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8/20/2019 2.SIMPLE ELECTRICAL SYMBOLS AND UNITS BY NDAKO MAIMUNA ALIYU(MRS).ppt
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Simple electrical symbols&units
By
Ndako Maimuna Aliyu
1simple electrical symbols and
units. by Ndako M.A.
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•Electrical current
• Voltage(emf & p.d)
•Resistance
•
Ohm’s law•Capacitance
•Conductors and insulators
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Introduction
Electron theory; All matter is composed ofatom. The nucleus or centre of an atom hasprotons with a positive polarity or ‘charge’ andneutrons with no charge.
The nucleus is surrounded by one or moreelectrons with a negative polarity. These twopolarities indicate 2 opposite characteristicsthat is fundamental in all physical
applications.
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The arrangement of electrons & protons
are basic particles of electricity thatdetermines the electrical characteristicsof all substances. when a material hasboth electrons and protons in it, No
evidence of electricity is seen because thenumber of electrons equal that of protonsin which case the opposite electrical
forces cancels out making the materialelectrically neutral.
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Note however that, it is the opposing
characteristics that provide a method ofbalancing one against the other.
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THE CHARGE;This is a property that
causes the opposite polarities (+ve & -ve )to attract or repel each other as the casemaybe. See the example below.
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VOLTAGE(potential difference);
potential refers to the possibility of doing work. Any charge has the potential(i.e. ability to dowork)of moving another charge by eitherattraction or repulsion. Therefore potential
difference refers to the difference of electricpotential between the two points of an electriccircuit .as seen below;
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Its symbol is V and the unit of measurement isvolts.The instrument used to measure the potential
difference is called as Voltmeter. The voltmeteris always connected in parallel with the circuitwhose voltage is to be calculated. As shown in asimple circuit below.
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Volt is a measure of the amount of work orenergy needed to move an electric energy.
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The required work to be done or pressure is also
needed to direct the electric charge to flow in auniform direction. i.e. from a low potential to ahigh potential. The force or pressure is referredto as electromotive force. Thus electromotiveforce is simply defined as work done per unit ofcharge.
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For instance, in the figure shown below, a
resistor is connected to the source of energy,here a battery, consider that the wires whichare connecting the resistor and battery areoffering no resistance to the flow of current.
Battery has two terminal +ve and –veterminals. +ve terminal at higher point ascompared to –ve terminal .
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Now if the internal resistance of the battery isneglected, there is a potential difference acrossthe battery. Terminal voltage of battery isequal to its electromotive force. Note howeverthat in practical situations, there would alwaysbe internal resistance of the battery wheneverthere is current flowing in the circuit.
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ELECTRICAL CURRENT;Is simply said
to be a continuous flow of electrons. Electronsmove because protons are 1800 times heavierand it is the movement of free electrons thatprovide s electric current in a metal conductor.
Current is often referred to as charge in motion.That is when the potential difference betweentwo charges forces a third charge to move, thecharge in motion is an electric current.
To produce a movement of an electron, it isnecessary to either have a –vely charged field“push it” or a +vely charged field “pull it”
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Its symbol isIand its unit is Ampere(A).The current in a circuit is measured by the
instrument known as Ammeter. Ammeter isalways connected in series with the circuit.
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AMPERE (A) It is a measurement thatcombines the quantity of electricity and thelength of time it takes the electricity to travel a
certain distance. One amp is the same as onecoulomb per second. I=Q/t.
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ALTERNATING CURRENT;If the
current changes direction after equal intervalsof time, it is called an alternating current,written as ac or AC.
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A frequency associated with the alternatingfrequency (A.C) is called alternating frequency.This frequency is the rate at which currentchanges its direction with respect to time.
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DIRECT CURRENT;If the current alwaysflows in the same direction, it is called Directcurrent and its represented as D.C or d.c. e.g.the current generated from a cell or battery is
D.C because its unidirectional. The +ve and –veterminals are fixed or it is single polarity.
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ELECTRICAL RESISTANCE;Whilediscussing electrical current, we learnt thatcertain materials such as copper have many freeelectrons while substances such as glass, andrubber have fewer free electrons. some othersubstances like mica have no free electrons atall thus making them good insulators. Betweenthe very good conductors such as silver, copper
and very good insulators e.g. glass and rubberlay other conductors of reduced conductingability. They “oppose” or “resist” the flow ofelectrons hence the term resistance.
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Electrical Resistance is the property of an
electrical element to oppose the flow of theelectrical current passing through it whenvoltage is applied across the element.
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Its symbol is R and its unit is ohm . Theinstrument that measures the resistance is
known as ohmmeter.Mathematically it is represented as the ratio ofvoltage to current. i.e. R=V/I
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OHM Ω;
The resistance or opposition to the flow ofelectrical current or electricity. It takes one voltto push one ampere through one ohm ofresistance, this is known as ohms law.
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OHM’S LAW;
The electric potential difference between twopoints on a circuit (V) is equivalent to the∆product of the current between these two points(I) and the total resistance of all electrical
devices present between these two points. (R).
∆ V=I·R
This law can be represented or rearranged as
I=V/R∆
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I=V/RThe equation above indicates the two
variables that would affect the amount ofcurrent in a circuit. The current in a circuit isdirectly proportional to the electric potentialdifference impressed across its end and
inversely proportional to the total resistanceoffered by the external circuit. The greaterthe Emf, the greater the current and the lessthe resistance. The greater the resistance, the
less the current .Charge flows at the greatest rates when thebattery voltage is increased and the
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The ohm’s law equation is often explored in
laboratory using a Resistor, a battery packand a Multimeter. The Multimeter is used tomeasure both current and voltage when setappropriately.
By alternating the number of cells in thebattery pack, the emf across the externalcircuit can be varied.
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CAPACITANCE C; In the topic current we learnt of the unit of
measuring electrical quantity or charge was acoulomb. Now a capacitor (formerly condenser)has the ability to hold a charge of electrons.The number of electrons it can hold under agiven electrical pressure (voltage) is called itscapacitance or capacity. Two metallic platesseparated by a non-conducting substance
between them make a simple capacitor.
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The symbol of a capacitor is seen below in a
simple circuit charged by a battery
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In the circuit above, when the switch is openthe capacitor has no charge upon it, when theswitch is closed current flows because of thevoltage pressure, this current is determinedby the amount of resistance in the circuit. At
the instance the switch closes the emf forceselectrons into the top plate of the capacitorfrom the negative end of the battery and pullsothers out of the bottom plate toward the
positive end of the battery.
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Two points need to be considered here. Firstlyas the current flow progresses more electrons
flow into the capacitor and a greater opposingemf is developed there to oppose further currentflow, the difference between battery voltage andthe voltage on the capacitor becomes less and
less and current continues to decrease. Whenthe capacitor voltage equals the battery voltageno further current will flow.The second point is if the capacitor is able tostore one coulomb of charge at one volt it is saidto have a capacitance of one Farad.
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CONDUCTORS;The behavior of an object that has been charged
is dependent upon whether the object is madeof a conductive or a nonconductive material.conductors are materials that permit electronsto flow freely from particle to particle. An objectmade of a conducting material will permitcharge to be transferred across the entiresurface of the object. If charge is transferred to
the object at a given location, that charge isquickly distributed across the entire surface ofthe object. The distribution of charge is theresult of electron movement.
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Since conductors allow for electrons to be
transported from particle to particle, a chargedobject will always distribute its charge until theoverall repulsive forces between excesselectrons is minimized. If a charged conductor
is touched to another object, the conductor caneven transfer its charge to that object. Thetransfer of charge between objects occurs morereadily if the second object is made of a
conducting material. Conductors allow forcharge transfer through the free movement ofelectrons.
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SIEMENS S
Siemens measures conductance, or how easilyan electric current flows through an object.
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INSULATORS;
In contrast to conductors,insulators arematerials that impede the free flow of electronsfrom atom to atom and molecule to molecule. Ifcharge is transferred to an insulator at a given
location, the excess charge will remain at theinitial location of charging. The particles of theinsulator do not permit the free flow of electrons;subsequently charge is seldom distributed evenly
across the surface of an insulator.
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Conductive objects are often mounted upon
insulating objects. This arrangement of aconductor on top of an insulator preventscharge from being transferred from theconductive object to its surroundings. This
arrangement also allows for the personcarrying out the experiment to manipulate aconducting object without touching it. Theinsulator serves as a handle for moving the
conductor around on top of a lab table
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If charging experiments are performed with
aluminum pop cans, then the cans should bemounted on top of Styrofoam cups. The cupsserve as insulators, preventing the pop cansfrom discharging their charge. The cups also
serve as handles when it becomes necessary tomove the cans around on the table.
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Examples of Conductors and InsulatorsExamples of conductors include metals, aqueous solutions
of salts (i.e.,ionic compoundsdissolved in water),graphite, and the human body. Examples of insulatorsinclude plastics, Styrofoam, paper, rubber, glass and dryair. The division of materials into the categories ofconductors and insulators is a somewhat artificial
division. It is more appropriate to think of materials asbeing placed somewhere along a continuum. Thosematerials that are super conductive (knownassuperconductors) would be placed at on end and the
least conductive materials (best insulators) would beplaced at the other end. Metals would be placed near themost conductive end and glass would be placed on theopposite end of the continuum
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Note however that, The conductivity of ametal might be as much as a million trillion
times greater than that of glass.
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SUMMARYThere are many atoms around us which
carry fundamental particles. Thesefundamental particles; electrons and protonswhich carry –ve and +ve charges are the
reason for electricity. The particles neutronsand protons are present in the nucleus whileelectrons are moving around the outer shell ofthe atom. The movement of electrons is the
reason for electricity in which the effect isseen in our everyday life e.g. lightening whichis a spark or flashlight.
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Electrical current; This is themovement of charge by a potential difference.
If the current changes direction at equalintervals it is said to be an alternatingcurrent(A.C) while it is called a directcurrent(D.C) when it flows in the samedirection. Voltage(emf or p.d); Is the electrical
pressure or force that is required to force a
current through a resistance.Resistance; Because conductors are notperfect, they resist to some degree the flow ofcurrent.
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The resistance of a conductor is its voltage
drop divided by the current flowing throughthe conductor. This is also known as OHM’SLAW. The law is simply represented as R=V/I.measured in .
Ohm’s law can be simplified using what I callthe “WATER DISPENSER ANALOGY”
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Quantity Symbol Equation(s) Standard
Metric UnitOther Units
Voltage(emf
or p.d)∆V
∆V = ∆PE / Q
∆V = I • R
Volt (V) J / C
Current I
I = Q / t
I = ∆V / R
Amperes (A)
Amp or C / s
or V / Ω
Resistance R
R = ρ • L / A
R= ∆V / I
Ohm (Ω) V / A
Table of electrical units and
symbols
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References:1.Fundamentals of electric circuits by Mitchel ESchulz2.Grob’s basic electronics by Charles K. Alexander andMathew N.O. Sadiku.
3. Getting started in electronics by Forrest M Mims III4.www.physicsclassroom.com/current electricity5.physics.tutovista.com/electricity-and-magnetism/electri-current.html6.www.rapidtables.com
7.www.completepowerelectronics.com8.www.electronics-tutorials.com