3) Our palm points in the direction of the force. The
force acting on a conductor conducting current in a magnetic field can be
calculated using the equation F = BI L B = the external magnetic field I = current flowing through the wire L = length of the conductor The
above equation can be generalized for any charge moving through a magnetic
field. The force acting on a charge moving through a magnetic field is F = q v B v = velocity of charge in m/s |
|
The
Motor We can see how this force can turn the coil in a motor from the following diagram. |
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