Introduction Mathieu Bardoux · Mathieu Bardoux (IUTLCO GTE) Electricity First year 6 / 20....

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LITTORAL CÔTE D’OPALE Electricity Introduction Mathieu Bardoux IUT du Littoral Côte d’Opale Département Génie Thermique et Énergie First year

Transcript of Introduction Mathieu Bardoux · Mathieu Bardoux (IUTLCO GTE) Electricity First year 6 / 20....

  • LITTORAL CÔTE D’OPALE

    ElectricityIntroduction

    Mathieu Bardoux

    IUT du Littoral Côte d’OpaleDépartement Génie Thermique et Énergie

    First year

  • Summary

    1 Electric current

    2 Voltage and Power

    3 Electrical Resistance

    4 Hydraulic Analogy

    Mathieu Bardoux (IUTLCO GTE) Electricity First year 2 / 20

  • Electric current

    Summary

    1 Electric currentElectron ?Electric current

    2 Voltage and PowerVoltagePower

    3 Electrical ResistanceDefinitionJoule effect

    4 Hydraulic Analogy

    Mathieu Bardoux (IUTLCO GTE) Electricity First year 3 / 20

  • Electric current Electron ?

    Electron ?

    I Elementary particle (light particle or lepton)I Negative electric charge : −e , with e = 1,602176535×10−19 CI Electrons + Protons (charge : e) + Neutrons = Atoms

    Mathieu Bardoux (IUTLCO GTE) Electricity First year 4 / 20

  • Electric current Electron ?

    Atoms : structure and dimensions

    10−15 m

    10−10 m

    Mathieu Bardoux (IUTLCO GTE) Electricity First year 5 / 20

  • Electric current Electron ?

    Conductors vs Insulators

    Conductors : high conductivity / low resistivityI métals (copper, gold, aluminium, iron & alloys)I carbon (graphite, diamond, nanotubes. . . )I water (+ electrolytes)I human bodyI ground

    Insulators : low conductivity / high resistivityI glassI porcelainI paperI dry woodI rubberI plastic

    Mathieu Bardoux (IUTLCO GTE) Electricity First year 6 / 20

  • Electric current Electric current

    Electric current

    I overall flow of electric chargesI created by the action of electromagnetic forceI carriers : ions or (in most cases) electronsI in electrical networks, a generator produces a charge imbalance⇒ electrons move through a closed loop

    Mathieu Bardoux (IUTLCO GTE) Electricity First year 7 / 20

  • Electric current Electric current

    Current intensity

    i =dqdt

    By definition, 1A = 1C · s−1

    The current is measured using an ammeter connected in series.

    A

    i

    Mathieu Bardoux (IUTLCO GTE) Electricity First year 8 / 20

  • Electric current Electric current

    Conventions

    I Current can be created by positive or negative charge carriers.I Conventional current is arbitrarily defined as a positive charges

    flow.I By convention, the electrical current exits the generator through

    the positive (+) terminal and returns to the generator through itsnegative (-) terminal.

    I Inside the generators, the inverse convention applies.I The conventional direction may differ from the actual direction of

    the charge carriers.

    Mathieu Bardoux (IUTLCO GTE) Electricity First year 9 / 20

  • Electric current Electric current

    Propagation rate

    I Propagation rate of the electric current in a copper wire :273000 km · s−1

    I This is not the speed of electrons (a fraction of millimeter persecond)

    I Signal is faster than matter

    What distance does an electron travel in domestic network ?

    Mathieu Bardoux (IUTLCO GTE) Electricity First year 10 / 20

  • Electric current Electric current

    Propagation rate

    I Propagation rate of the electric current in a copper wire :273000 km · s−1

    I This is not the speed of electrons (a fraction of millimeter persecond)

    I Signal is faster than matter

    What distance does an electron travel in domestic network ?

    Mathieu Bardoux (IUTLCO GTE) Electricity First year 10 / 20

  • Electric current Electric current

    Effects

    I HeatingI Chemical decompositionI Mechanical actionI Creation of magnetic fieldsI . . .

    Mathieu Bardoux (IUTLCO GTE) Electricity First year 11 / 20

  • Voltage and Power

    Summary

    1 Electric currentElectron ?Electric current

    2 Voltage and PowerVoltagePower

    3 Electrical ResistanceDefinitionJoule effect

    4 Hydraulic Analogy

    Mathieu Bardoux (IUTLCO GTE) Electricity First year 12 / 20

  • Voltage and Power Voltage

    Voltage

    I Voltage between two points = work done per unit of chargeagainst a static electric field to move between these points.

    I Voltage unit = VoltI 1V = 1J ·C−1

    I Notation U (single-phase) or V (three-phase).I Measured with a voltmeter or an oscilloscope connected in

    parallel.

    V

    R

    −+U

    Mathieu Bardoux (IUTLCO GTE) Electricity First year 13 / 20

  • Voltage and Power Power

    Electrical power

    I Power = Energy per unit of TimeI Power unit = WattI 1W = 1J · s−1 and 1J = 1W · sI Power = flow of EnergyI Electrical power : P = U · I

    Mathieu Bardoux (IUTLCO GTE) Electricity First year 14 / 20

  • Electrical Resistance

    Summary

    1 Electric currentElectron ?Electric current

    2 Voltage and PowerVoltagePower

    3 Electrical ResistanceDefinitionJoule effect

    4 Hydraulic Analogy

    Mathieu Bardoux (IUTLCO GTE) Electricity First year 15 / 20

  • Electrical Resistance Definition

    Electrical resistance

    I Measurement of the difficulty to pass a current through acomponent

    I Leads to a drop in carriers energy when passing through thecomponent

    I Unit : OhmI Ohm’s law : U = R · I

    Mathieu Bardoux (IUTLCO GTE) Electricity First year 16 / 20

  • Electrical Resistance Joule effect

    Power dissipation in a resistor : Joule effect

    I Conversion of electrical energy into heat.I P = U · II P = R · I 2

    I P =U 2

    R

    Mathieu Bardoux (IUTLCO GTE) Electricity First year 17 / 20

  • Hydraulic Analogy

    Summary

    1 Electric currentElectron ?Electric current

    2 Voltage and PowerVoltagePower

    3 Electrical ResistanceDefinitionJoule effect

    4 Hydraulic Analogy

    Mathieu Bardoux (IUTLCO GTE) Electricity First year 18 / 20

  • Hydraulic Analogy

    Hydraulic AnalogyExample of a waterfall

    I Electrical charge⇔ Quantity of waterI Electrical current⇔ Hydraulic volume flow rateI Voltage⇔ Hydraulic head

    BFluid particles can move at variable speed

    Mathieu Bardoux (IUTLCO GTE) Electricity First year 19 / 20

  • Conclusion

    ConclusionIn this chapter we have seen. . .

    I how electric current is created in conductive materialsI the definitions of fundamental parameters of electric currentI the main properties of resistors

    Mathieu Bardoux (IUTLCO GTE) Electricity First year 20 / 20

    Electric currentVoltage and PowerElectrical ResistanceHydraulic Analogy