lecture 1 fundamental of electricity

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By SY Cheung EL / IVE (HW) LECTURE 1Fundamental of Electricity EEE3404 – Electrical Engineering Principles 1

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Page 1: Lecture 1   fundamental of electricity

By SY CheungEL / IVE (HW)

LECTURE 1

Fundamental of Electricity

EEE3404 – Electrical Engineering Principles 1

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2© Vocational Training Council, Hong Kong EEE3404 Electrical Engineering Principles 1 Weeks 1 ~ 2

1. Atom Model Nucleus

Electron

Fundamental of Electricity

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2. Atom

• Protons

• Neutrons

• Electrons

Fundamental of Electricity

“Each atom has the same number of protons and electrons.”

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4© Vocational Training Council, Hong Kong EEE3404 Electrical Engineering Principles 1 Weeks 1 ~ 2

3. Proton and Electron

Protons carries positive charge

– it is relatively large mass

– does not play active part in electrical current flow

Electrons carries negative charge

– light mass

– play an important role in electrical current flow

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4. Unit of Charge

• Unit of Charge is called Coulomb (C)

• An electron and a proton have exactly same amount of charge

• One coulomb of charge is equal to approximately 628 x 1016 electron charge

Fundamental of Electricity

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5. Free Electrons

Free Electrons

Applying Heat or Light

Fundamental of Electricity

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6. Electrical Materials

All material may be classified into three major classes:

Fundamental of Electricity

• Conductors (copper, aluminum, siliver,

platinum, bronz, gold)

• Semiconductors (germanium, silicon)

• Insulators (glass, rubber, plastic, air,

varnish, paper, wood, mica, ceramic,

certain oils)

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8© Vocational Training Council, Hong Kong EEE3404 Electrical Engineering Principles 1 Weeks 1 ~ 2

• Conductors have many free electrons which will be drifting in a random manner within the material

6. Electrical Materials

Fundamental of Electricity

• Insulators have very few free electrons

• Semiconductors falls somewhere between

these two extremes

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9© Vocational Training Council, Hong Kong EEE3404 Electrical Engineering Principles 1 Weeks 1 ~ 2

7. Electric current

• Electric current is the movement, or flow of electrons through a conductive material

• It is measured as the rate at which the charge is moved around a circuit, its unit is ampere (A)

I=Q/t or Q=It

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10© Vocational Training Council, Hong Kong EEE3404 Electrical Engineering Principles 1 Weeks 1 ~ 2

8. Electromotive Force

• In order to cause the 'free' electrons to drift in a given direction an electromotive force must be applied

• The emf is the 'driving' force in an electrical circuit

• The symbol for emf is E and the unit of measurement is the volt (V)

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8. Electromotive Force

Typical sources of emf are cells, batteries and generators

The amount of current that will flow through a circuit is related to the size of the emfapplied to it

Fundamental of Electricity

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9. Potential Difference (p.d.)

• Whenever current flows through a circuit element in a circuit such as resistor, there will be a potential difference(p.d.) developed across it

• The unit of p.d. is volts(V) and is measured as the difference in voltage levels between two points in a circuit

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9. Potential Difference (p.d.)

• Emf (being the driving force) causes current to flow

• Potential difference is the result of current flowing through a circuit element

• Thus emf is a cause and p.d. is an effect

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9. Potential Difference (p.d.)

LOAD

P.D.=1.4 V

E.m.f.=1.5V, Rint.

Equivalent circuit of a battery

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10. Resistance

• Resistance is the 'opposition' to the current flow measured in ohms (Ω)

• Conductors have a low value of resistance

• Insulators have a very high resistance

• Load in DC/AC circuits

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Circuit convention

+

-

+

-

I

E VR

11. Ohm’s Law

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11. Ohm’s Law

It states that current in a resistive circuit is directly proportional to its applied voltage and inversely proportional to its resistance provided that all other factors (e.g. temperature) remain constant.

IRVorI

VRor

R

VI.e.i ===

V

IR

Slope = 1/R

V

I

V α I

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12. Power

Power (P) is defined as the rate of doing work (W).

havewet

QIand

Q

WVSince

Wwattst

WPei

==

= )(..

Additional relationships are obtained by substituting

V=IR and I=V/R, we have:

P = VI

R

VPandRIP

22

==

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13. Resistors in Series

E

I

V1

V2

V3

R1

R2

R3

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By Ohm's law

• V1 = IR1 volts;

• V2 = IR2 volts; and

• V3 = IR3 volts

• E = V1 + V2 + V3

• E = I (R1 + R2 + R3)

13. Resistors in Series

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• E = IReq and

• Req = R1 + R2 + R3 ohm

• where Req is the total circuit resistance

when resistors are connected in series the total resistance is found simply by adding together the resistor values

13. Resistors in Series

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14. Potential Divider

The voltage drops shared by the resistors

are given as follows:

• V1=E x R1/ (R1+ R2+ R3)

• V2=E x R2 / (R1+ R2+ R3)

• V3=E x R3 / (R1+ R2+ R3)

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15. Resistors in Parallel

R1

R2

R3

I1

I2

I3

I

E

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By Ohm’s Law

I1=E/ R1

I2=E/ R2

I3=E/ R3

15. Resistors in Parallel

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The total current of the circuit I is the sum of I1, I2 and I3 , thus

I = I1 + I2 +I3

15. Resistors in Parallel

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The total resistance or the equivalent resistance(Req) of the circuit is defined to be

Req= E/I

15. Resistors in Parallel

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By substituting the above expression for the currents, we have

E/Req=I=E(1/R1+1/R2+ 1/R3)

Thus we found

1/Req=(1/R1+1/R2+ 1/R3)

15. Resistors in Parallel

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Quiz

Calculate the total resistance of the following resistors connected in parallel:

a)30 Ω, 60 Ω

b)180 Ω, 90 Ω, 60 Ω, 60 Ω

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16. Current Divider

The current in each branch of the circuit is

given as

• I1= I x Req/ R1

• I2= I x Req/ R2

• I3= I x Req/ R3

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17. Power and Energy in a resistive

circuit

Power is equal to the current multiplied by the voltage and the unit of power is watt (W)

P = I x E (W)

Energy is equal to the power multiplied by the time for the circuit being energized. The unit is Joule (J).

Energy = P x t (J)

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18. Power in a resistive circuit

By Ohm's law E=IR, the above equation can be modify to be

P = I2R

Power is equal to the current squared, multiplied by the resistance.

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Use Ohm's law again, where I =E/R, we have

P=E2/R

Power is equal to the voltage squared, divided by the resistance.

18. Power in a resistive circuit

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Example 1

RBC

E=10V

I

VAB

VBC

VCD

2Ω 5Ω 3Ω

A B C D

RAB

RCD

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•VAB + VBC + VCD is exactly equal to the emf=10V

•The total resistance of the circuit is 2+5+3=10Ω

•By Ohm's law V=IR, the current I should be equal to 1A

Example 1 - Answer

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• VAB = IRAB =1 x 2 = 2V.

• VBC = I RBC =1 x 5 = 5V.

• VCD = IRCD =1 x 3 = 3V.

• Power dissipation in RAB = I2RAB = 12 x 2 = 2W.

• Power dissipation in RBC = I2RBC = 12 x 5 = 5W.

• Power dissipation in RCD = I2RCD = 12 x 3 = 3W.

• Total power dissipated = 2+5+3 =10W

Example 1 - Answer

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Example 2

R1

R2

R3

I1

I2

I3

I

E=6V

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–The potential difference across each of the three resistors is equal to the battery emf 6V

–Apply Ohm's Law

• E=I1 R1 ; I1=E/R1 = 6/2 = 3A

• E=I2 R2 ; I2=E/R2 = 6/3 = 2A

• E=I3 R3 ; I3=E/R3 = 6/6 = 1A

Example 2 - Answer

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• The total current I is equal to the sum of currents

• I1+I2+I3 = 3+2+1 =6A.

• Power dissipation in R1 = I12R1 = 32 x 2 = 18W.

• Power dissipation in R2 = I22R2 = 22 x 3 = 12W.

• Power dissipation in R3 = I32R3 = 12 x 6= 6W.

• Total power dissipated =18+12+6 =36W

Example 2 - Answer

Fundamental of Electricity