MAGNETIC FIELDS

motor loudspeaker

These are the fields we are most familiar with. Most of us have wandered around the house with a compass "getting lost". Because of our experience with compasses, we define the direction of a B field as the direction a compass N pole points. ( As "like" poles repel, ironically, the North Pole of Earth has "South" polarity.)

"B", the strength of a magnetic field has many names depending on which text you use and how much credibility you give history! In Tasmania, we call it "Magnetic Field Strength" to keep it in line with Electrostatics and Gravity BUT it is called at University "Magnetic Induction" just to confuse you with a different topic and other texts call it "Flux Density". ( Historically, Magnetic Field Strength is associated with a derived value, "H" which takes into account the properties of materials.) The different sources do agree that B is the correct abbreviation - stupidly.

Unit of B is the "tesla",T, in SI units - old units include the "gauss" and the "oersted". This is named after Nikola Tesla, a founder of the AC generation system used today across the world.

In the diagram above, the direction a compass needle points near a "conventional" current ( flowing from + to - ) terminals is closed WITH NO START OR FINISH. This is clearly different from electrostatics and gravity where field lines start and finish at objects. Magnetism seems to have no individual "North poles"and "South Poles", a problem for many subnuclear physicists.This is true even in metal bar magnets as well as current magnets.

Predicting the direction of the field line now is tricky - no problems outside a "bar magnet" with its ( nonexistant ) poles where the lines look and behave like electrostatics but a real problem inside the metal and for a current carrying wire. We have to resort to memory aids

- USING THE RIGHT HAND.

Here the thumb sticking up represents the current, and the curl of the fingers represents the field line and direction.

EVALUATING "B"

To give the field a value, we once again note that forces exist between the wires so the field strength can be given in terms of force on a small test magnet.

For convenience, we select a small straight piece of wire of known length and current. I shall call it Itest because it must be small ( so small you can scarcely see it - get it? ). Arrange the wire so you get the LARGEST force on it. This is different from gravity and electrostatics where the orientation of the test object is irrelevant.

Similarly to the two other fields, DEFINE B as a force divided by by the test magnet values of current and length.

B = Fmax / Itest l the units of tesla are NA-1m-1

The direction of B is NOT the direction of the force however - this is radically different from electrostatics and gravity - this is where we start being non newtonian!


The largest force occurs when the current is at rt angles to B - and we find that B and F are also perpendicular !!!!

OH WOW!!!! Newton would not be a happy budgie if he knew.

When we compensate for angles, we must insert sinθ. So rearranging the definition

F = IlBsinθ for the SIZE of F on a current - and some kind of memory system for the direction!!

DIFFERENT TEACHERS, DIFFERENT SCHOOLS use different memory tricks at this point. One book will refer to "The right hand Palm Rule", another to "Fleming's Left Hand Rule" - and others. I personally use a variation on "vector products" - the "Right Hand Screw Rule". It sounds suitably rude.

The trick is to look at the equation as

  • Thumb sticking out is the Force
  • Il is the first sense of vector so start fingers in the Il direction.
  • Twist, rotate, contort your wrist / arm so that your fingers can close into the B direction ( remembering that is the direction of a compass needle )
  • - and your thumb gives F.

(DO remember to use your right hand and conventional current - if you insist on electron flow, you may use your left hand. )

It doesn't matter a damn which variant you use as long as it works for you.

( This is an example of a "vector product" or "cross product" which is a generalised type of vector rule. Click here for more.)

The Electric Motor can be explained by this force law.

Motors - electrical energy IN, mechanical energy OUT

Each side of the rectangle has the force F= IlB acting upon it, one side UP, the other side DOWN. The system will rotate until the wires are at top and bottom. This is stable and rotation will cease. So to continue rotation, we provide a simple automatic switch reversing the current. This automatic switch is the COMMUTATOR, bits of copper plate stuck to each side of the axle and turning with it. Brushes rubbing the plates bring the current into the rectangle.

The motor can also be thought of as rectangle with current making it a magnet which is rotates in an attempt to align its field with the external field. Each time it approaches this, the current is reversed causing further rotation.

The Loudspeaker

The standard loudspeaker is also a magnetic motor but it is not a rotating device. The moving component is a cylinder ( with the loudspeaker cone attached ) inserted in a very powerful radial magnetic field. This field is created by a central pole surrounded by the opposite pole. The cylinder fits in the slot between the poles. Wires are wrapped around the cylinder, so an alternating current from an amplifier into the wires is then subjected to powerful magnetic forces ( F = IlB and the RHS rule for direction). These forces are along the axis of the cylinder making it move back and forth in proportion to the current.

The cone then pumps the air creating sound.

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