FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM
description
Transcript of FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM
![Page 1: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/1.jpg)
FOWLER CHAPTER 7LECTURE 7 MAGNETS AND
ELECTROMAGNETISM
![Page 2: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/2.jpg)
CHAP 7 P-173 MAGNETISM
MAGNETISM IS A FORCE THAT ACTS ON CERTAIN MATERIALS.
WHAT MATERIALS? ALLOYS OF COPPER,NICKEL, ALUMINIUM, IRON, COBALT.
THIS MAGNETIC FORCE IS REFERRED TO AS A MAGNETIC FIELD. THE FIELD EXTENDS OUT FROM THE MAGNETIC MATERIAL IN ALL DIRECTIONS.
![Page 3: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/3.jpg)
LINES OF FORCE OF A MAGNETIC FIELD ARE KNOW AS MAGNETIC FLUX (Φ)
FLUX IS STRONGER WHERE LINES OF FORCE ARE CLOSER.
FLUX IS WEAKER WHERE LINES OF FORCE ARE FATHER APART.
FLUX IS ALWAYS STRONGEST AT THE END OF A MAGNET.
LINES OF FORCE LEAVE THE N POLE AND ENTER THE S POLE.
![Page 4: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/4.jpg)
AS WITH ELECTRIC CHARGES, LIKE MAGNETIC POLES REPEL EACH OTHER, UNLIKE MAGNETIC POLES ATTRACT EACH OTHER
P.175
![Page 5: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/5.jpg)
MAGNETIC FORCE DECREASES AT A INVERSE SQ. RATE 1/R²
![Page 6: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/6.jpg)
![Page 7: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/7.jpg)
EACH TIME A MAGNET IS BROKEN A NEW PAIR OF POLES IS CREATED.
MAGNETIC FLUX LINES ARE IN CONTINOUS LOOPS.
P.175
![Page 8: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/8.jpg)
FLUX CAN BE ENTIRELY CONTAINED WITHIN A MAGNET AND THUS HAVE NO POLES. F.7.6 ,P-176
ELIMINATING THE GAP,ELIMINATES THE POLES
![Page 9: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/9.jpg)
ELECTROMAGNETISM
A ELECTRIC CURRENT CREATES A MAGNETIC FIELD WHICH IS PERPENDICULAR TO THE CURRENT FLOW
P.177
Magnetic field around a straight wire http://www.youtube.com/watch?v=Z927bDX1l04&feature=fvwp&NR=1
![Page 10: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/10.jpg)
.Motion of particles in magnetic and electric fields . http://www.youtube.com/watch?v=Gkfwc4Uzgss
http://www.youtube.com/watch?v=4CtnUETLIFsElectromagnetic wave HD
![Page 11: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/11.jpg)
P.177
+
![Page 12: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/12.jpg)
P.177
![Page 13: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/13.jpg)
Direction of flux is found by the RIGHT hand rule.
![Page 14: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/14.jpg)
Field strength is directly proportional to the amount of current flowingthru the conductor. If the current doubles, the field strength doubles.
![Page 15: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/15.jpg)
FORCE BETWEEN CONDUCTORS P.177
TWO PARALLEL CURENT CARRYING CONDUCTORS ATTRACH EACH OTHER, IF THE CURRENTS ARE FLOWING IN THE SAME DIRECTION.( F7-10 P.178) THE FIELD LINES JOIN TOGETHER. THE OPPOSITE OCCURS IF CURRENTS ARE TRAVELING IN THE OPPOSITE DIRECTIONS.
REPEL EACH OTHER
ATTRACH EACH OTHER
![Page 16: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/16.jpg)
COILS
IF A CURRENT CARRYING WIRE IS TIGHTLY WOUND INTO A COIL, A ELECTROMAGNET IS CREATED. P.178,F.7-10
![Page 17: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/17.jpg)
MAGNETIC MATERIALS
ARE ATTRACTED TO MAGNETIC FIELDS.EXAMPLES OF FERROMAGNETIC MATERIALS;IRONIRON COMPOUNDSALLOYS OF IRON OR STEEL
NONMAGNETIC MATERIALS:( NO ATTRACTION) METALS SUCH AS COPPER, BRASS, AL,SILVER ZINC, TIN.FLUX TRAVELS THRU NONMAGNETIC MATERIALS.
P.179
![Page 18: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/18.jpg)
THEORY OF MAGNETISM P180ELECTRONS HAVE A MAGNETIC SPIN, WHEN RANDOMLY ARRANGED THE NET SPIN IS ZERO(NO MAGNETIC FIELD).
DOMAINS ARE GROUPS OF MOLECULES THAT HAVE MAGNETIC POLES.THESE ARE USUALLY RANDON IN UNMAGNETIZED MATERIALS. F.7-13 P.180
IF AN EXTERNAL MAGNETIC FIELD IS APPLIED, THE DOMAINS WILL LINE UP, FORMING EITHER A TEMPORARY OR A PERMANENT MAGNET.
![Page 19: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/19.jpg)
PERMANENT MAGNETSDOMAINS REMAIN ALIGNED. EXAMPLES:Fe WITH 0.8% CARBONALLOYS LIKE ALNICO (COMPOUND OF Fe COBALT ,NICKEL, Al, AND Cu)ALSO CERTAIN CERAMIC MATERIALS
P.180
![Page 20: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/20.jpg)
HOW TO MAKE A PERMANENT MAGNETS
![Page 21: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/21.jpg)
TEMPORARY MAGNETSLOOSE MAGNETISM AFTER MAGNETIC FIELS IS REMOVED, DOMAINS BECOME RANDOMEXAMPLES: PURE Fe FERRITE: MAGNETIC MATERIAL THAT IS NOT A CONDUCTOR. SILICON STEEL
P.180
![Page 22: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/22.jpg)
MAGNETOMOTIVE FORCE( MMF) P.181
IS WHAT CREATES MAGNETIC FIELDS AND FLUX. MMF INCREASES AS THE # OF TURNS OR THE CURRENT IN THE COIL INCREASES.
SATURATION: P.182 OCCURS WHEN AN INCREASE IN MMF NO LONGER WILL INCREASE THE MAGNETIC FLUX.
![Page 23: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/23.jpg)
DEMAGNETIZING P.182
CAN BE DONE TO A PERMANENT MAGNET BY HAMMERING IT OR HEATING IT TO A HIGH TEMPERATURE.EASIEST WAY IS TO DO THIS IS WITH A COIL AND A AC SOURCE. F.7-17B
http://www.youtube.com/watch?v=OODRqLwV5uIHow to demagnetize a screwdriver
![Page 24: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/24.jpg)
ONE WAY: MAGNET IS SLOWLY MOVED AWAY FROM THE COIL, AND WITH EACH REVERSAL IN POLARITY IT BECOMES WEAKER. THE SOLDERING IRON PICTURED BELOW CAN PERFORM THIS FUNCTION.
ANOTHER WAY: SLOWLY REDUCE THR MAGNITUDE OF THE AC UNTIL IT BECOMES ZERO.
DEMAGNETIZING A MAGNET
![Page 25: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/25.jpg)
RESIDUAL MAGNETISM P.183IS THE FLUX THAT REMAINS IN A TEMPORARY MAGNET.
IDEAL PERMANENT MAGNET WOULD RETAIN ALL ITS FLUX.IDEAL TEMPORARY MAGNET WOULD RETAIN NO FLUX.
RELUCTANCE P.183OPPOSITION TO MAGNETIC FLUX. DEPENDS ON SIZE AND THE MATERIAL OF THE OBJECT.AIR, NONMAGNETIC MATERIALS HAVE HIGH RELUCTANCEMAGNETIC FLUX LINES TAKES THE LOWEST AND SHORTEST RELUCTANCE PATH.
HIGH RELUCTANCE PATH
LOW RELUCTANCE PATH
![Page 26: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/26.jpg)
HIGH RELUCTANCE PATHLOW RELUCTANCE PATH
![Page 27: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/27.jpg)
MAGNETIC SHIELDS P.184
MAKE USE OF THE TENDENCY OF FLUX TO DISTORT AND FOLLOW THE PATH OF LOWEST RELUCTANCE.
![Page 28: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/28.jpg)
![Page 29: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/29.jpg)
INDUCED VOLTAGE P.185
WE KNOW THAT CURRENT CARRYING CONDUCTORS PRODUCT A MAGNETIC FIELD.CONSIDER THE OPPOSITE.A MAGNETIC FIELD CAN INDUCT A VOLTAGE/CURRENT IN A WIRE.THIS IS THE BASES OF ALL ELECTRIC MOTORS.
![Page 30: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/30.jpg)
![Page 31: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/31.jpg)
Energy for the operation of most electrical equipment depends upon the electrical energy supplied by a generator. A generator is any machine which converts mechanical energy into electrical energy by electromagnetic induction. A generator designed to produce alternating current energy is called an ac generator, or alternator; a generator which produces direct current energy is called a dc generator. Both types operate by inducing an ac voltage in coils by varying the amount and direction of the magnetic flux cutting through the coils.
![Page 32: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/32.jpg)
SIMPLE DC GENERATOR P.185
PATRS NEEDED: MAGNET COIL OF WIRE COMMUTATOR BRUSH } MAKES CONTACT TO THE
ROTATING LOOPOF WIRE
![Page 33: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/33.jpg)
AS THE WIRE TURNS, THE COMMUTATOR TURNS WITH IT. WHEN WIRE TURNS IN CW DIRECTION A CURRENT IS INDUCED IN THE WIRE WHICH FLOWS FROM THE COMMUTATOR TO THE BRUSH. THIS CHANGES POLARITY EVERY 90º, SINCE BRUSH CHANGES FROM ONE COMMUTATOR TO THE OTHER. POLARITY STAYS THE SAME AND RESULTS IN A DC OUTPUT. (SEE NEXT SLIDE)
![Page 34: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/34.jpg)
YOU TUBE : Direct Current Electric Motor http://www.youtube.com/watch?v=Xi7o8cMPI0E
![Page 35: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/35.jpg)
SIMPLE TRANSFORMER P.186WHEN A CURENT CARRYING WIRE IS WRAPED AROUND A Fe CORE ( PRIMARY WINDING)IT WILL INDUCE A MAGNETIC FLUX IN THE Fe CORE.IF A SEPARATE SECOND COIL IS WRAPED AROUND THE CORE (SECONDARY WINDING) ACURRENT WILL BE INDUCED IN THIS WIRE.THESE CHANGES ARE PROPORTIONAL TO THE AMOUNT OF FLUX CHANGE AND THE RATEOF FLUX CHANGE.
![Page 36: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/36.jpg)
THE INDUCED VOLTAGE FROM A TRANSFORMER DEPENDS ON THE NUMBER OF WINDINGS IN BOTH THE 1º AND 2º COILS.
1º : PRIMARY2º : SECONDARY
YOU TUBE : Transformer Animation http://www.youtube.com/watch?v=VucsoEhB0NA
![Page 37: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/37.jpg)
Magnetic Quantities p. 186
Remember MMF is the force that carries flux.
Ampere-Turn: The MMF carried by 1 Amp flowing thru 1 turn of a coil.
MMF= #of turns( around coil) x current
1 ampere-turn
6 ampere-turn
1 ampere 1 ampere
![Page 38: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/38.jpg)
How many ampere-turns are there for this two coils?
![Page 39: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/39.jpg)
WEBER: BASE UNIT OF MAGNETIC FLUX(Φ)
MAGNETIC FIELD STRENGTH (H):DEFINED AS AMPERE-TURN/ METEROR MMF/CIRCUIT LENGTH.
![Page 40: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/40.jpg)
FLUX DENSITY(B) FLUX /UNIT CROSS SECTIONAL AREA
YOU TUBE:Magnetic Field and Flux Animation http://www.youtube.com/watch?v=pB7oZNBIqqc
![Page 41: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/41.jpg)
TESLA (T) : FLUX/UNITAREA = 1 WEBER/M²
![Page 42: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/42.jpg)
PERMEABILITY (u): ABILITY OF A MATERIAL TO CONDUCT FLUX.
u =B/H=FLUX DENSITY/MAGNETIC FIELD STRENGTH
The higher the magnetic permeability, the stronger the magnetic field.
![Page 43: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/43.jpg)
LOW PERMEABILITY (u):
MEDIUM PERMEABILITY (u):
HIGH PERMEABILITY (u):
![Page 44: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/44.jpg)
DC MOTORS P.191IS A DC GENERATOR WORKING IN REVERSE.CURRENT FROM THE POWER SOURCE FLOWS THRU THE BRUSHES, COMMUTATORS INTO THE ARMATURE COIL. WHICH PRODUCES A MAGNETIC FIELD IN THE ARMATURE. THE ARMATURE POLES ARE ATTRACHED TO THE FIELD POLES WHICH CAUSES ROTATION OF THE ARMATURE.SINCE THE COMMUTATOR/BRUSHES CHANGE DIRECTION OF CURRENT EVERY 90º, THE ARMATURE SPINS UNITL THE CURRENT IS TURNED OFF.
FIELD POLEFIELD POLE
![Page 45: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/45.jpg)
![Page 46: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/46.jpg)
http://www.k-grayengineeringeducation.com/blog/index.php/2009/02/2/engineering-education-today-in-
history-blog-thomas-davenport-patents-the-electric-motor-and-electric-railway-2/
![Page 47: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/47.jpg)
![Page 48: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/48.jpg)
![Page 49: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/49.jpg)
![Page 50: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/50.jpg)
![Page 51: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/51.jpg)
SOLENOIDS P.192
AN ELECTROMAGNETIC DEVICE THAT ALLOWS A ELECTRIC CIRCUIT TO CONTROL A MECHANCIAL DEVICE.( VIA A PLUNGER)INCREASING THE MMF OR DECREASING THE RELUCTANCE WILL INCEASES THE PULL.
![Page 52: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/52.jpg)
ONE CURRENT CARRYING WIRE LOOP AND ITS ASSOCIATED MAGNETIC FIELD.
![Page 53: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/53.jpg)
MULTILOOPED WIRE AND ITS MAGNETIC FIELD.
![Page 54: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/54.jpg)
![Page 55: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/55.jpg)
![Page 56: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/56.jpg)
1. Valve Body 4. Coil / Solenoid 7. Plunger
2. Inlet Port 5. Coil Windings 8. Spring
3. Outlet Port 6. Lead Wires 9. Orifice
INTERNAL CONSTRUCTION OF A SOLENOID
![Page 57: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/57.jpg)
EXAMPLE OF AN INDUSTRIAL SOLENOID
![Page 58: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/58.jpg)
VARIOUS TYPES OF SOLENOIDS
![Page 59: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/59.jpg)
HOW DOOR CHIMES WORK
![Page 60: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/60.jpg)
A relay is an electrical switch that can be opened or closed by an electrical signal. It is an electrically controlled switch. People use them when they want a small amount of electricity to control a bigger amount of electricity. The same thing can be done with transistors, but transistors can't handle the amount of current that relays can.
RELAYS P.192
![Page 61: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/61.jpg)
RELAYS P.192
USE THE ATTRACTION BETWEEN A ENERGIZED COIL AND A Fe ARMATURETO OPEN/CLOSE ELECTRICAL CONTACTS. THIS CAN ALLOW THE REMOTE CONTROLOF MOTORS, LIGHTS, ETC.RELAYS CAN OPERATE ON AC OR DC, RELAYS ARE NOT INTERCHANGEABLE.
![Page 62: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/62.jpg)
Relays are used as switches. These are different from manual switches where we push a button to turn them on and off. Relays are electromagnetic device, and very useful in scenarios where we want to control a high voltage device through a low-voltage circuit.For example, assume that you have designed a small water pump controller which works on 12V DC. When water level on the overhead tank goes low, the controller outputs 5v on the output pin indicating that the pump should be turned on now. Similarly, when the tank is about to overflow, the circuit outputs 0v on output pin indicating the pump to turn off. Now in this case how will you control a 110V AC pump motor? The answer is very simple. Use relay as show in the diagram below.
![Page 63: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/63.jpg)
![Page 64: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/64.jpg)
VARIOUS RELAY SYMBOLS
![Page 65: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/65.jpg)
CIRCUIT TO CONTROL TRAFFIC LIGHTS USING RELAYS
![Page 66: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/66.jpg)
![Page 67: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/67.jpg)
![Page 68: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/68.jpg)
(a) .Contacts that have not turned a circuit on and off.
(b) After many on and off operations, these contacts show severe wear from arcing.
Fig. 7-35 Condition of relay contacts..
![Page 69: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/69.jpg)
![Page 70: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/70.jpg)
MK-S-series Power Relays with DC Switching Models That Can Switch 220 VDC, 10 A
![Page 71: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/71.jpg)
RELAY DESIGNED FOR USE WITH A PLC (PROGRAMABLE LOGIC CONTROLLER)
![Page 72: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/72.jpg)
HALL EFFECT P.194 THE PRODUCTION OF VOLTAGE ON OPPOSITE SIDES OFA CURRENT CARRYING SEMICONDUCTOR WHEN A MAGNETIC FIELD PASSESTHRU IT.
http://www.youtube.com/watch?v=_ATDraCQtpQHALL EFFECT ANIMATION
http://www.youtube.com/watch?v=fmZJqhzVXc4
![Page 73: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/73.jpg)
HALL EFFECT VOLTAGE DEPENDS ON:1 TYPE OF MATERIAL2 MAGNITUDE OF CURRENT3 AMOUNT OF FLUX
![Page 74: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/74.jpg)
![Page 75: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/75.jpg)
THIS VOLTAGE CAN BE USED AS A CONTROL DEVICE FOR MANY APPLICATIONS.
![Page 76: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/76.jpg)
Here the Hall effect device is used as an ammeter in a automobile. The current sensor consists of a ferrite core placed around the battery leads, with a Hall effect device positioned in the air-gap. A magnetic flux is induced in the ferrite Core when ever current flows through the leads and this flux passes through the Hall effect device which generates a proportional output voltage.
![Page 77: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/77.jpg)
![Page 78: FOWLER CHAPTER 7 LECTURE 7 MAGNETS AND ELECTROMAGNETISM](https://reader035.fdocument.pub/reader035/viewer/2022062408/56813bda550346895da5049e/html5/thumbnails/78.jpg)