Video Lectures created by Tim Feiegenbaum at North Seattle Community College.
Okay, we're in Section 2.4. We're going to be introducing Magnetism and Electromagnetism in this particular section. Magnetic and electromagnetic fields play important roles and are fundamental to electronic and electromechanical systems. Motors, generators, speakers, microphones, computer storage devices like hard drives and many other devices are based upon magnetic, electromagnetic principles.
Okay, magnetic fields. Here we have a picture of one. Surrounding all magnetic objects is an invisible but measurable field. Now notice that's surrounding all magnetic objects. It is invisible. It is measurable.
A magnetic field is a region around a magnet where another magnet would experience interaction and it would be either attraction or repulsion. The fields are not objects but invisible lines of force. Here we see a bar magnet and we see the magnetic flux lines that appear around this magnet.
The lines around a magnet are called lines of flux or magnetic flux lines. Each flux line is elastic but continuous. Flux lines never touch or intersect each other. The unit of magnetic flux is the weber. One weber is equal to 100,000 flux lines. The symbol for magnetic flux is ?. That's this letter right here. A Greek letter Phi.
Here we see a bar magnet and it is not energized but you see all these metal filling. If I press the little 'ON' button here you'll see that the magnetic field will cause those fillings to align in a certain way. That's a cool little interactive video there. So magnetic poles.
Flux density is the measure of how many flux lines appear in a certain area. The unit of measure for flux density is the Tesla (T). One Tesla corresponds to a flux density of one weber per square meter. Remember one weber is equal to 1,000 flux lines, so a Tesla has to do with 100 flux lines per square meters if it's one Tesla. If it's more than one then we're going to have more webers per square meter. The more Teslas the stronger the magnetic field.
Materials that can be magnetized have regions called magnetic domains. Each magnetic domain acts like a miniature bar magnet. The length of a domain is only a fraction of a millimeter. They are very, very small. It takes energy to rotate or change the orientation of magnetic domains. This energy loss is often evidenced as heat in electromagnetic devices. Figure 2-16 has a text, a picture of this. It displays the magnetic domains. It shows them as they occur randomly. It shows them also when a current is introduced through it and all of the magnetic domains then they line up and orient themselves be it north or south.
Okay, magnetomotive force, MMF, refers to the energy source that actually creates the flux. It is the magnetic equivalent of, remember we talked about this, emf. Remember that was voltage and this is mmf so it is the magnetic equivalent to voltage. The symbol for magnemotive force is, and it's right here. The unit of measure is ampere-turns, okay and that is Amps* time.
Then we have magnetizing force, magnetizing force, upper case H, also called magnetic field intensity is closely related to the magnetomotive force but includes a physical dimension. The unit of measure for magnetizing force is ampere-turns, notice per meter. In this case the magnetizing force H=Amps*time/meters. Now since H is the result of Amps times the fractional value of t/m so you have A*t/m, the fractional value of t/m, the larger the m, the smaller the H. Okay the H will be over here, H=A*t/m. The larger the m in the meters, the smaller the H and vice versa. H addresses the concentration of a magnetic field so if the concentration is smaller notice if this field is in a smaller area then the H is going to increase. That is the magnetizing force.
Then we have the term Reluctance. It is the magnetic equivalent of resistance. Reluctance opposes the passage of magnetic flux. A material with a higher reluctance will have less flux for a given magnetic force. The symbol for reluctance is here we have this R and the unit of measure is A*time per weber.
Okay more magnetism terms and units, Ohm's law for magnetic circuits. This is kind of an interesting way to look at it. Remember the magnetic force is equivalent to emf or volts so this would be equivalent to E. Reluctance is equivalent to resistance so that would be R and magnetic flux is equivalent to current. So magnetism is very closely related to electricity and you see here very graphically the relationship between current, voltage and resistance as related to magnetic force, reluctance and magnetic flux.
Permeability is the ability of a material to pass magnetic flux. Its symbol is the Greek letter (�). It is easier to pass a magnetic field through a material with a higher permeability. The higher the permeability the easier it is to pass a magnetic field. Permeability in a magnetic field is similar to guess what? Conductivity in an electrical circuit.
Many electrical devices use temporary magnets for their operation. These magnets exhibit magnetic characteristics as long as they are under the influence of a magnetizing field. Temporary magnets generally rely on the flow of electrons through a conductor to create the magnetizing field. The direction of magnetic fields is determined by the direction of current flow in a conductor. This is an important point.
The direction of magnetic fields is determined by the direction of current flow in a conductor. If we look at this particular demo over here. Here we have a DC supply, this is supplying DC voltage and here we have a conductor. What we're looking at here is the direction of the magnetic field that is built as current flows through this particular conductor.
Here we have this DC here, notice the polarity. This is the negative side, this is the positive side. As current electron flow, current flow through this device notice the magnetic lines of flux are forming in this particular direction. Now, if in this case everything is the same except that the polarity has been changed here and so now the negative side rather than coming in through the bottom, negative is going in through here and the current is flowing the other direction. Now, the current is flowing through the wire in this direction and you will notice that the magnetic field now has changed direction. The lines of flux are now moving in this direction.
The Left Hand rule is one way of remembering the information on the previous slide. The left hand on the wire below illustrates the Left Hand rule for magnets. The thumb is pointing in the direction of electron flow, remember negative to positive. The fingers wrapped around the wire indicate the direction of the magnetic field. What we say, and this has got to be your left hand. If you do it with your right hand it would be wrong. With you left hand you'll see this is indicating current going this way and electron flow. If we had a battery here and this is the positive terminal this is the negative terminal and we connected a wire like this, we would have here is the direction of the current flow and the direction of the magnetic field is going to be like this in this particular direction. That's referred to as the Left Hand rule.
Earlier in this presentation I showed you one of the slides concerning magnetic orientation. If you want to go to that site the URL is right here. I'm going to post this link on the class website but if you just want to jot it down there it is. http://micro.magnet.fsu.edu/electromag/java/index.html
In this particular lesson we looked at we ended up looking at the left hand rule, we looked at magnetic versus electromagnetic fields, we talked about permeability and remember permeability was kind of similar to conductivity. Remember we talked about Siemens which were the reciprocal of resistance and permeability is very similar in concept to conductivity. We looked at the equivalent of Ohm's law in terms of magnetism. We talked about reluctance and it is electrically the equivalent of resistance. We looked at magnetizing force which is a symbol H and the important thing about magnetizing force is it brought in the factor of area, in this case meters, and so the smaller the area of the magnetizing force the greater that force.
Then we looked at magnetomotive force and this was just Amps*time and it's equivalent to emf. We looked at magnetic domains I didn't have a picture online but we do have a picture in your text. It's Figure 2-16. Flux density is measured in a unit called the Tesla. We looked at magnetic poles, magnetic flux and we refered to magnetic flux in terms of the weber. We looked at the magnetic fields. That concludes 2.4.
Video Lectures created by Tim Fiegenbaum at North Seattle Community College.
In Partnership with Future Electronics
by Jeff Child
The video was really helpful but the formula for flux density is product of Current and Number of turns.
So, to start with, (1) weber is actually equal to 100,000,000 (one hundred million) flux lines, but in the video he keeps saying “one hundred thousand” even though the slide says 100,000,000, and in the text above on this page, under the heading “Magnetic Flux”, it says (1) weber is equal to “100,000”, and then right below that, under the heading “Flux Density”, it says that (1) weber is equal to “1,000” flux lines. Someone needs to do some serious proofreading. Not to mention that he kept pronouncing Tesla as Telsa…
And in the equation H=A*t/m, doesn’t the “t” stand for turns and not time?
This just made magnetism 1,000 or 100,000 or 100,000,000 times more confusing…