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Unit 3 - Electric Charge

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    AS Physics 9702 unit 3: Electric Charge 1

    UNIT 3ELECTRIC CHARGE

    ELECTRIC CIRCUITS:

    For the current to exist it must have a complete path of conductors. This complete path of conductorsis called electric circuit. For example copper wires, which are conductors, are used to connect lampsin a circuit to complete the path for the flow of charges. The battery is also attached to the circuit topush these charges around. To draw on a paper the diagram of complete path of charges is calledcircuit diagram. It contains symbols for every component of the circuit. Following are some commoncircuit symbols:

    There are two different ways of connecting circuit components in a circuit to the same battery. Theyare called series and parallel circuits. We will discuss about these circuits later in this section.

    ELECTRIC CHARGE:All matter is made up of atoms. Atoms have three elementary particles that are electrons, protons andneutrons. Since the atom and its particles are very small for us to observe we can understand thepresence of these atomic particles by rubbing two polythene rods (an insulator) with woolen cloth.These rods when brought close to each other they repel. It means that rods have acquired an electriccharge. There are two types of charges - the positive charge and negative charge. The positive chargeis carried by protons or positive ions and negative charge is carried by electrons or negative ions.Following table will describe how different substances behave when rubbed with different materials.

    Charging an object by rubbing is called electrostatic induction by rubbing or by friction.

    Material Rubbed with Charge acquired Behaviour

    Polythene rod Woollen cloth Negative Attract each otherPerspex Woollen cloth Positive

    Ebonite Fur Negative Attract each other

    Glass Silk positive

    It must be noted that the charges are not created by rubbing action. When polythene rod is rubbedwith a woolen cloth, some of the electrons of the surface atoms of the cloth transferred to the rod andtherefore the polythene rod become negatively charged and cloth becomes positively charge. Thatmeans that the charges are transferred from cloth to polythene and total charge is always conservedor same.

    The unit of charge is coulomb or C (capital C). The most common letters used to express charges areQ, q or e. Small e is specifically used for expressing the charge of elementary particle electron (e-)or proton (e

    +).

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    ELECTRIC FIELD:

    1. It is a field of electric force.2. An electric field is a space or region around a charged object Q where a

    stationary positive charge qo experience electric force.3. It is a vector quantity and its direction is along the direction where the

    positive charge would move. This means that the electric field is alwaysout from positive charge and in to negative charge.

    4. The electric field is represented by the radial straight lines around thecharge object. Stronger the field more the number of lines.

    Electric field intensity or electric field strength

    of an Eelectric charge

    1. The electric field intensity is defined as force per unit charge. Inequation form this is represented as:

    2. The unit of electric field intensity is newton per coulomb orN/C.3. The electric field around charge Q, is considered to be a uniform

    radial field. This means that a charge qo experiences same forcearound a charge object Q if it is at equal distance from the centre ofthe charge at any position.

    4. We can plot a graph of electric field intensityEagainst the distance rfrom its centre.We can see that the graph shows inverse square lawcurve that is Einversely proportional to r

    2.

    5. When two charged plates are placed together, the radial fields of thecharges combine to make a uniform electric field. Notice that the

    field bulges at the ends; generally we ignore this. In this case we canshow that the electric field intensity is given by a simplerrelationship:

    6. Eelectric field intensity; Vpotential difference betweenthe two plates and; d- distance between the two plates inmeters. In this case the unit of electric field intensity isvolts/metre V/m which is same as the other unit that isnewton/coulombN/C.

    7. When a charged particle is moving in between the twoparallel plates that are carrying opposite charges and

    have uniform electric field between the plates then thecharge particle experience a constant force centripetalperpendicular to the motion of the particle. Thedeflection of the particle will be towards the oppositecharge plate as show in the diagram.

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    AS Physics 9702 unit 3: Electric Charge 3

    Exercise no 3.1: Solve the following questions from past paper.

    1. Oct/Nov 2010, Paper 12, questions 28, 292. May/Jun 2010, Paper 12, questions 26, 27, 283. Oct/Nov 2009, Paper 12, questions 26, 27, 284. May/Jun 2009, Paper 1, questions 27, 28, 295. May/Jun 2008, Paper 1, questions 30, 31,6. Oct/Nov 2007, Paper 1, questions 26, 27

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    ELELCTIC CURRENT (I):

    Current (I) is defined as the rate of flow of electric charges (Q) inan electric circuit.

    The unit of current is ampere (A). Multiple units of ampere are:

    milli-ampere (mA) = 10-3

    A and micro-ampere (A) = 10-6

    A

    Current is measured by a device called ammeter or multimeter. There are two

    types of ammeters; analogue and digital.

    Electric charge (Q) in a conductor is carried by atomic particleselectrons ornegative ions. Unit of electric charge is coulomb (C). The quantity of electriccharge of electron or proton is 1.610

    -19C.

    One coulomb is defined as:

    a charge passing through any point in a circuit when a steady current of1 ampere maintained for 1 second, that is:

    1coulomb (C) = 1ampere (A)1second (t).

    Conventional current:

    The electric current is really a flow of electrons from negative to positive terminal of the battery.However when it was first discovered, scientists wrongly guessed that something that carries chargesflows from positive to negative terminal and therefore they describe it as conventional current.

    Whenever we study electric current and flow of charges we always consider conventional current thatis from positive to negative.

    Direct and alternating currents (d.c. and a.c.):

    The electrons constantly flowing around the circuit, from the negativeterminal of the battery to the positive terminal, produce direct current(d.c). All batteries produce direct current.

    In mains electricity at homes, the electrons in the circuit movebackwards and forwards 50 to 60 times in one second. This kind ofcurrent is called alternating current (a.c.). The main advantage of usingalternating current over direct current is it can be transmitted frompower stations to our homes at very high voltage which reduces theamount energy that is lost during the transmission.

    Movement of charges in liquids:Electrolysis:

    Electrolysis is the process in which chemical changes are occur in a conductingliquid when electric charges are passing through it.

    The conducting liquid is called electrolyte. The word electrolysis means theprocess of breaking molecules of conducting liquid into its parts (ions) by usingelectric current. Positive and negative poles of an electric source, such as abattery, can absorb opposite ions of an electrolyte, causing separation of ions andcreation of a new substance. Liquid metals are not electrolyte since they can passcurrent without there being any associated chemical change or making of ionsfor example in mercury which is liquid. However solution of sodium chloride(NaCl) in water is a good example of electrolyte. Some substances that do notconduct electricity is called non-electrolyte for example sugar-solution.

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    AS Physics 9702 unit 3: Electric Charge 5

    The figure illustrates a simple arrangement of producing electrolysis. The plates by which the currententers and leaves are called electrodes. Electrode connected to the positive terminal of the battery iscalled anode and an electrode connected to the negative terminal is called cathode. Consider theexample of sodium chloride (NaCl) in water as an electrolyte. It contains Na

    +and Cl

    -ions which are

    free to move in water and it conduct electric current. Solid sodium chloride cannot conduct electricitybecause ions are not free to move but when the current exists through the solution, NaCl splits intoNa+ and Cl- ions. Sodium ion (Na+) gains an electron at the cathode and deposit on the surface of theplate and similarly Chlorine ion (Cl-) losses an electron at anode and deposit on the surface of anode.

    Movement of charges in solids:

    Metals:

    The atomic structures of metals are such that each atom onaverage has one outer electron which is not required for

    bonding and which need not to remain attached with its atom.This electron is called free electron or de-localized electron.When the current does not exist these free electrons move

    randomly in all direction throughout the conductor. When thebattery is attached and potential difference is put across the

    conductor, it produces an electric field and affects the flow offree electrons. It pushes the free electrons towards the positive

    end of the battery. Thus this creates the flow of charges acrossthe conductor which means electric current.

    Exercise no 3.2: Solve the following questions from past papers.

    1. Oct/Nov 2009, Paper 12, question 332. Oct/Nov 2008, Paper 1, question 343. Oct/Nov 2007, Paper 1, question 30

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    SERIES AND PARALLEL CIRCUITS:

    Series Circuit:

    A series circuit is a circuit in which components (egresistors) are arranged in a chain, so the charges have only

    one path to follow. The current (rate of flow of charges) is same through each

    component in series circuit.

    The total resistance of the circuit is found by simply addingup the resistance values of the individual resistors. Equivalent resistance (R) in series circuit

    can be expressed by.

    whereR1 andR2 are the resistances of each resistor.

    In series circuit the total potential difference (battery voltage) is the sum of individualpotential differences (p.d.) across each resistor. That is

    V = V1

    + V2

    + ... where V1

    and V2

    are p.d. across the componentR1

    andR2.

    The current (I) is same in each resistance therefore the ammeter is connected in series withthe other resistances.

    In series circuit if one component breaks down then the whole circuit will stop working. More the resistance of the component, the higher the potential difference across it. In series circuit the voltage across each resistor divides according to the ratio of resistance

    value of each resistor.

    Parallel Circuit:

    A parallel circuit is a circuit in which the components arearranged such that each component is directly connected to

    the battery. The parallel circuit makes branches for thecurrent.

    The current in a parallel circuit breaks up with some currentflowing along each parallel branch and re-combining when

    the branches meet again.

    The voltage across each resistor in parallel circuit is same. Lesser the resistance in the branch more the current in that

    branch.

    Equivalent resistance of each component or resistors R1 andR2 in parallel circuit can be expressed by:

    or

    In parallel circuit the total current is the sum of individual currents in each branch.I = I1 + I2 +

    Voltage remains same across each resistor that is it has same value as the voltage of thebattery.

    The combine resistance of all resistors in parallel circuit is less than the least resistor in thecircuit.

    http://physi.files.wordpress.com/2010/02/parallel_circuit.jpghttp://physi.files.wordpress.com/2010/02/series_circuit.jpg
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    AS Physics 9702 unit 3: Electric Charge 7

    POTENTIAL DIFFERENCE:

    An electric potential difference (V) must exist for current to flowin an electric circuit.

    It is the work done per unit charge as the charge is moved

    between two points in an electric circuit.The potential difference (p.d.) between two points in a circuit is1V if 1J of electrical energy (E) is transferred to another form ofenergy (i.e. to chargers) when 1 coulomb (C) of charge (Q)passes from one point to another.

    or

    Replacing the from the definition of charge and current.

    The equation will be

    or

    Measuring potential difference:

    A voltmeter is used to measure the electric potential differencebetween two points in an electric circuit. It is connected in parallelacross a resistor in the circuit. It has a very high internal resistance.The unit of potential difference or voltage is volts.

    OHMS LAW:

    As the potential difference (V) is increased across a given material(ohmic material or metal) in a circuit, the current (I) flow through thematerial also increases.

    or

    The potential difference (V) between any two points in a conductor isdirectly proportional to the current (I) through it if the temperature,resistance of the conductor and other conditions are constant.

    whereR is the resistance of a conductor.

    RESISTANCE:

    The opposition of to the current in a conductor is called resistance of that conductor. All metals are good conductor of electricity. The best conductor is silver (%) and copper (%) is

    next to it. All substance have some degree of resistance, there is no substance possible without

    any resistance and normal temperature. Substances that do not carry current is called insulator. Germanium and silicon have conductivity

    in between conductors and insulators. They are called semiconductor.

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    The unit of resistance is ohm (Greek symbol omega ). One ohm is the resistance when currentof one ampere and potential difference of one volt is applied across the resistor.

    A resistance of a cylinder or wire of certain material: increases if its length (L) increases, increases if its cross-section area (A) decreases, depends upon the type of material

    where is the resistivity of the conductor which is constant for every material.

    Measuring resistance:

    The resistance (R) of a conductor is measured by ohm-meter.Alternatively the resistance of a conductor can be found by setting up

    the circuit shown in figure and measuring the current (I) and potentialdifference (V) applied across it. The resistance of the resistor R can be

    found by the formula

    . Multiple values of (V) and (I) can be

    recorded by changing the resistance of a variable resistor.

    By plotting the graph between VandIand finding the gradient of theline. The gradient is the resistanceR.

    Electromotive force (e.m.f.):

    In energy terms the e.m.f. is defined as:

    The energy when converted from any form (chemical or mechanical energy) to electrical energy thatit is used to drive one coulomb charge around the complete circuit. This energy per coulomb is calledelectromotive force or e.m.f.

    The e.m.f. of a battery is across its terminals when it is not connected to the circuit and it is sometimes

    called the terminal potential difference. When the circuit is closed, the voltage across the battery falls,because the energy and the voltage of the battery are lost across the internal resistance of battery.

    To measure e.m.f. or potential difference (p.d.) in a circuit the voltmeter should be connected inparallel. Voltmeter should always have very high internal resistance.

    Internal resistance of a cell:

    The p.d. across the terminals of a cell depends on the size of thecurrent being drawn. If no current is being drawn it means the cell isnot connected with the circuit then the potential difference betweenthe terminal has its maximum value and know as the electromotiveforce (e.m.f.) of the cell. This e.m.f. is solely because of the chemicalreaction occurring inside the cell.

    The chemical inside the cell creates a resistance to the current (I).This resistance is called the internal resistance (r) of the cell. When a

    cell is connected across an external circuit (loadR) some of the e.m.f. is used to drive current throughthe load and rest of the emf drives the same current through the internal resistance. The internal

    resistance behave as it is in series with the external resistance of the circuit. The equation for the two

    resistance connected in series is

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    AS Physics 9702 unit 3: Electric Charge 9

    or

    or

    whereIris the p.d. across the internal resistance and Vis the potentialdifference across the external resistance. From equation whenI=0 it

    means that the cell is not connected to any external resistance thenV=Ethe emf of the cell.

    Measurement of e.m.f. and internal resistance of a cell:

    1. Connect the circuit as shown in the diagram.2. Record six readings of voltmeter (V) and ammeter (I) of the cell by changing the values of

    variable resistanceR.3. The resistance of the voltmeter should be higher than the combine resistances ofrandR.4. Plot the graph between V(on y-axis) andI (on x-axis) and draw the best fit straight line. The

    equation of the straight line should be .

    5. Compare the straight line equation with the equation of e.m.f. or by rearranging .

    6. Comparing these two equations shows gradient of the line m isr and y-intercept c isE, the e.m.f. of the battery.

    7. The internal resistance of a typical 1.5Vcell is 1 if the currentis limited to 0.2A, the terminal PD will range from 1.5VwhenI= 0 to 1.3VwhenI=0.2A.

    Maximum power delivered by the cell:

    Consider the circuit diagram shown in the figure in which the e.m.f.of the cell is E, the internal resistance is r and driving current isIthrough a load of resistanceR. The power delivered by the cell to

    resistanceR is

    but we know that

    therefore by replacing

    The maximum power dissipated by cell is whenR=r. A givensource ofe.m.f. delivers maximum amount of power to a loadwhen the resistance of the load is equal to the internal resistance of

    the source.

    Exercise no 3.3: Solve the following questions from past papers.

    1. Oct/Nov 2007, Paper 1, question 292. Oct/Nov 2009, Paper 12, question 303. Oct/Nov 2010, Paper 22, question 64. Oct/Nov 2009, Paper 21, question 65. Oct/Nov 2009, Paper 22, question 66. Oct/Nov 2009, Paper 22, question 67. May/June 2008, Paper 1, question 388. May/June 2010, Paper 22, question 6(a)9. May/June 2008, paper 2, question 610. May/June 2007, paper 2, question 6

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    I-V Characteristic of various components:

    Metal:

    Metal conductors obey ohms law, provided their temperature doesnot change or we can say that the metal conductors have constantresistance provided its temperature is constant. TheI-Vgraph

    between current (I), on y-axis (dependent variable) and voltage (V)on x-axis (independent variable) is straight line.

    Diode:

    In semiconductor diode it allows the current only in one directionand that is forward bias connection. In diode the current is not proportional to voltage (or PD) appliedbecause when the PD is reversed, the current is almost zero. This is reverse biased connection.

    Filament:

    In tungsten filament as the current increases, the temperature also rises and the resistance goes up. Sothe current is not proportional to PD. This happens because as the current increases in the filament thetemperature also increases which increase the resistance of the conductor and decrease the flow ofcharges in the conductor.

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    AS Physics 9702 unit 3: Electric Charge 11

    Thermistor:A thermistor is a heat sensor (resistor) which changes its resistance with the change of

    temperature (heat) around it. Its resistance decreases as the temperature increases which isreverse to the normal conductor. For example:

    Icy water 0C has high resistance, about 12k.

    Room temperature 25C has medium resistance, about 5k. Boiling water 100C has low resistance, about 400.

    Thermistor is called input transducer. It means it changes its resistance withthe change in environment. TheI-Vgraph of a thermistor is not a straightline and therefore it does not obey Ohms law. As more current is throughthe thermistor the graph gets steeper. The thermistor is a semiconductor and

    conducts more electricity when heated. This is because as the temperatureincreases the thermistor makes available more free electrons to carry current.

    Therefore as the current increases the thermistor get hotter and releasingmore electrons resulting in a reduction in resistance.LDR (Light Dependent Resistor):An LDR is a light sensor (resistor) which changes its resistance with thebrightness of light around it. It is made from cadmium sulphide compound (CdS) and its resistance

    decreases as the brightness of light falling on the LDR increases.

    Darkness: maximum resistance, about 106. Very bright light: minimum resistance, about 100.

    LDR is called input transducer. It means it changes resistance with the change in environment. The I-V graph is a straight line. When light shines on it releases electrons which increases the number ofelectrons to carry the current. Thus, as the light increases the current increases resulting in a reductionin resistance. In dark however no extra electrons are available so the current experiences a greater

    resistance.

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    ELECTRIC POWER:

    Rate of doing work is called power. It is define as

    replacing

    replacing

    Unit of power is watts (W) and larger units are 1 kilowatt (kW) = 1000 W and 1megawatt (MW) =1000 000 W. The power of electrical appliances can be calculated by multiplying the current (I)

    passing through it by the potential difference (V) across it.

    Exercise no 3.4:

    Solve the quiz on the website

    http://www.learnabout-electronics.org/resistors_23.php

    Solve the following questions from past papers.

    1. May/June 2008, Paper 2, question 62. Oct/Nov 2007, Paper 1, question 29

    http://www.learnabout-electronics.org/resistors_23.phphttp://www.learnabout-electronics.org/resistors_23.phphttp://www.learnabout-electronics.org/resistors_23.php
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    AS Physics 9702 unit 3: Electric Charge 13

    KIRCHHOFFS LAW:

    Kirchhoffs first law Junction rule - Conservation of charge:

    At junction in a circuit, the total current entering is equal to the total current leaving it.

    Mathematically I=0

    In figure at junction A current I1 and I2 are approaching and current I3 is leaving therefore.

    Kirchhoffs second law Loop rule - Conservation of energy:

    In any closed loop in a circuit, the sum of the e.m.f. (E) must be equal to the sum of all the IRproducts.

    Mathematically

    E = IR

    In the circuit in e.m.f. of V1 is E1 and

    e.m.f. of V2 is E2. Considering the loop 1

    clockwise then the equation can be writtenas

    for loop 2 anticlockwise

    and for loop 3

    Substituting the values and solving thethree equations simultaneously we can find

    the values ofI1, I2 andI3.Rules for applying Kirchhoffs Law:

    1. Draw an arrow to show the direction of current in each branch of the circuit. Choose anydirection clockwise or anticlockwise. If you chose the wrong direction then the value of

    current will turn out to be negative.2. Mark each resistor with a plus sign at one end and minus sign at the other end, in a way that is

    consistent with the direction of current chosen in step 1. Mark each battery such that thepositive terminal considered as higher potential and negative terminal considered as lowerpotential. Conventional current always flow from higher potential to lower potential.

    3. While calculating the current through a battery the internal resistance is considered asseparate resistance.

    4. Apply first and second rule to the circuit and obtained as many independent equations asmany number of variables.5. Solve the equations simultaneously for the known variables.

    Exercise no 3.5: Solve the following questions from past papers.

    1. Oct/Nov 2007, Paper 1, question 292. May/June 2010, Paper 22, question 6(a)3. May/June 2009, paper 22, question 74. May/June 2009, paper 21, question 7

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    POTENTIAL DIVIDER OR VOLTAGE DIVIDER

    A potential (or voltage) divider is combination of two resistors, as shown in thefigure. The output voltage V2 from a potential divider will be a proportion ofthe input voltage V1 and is determined by the ratio of the two resistancevalues.

    In the arrangement of the circuit in the diagram the value of V2, the outputvoltage can be determine by the formula:

    V1 is the input voltage and R1 and R2 are the resistor in series. This arrangement is normally used to change voltage acrossa circuit

    component, for example to change the brightness of the lamp, or control the

    volume (loudness) in a hi-fi amplifier circuit.

    Potential divider and LDR:

    Now what happend when one of the resistors is replaced with LDR, the light

    dependent resistor. The resistance of LDR decreases as more light falls on it. It means that there will be low p.d. across R2 and high p.d. across R1. If a lamp is connected across R1 then the brightness of the lamp increases when the intensity of

    light falling on LDR decreases.

    Voltage divider circuit gives an output voltage which changes with illumination of thesurrounding.

    Potential divider and thermistor:

    We can consider the similar situation by replacing thermistor with the R2 in thecircuit.

    The resistance of thermistor decreases as the temperature rises. They are called negative temperature coefficient, or ntc thermistors. A typical

    ntc thermistor is made using semiconductor metal oxide materials.

    Semiconductors have resistance properties midway between those of conductorsand insulators.

    As the temperature rises, more charge carriers become available and the resistance falls. If we connect a lamp across the resistance R1, then the brightness of the lamp increases if the

    temperature of the surrounding increases.

    Exercise no 3.6: Solve the following questions from past papers.

    1. Oct/Nov 2007, Paper 1, question 292. May/June 2008, Paper 1, questions 36, 373. Oct/Nov 2007, Paper 1, questions 32, 334. May/June 2010, Paper 22, question 6(a)

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    AS Physics 9702 unit 3: Electric Charge 15

    Comparing the E.M.F.s of two cells:

    A potentiometer can be used to compare the e.m.fs oftwo cells. Consider the circuit below. A resistance wireof length one meter is connected with a cell called thedriver cell that will remain unchanged. Connect the cell

    X, of known E.M.F., with the circuit and find the nullpoint on the centre deflection ammeter by bringing in thesliding contact with the resistance wire. Measure thelength of resistance wire as LX (example 0.70m). Repeatthe same procedure by connecting the battery Y of

    unknown EMF in the circuit and find the length of wire as LY (example 0.90m).

    The ratio of the two e.m.fs is equal to the ratio of their lengths of resistance wire.

    Exercise no 3.7: Solve the following questions past papers.

    1. May/June 2008, Paper 1, question 382. Oct/Nov 2007, Paper 1, question 34

    Comparing Electric and Gravitational Fields

    There are many analogies that can be drawn between electric fields and gravitational fields.Theoretical physicists would go as far as saying that the two are possibly different expression of thesame thing. Let us compare the two:

    Feature Electric F ield Gravity F ield

    Exert force on Positive or negative charge Mass

    Constant of Proportionality

    where 0 is the permittivity of

    free space. The value ofcan be

    changed by adding a material.

    G

    The value ofG, the universalgravity constant has the samevalue for all media, including avacuum.

    Relationship with distance r Inversely proportional to r . Inversely proportional to r .

    Force Equation or

    Nature of force Can be attractive or repulsive andgoes from positive to negativecharge

    Always attractive pointingtowards the centre of the earth

    Acceleration in uniform field

    Relative strength Strong at close range Weak. Can only be felt when theobjects are massive

    Range Infinite Infinite

    The gravitational attraction between particles in an atom is so small and considered negligible. The

    nucleus and its electrons are held together entirely by electrostatic forces, and these are involved inchemical reactions. Gravity forces hold planets together and hold them in their orbits. Electrostatic

    forces over the interplanetary distances can be ignored.

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    Charge to mass ratio of electron

    The mass of an electron is 9.11 x 10-31

    kg, and its charge is 1.602 10-19

    C. These quantities are toosmall to directly measure, even if you were somehow able to isolate a single electron in thelaboratory. However, using principles of electromagnetism, indirect measurements of the charge andthe mass of the electron can be accomplished. These indirect measurements will be accomplished by

    taking advantage of quantities that are directly measurable in the laboratory setting. These directquantities will be derived from knowledge of the velocity of an electron moving in a magnetic field.

    Consider an electron of charge e is passing in between the two parallel plates of potential differenceV. The direction of electric field is perpendicular to the direction of motion of electron. Electroncreates a curved (trajectory path) attracting towards the positive plate. The electric potential energylost by electron is

    The kinetic energy gain by the electron at any particular instance is given by

    As the electron is accelerating in the electric field it loses its electric potential energy and gains thekinetic energy (a similar analogy as an object is falling towards the earth in gravitational field).

    Equate the two energies.

    Rearranging the equation

    Vthe p.d. across the two plates can be recorded from the battery voltage and speed of the electron canbe calculated from the distance travelled by the electron in between the two plates (that is length ofthe plates) and time taken. The charge to mass ratio e/m is also called the specific charge of electron.

    Electron-volt:

    It is the energy required to accelerate an electron through a potential difference of one volt.

    Replacing the quantity of charge as e = 1.610-19

    Cand potential difference as 1 volt in equation

    This implies that 1ev=1.610-19 joules

    It is a convenient energy unit, particularly for atomic and nuclear processes. It is the energy given to

    an electron by accelerating it through 1 volt of electric potential difference.