continuation to: circuit variables

31
Continuation to: Circuit Variables EE2001 Electrical Circuits I: 13 October 2021, Wednesday Asst. Prof. Dr. M. Alparslan Zehir E-mail : [email protected] Room : M4-228 (2nd floor)

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Continuation to:

Circuit Variables

EE2001 Electrical Circuits I:

13 October 2021, Wednesday

Asst. Prof. Dr. M. Alparslan Zehir

E-mail : [email protected]

Room : M4-228 (2nd floor)

2

EE2001 Course Information:Tentative Schedule:

Week Date Subjects The Related Chapter

from the Book

1 Oct. 6, 7 Introduction and Circuit Variables 1

2 Oct. 13, 14 Circuit Elements 2

3 Oct. 20, 21 Simple Resistive Circuits 3

4 Oct. 27, 28 Node Voltage Analysis 4

5 Nov. 3, 4 Mesh Current Analysis 4

6 Nov. 10, 11 Thevenin and Norton Equivalents 4

7 Nov. 17, 18 The Operational Amplifies 5

8 Midterm Week

9 Dec. 1, 2 Inductance and Capacitance 6

10 Dec. 8, 9 Response of First-Order RL and RC Circuits 7

11 Dec. 15, 16 Natural and Step Responses of RLC Circuits 8

12 Dec. 22, 23 Sinusoidal Steady-State Analysis 9

13 Dec. 29, 30 Continuation to: Sinusoidal Steady-State Analysis 9

14 Jan. 5, 6 Sinusoidal Steady-State Power Calculations 10

15 Jan 12, 13 Continuation to: Sinusoidal Steady-State Power Calculations 10

16 Jan. 19, 20 Review

Outline5. Voltage and Current

6. The Ideal Basic Circuit Element

7. Passive Sign Convention

8. Power and Energy

3

• Voltage (electric potential) is electric potential energy per unit charge:

𝑣 =𝑑𝑤

𝑑𝑞

• Electric current is the rate of charge flow:

𝑖 =𝑑𝑞

𝑑𝑡

• The voltage has a polarity and the current has a direction.

• Although in reality electrons are moving from negative terminal to positive terminal, the

current flow direction is conventionally assumed from positive terminal to negative terminal.

• Although the charge is a discrete quantity, there are enormous number of charge and the

current is treated as a continuous quantity.

• If two physically different circuit elements have the same current-voltage characteristics,

their circuit models are identical and they are identical from the point of circuit analysis.

Voltage and Current

4

5𝑣 : the voltage in volts

𝑤 : the energy in joules

𝑞 : the charge in coulombs

𝑖 : the current in amperes

𝑡 : the time in seconds

The Ideal Basic Circuit Element

5

6

• An ideal basic circuit element has three attributes:

It has only two terminals,

It is described mathematically in terms of current and/or voltage,

It can not be subdivided into other elements.

• Idel basic circuit elements form the building blocks for constructing circuit models.

Passive Sign Convention

6

7• You can assume either voltage polarity or current direction arbitrarily.

• After one of them is chosen, it dictates the assumed direction of the other parameter.

• Which means, once one of these are assigned,

the corresponding equations must be written

accordingly (consistency between the equations).

• These assumptions provide reference voltage

polarity and current directions. It has nothing

to do with actual directions.

• These assumptions are done for each element one by one, independent from the other

elements in the circuit.

• The most commonly used sign convention is the passive sign convention.

7

7

• The Passive Sign Convention: If the reference direction of the current in a circuit element

is in the direction of the reference voltage drop across the circuit element, use a

positive sign in any expression that relates the voltage to the current. Otherwise, use a

negative sign.

• Basically, positive current enters the positive

voltage terminal.

Passive Sign Convention

• An example:

8

7

+-5 V

0.5 A

+

-𝑣1

𝑖1+ -𝑣2

𝑖2

𝑖3+

-

𝑣3

+

-

𝑣4𝑖4

After calculating the values for each, the negative values mean that the related parameter is in

the inverse direction than your assumption (which is ok).

Passive Sign Convention

Power and Energy

9

8

• Power and energy calculations are also important in circuit analysis.

• These can be the output of the circuit converted to other forms.

• The circuit elements have power specifications which need to be considered in a design

process.

• Power is the time rate of energy consumption or supply.

• The power can be expressed in terms of the current and the voltage

𝒑 =𝑑𝑤

𝑑𝑡=𝑑𝑤

𝑑𝑞

𝑑𝑞

𝑑𝑡= 𝒗𝒊

• For 𝒑 > 𝟎 the circuit element absorbs power from the circuit.

• For 𝒑 < 𝟎 the circuit element delivers power to the circuit.

10

End of the topic:Circuit Variables

Any questions?Supplementary videos: Enter Youtube-> Search for ‘Alparslan Zehir’ -> Go to Playlists -> Watch ‘Electrical Circuits’ playlist

Asst. Prof. Dr. M. Alparslan Zehir

E-mail : [email protected]

Room : M4-228 (2nd floor)

Circuit Elements

EE2001 Electrical Circuits- I:

13 November 2021

From our course book*

12*James W. Nilsson, Susan A. Riedel: “Electric Circuits”, 9th Ed., Prentice Hall, New Jersey, 2011.

Developing models that provide an understanding that is imperfect but adequate

for solving practical problems lies at the heart of engineering.

Outline

1. Introduction to Circuit Elements

2. Voltage and Current Sources

3. Electrical Resistance (Ohm’s Law)

13

There are five ideal circuit elements:

• Voltage sources

• Current sources

• Resistors

• Inductors

• Capacitors

First we will learn,

• Voltage sources

• Current sources

• Resistors

Introduction to Circuit Elements

14

1

Why?

Many practical system can be modelled with them

Relative simplicity, algebraic equations

Active elements: can generate electrical energy

Passive elements: cannot generate electrical energy

Voltage and Current Sources2

• An electrical source is a device which is capable of converting non-electric (other type of)

energy to electric energy and vice versa (e.g. battery, dynamo).

• They either deliver or absorb electric power, maintaining either voltage or current. This

behavior led to the development of the ideal voltage source and ideal current source as

basic circuit elements.

• An ideal voltage source maintains a specified voltage across its terminals

regardless of the current flowing in those terminals.

• An ideal current source maintains a specified current through its terminals

regardless of the voltage across those terminals.

Voltage and Current Sources

16

2

• The circuit symbols for independent sources:

Voltage and Current Sources

17

2

Ideal independent

voltage source

Ideal independent

current source

Value of the supplied voltage

and

the reference polarity

Value of the supplied current

and

the reference direction

• There are also dependent sources.

• The value of a dependent source depends on the value of the current or voltage

somewhere else in the circuit.

• The value of the dependent source can be specified only when the value of the voltage or

current it depends on is known.

• Dependent sources are also known as controlled sources.

• There are four possible types of dependent sources.

Voltage and Current Sources

18

2

• The circuit symbols

for dependent sources:

Voltage and Current Sources

19

2

Voltage-controlled voltage source Voltage-controlled current source

Current-controlled voltage source Current-controlled current source

µ is a dimensionless

multiplying constant

𝝆 has the dimension

volts per ampere

𝜶 has the dimension

amperes per volt

𝜷 is a dimensionless

multiplying constant

• Examples:

Voltage and Current Sources

20

2

Valid

ValidValid

Invalid

• Examples:

Voltage and Current Sources

21

2

Invalid

ValidInvalid

Valid

Electrical Resistance (Ohm’s Law)3

(an example)

Electrical Resistance (Ohm’s Law)

23

3

• Resistance is the ability of materials to impede the flow of current.

• Resistor is the circuit element used to model this behavior.

• Moving electrons that make up electric current interacts with and being resisted by the

atomic structure of the material. Through this interactions some amount of electrical energy

is converted into thermal energy and dissipated in the form of heat.

• This may be undesirable in many applications. On the other hand, several electrical

devices take advantage of resistance such as stoves, irons, space heaters, water heaters.

• Materials such as copper and aluminum have very small resistances (they are good

conductors). Usually they are not modeled as a resistor in the circuit.

Resistor symbol

Electrical Resistance (Ohm’s Law)

24

3

• The current-voltage characteristics of resistors obey Ohm’s Law, using the passive sign

convention:

Resistor symbol with an example value

Riv Riv

• The SI unit for resistance is Ohm (Ω) (1Ω = 1V/1A).

• This model of ideal resistor assumes a constant resistance. In reality resistance can vary

(e.g. depending on the temperature).

6 Ω

Electrical Resistance (Ohm’s Law)

25

3Flashback to passive sign convention (a topic covered in the past weeks):

• You can assume either voltage polarity or current direction arbitrarily.

• After one of them is chosen, it dictates the assumed direction of the other parameter.

• Which means, once one of these are assigned,

the corresponding equations must be written

accordingly (consistency between the equations).

• These assumptions provide reference voltage

polarity and current directions. It has nothing

to do with actual directions.

• These assumptions are done for each element one by one, independent from the other

elements in the circuit.

• The most commonly used sign convention is the passive sign convention.

Electrical Resistance (Ohm’s Law)

26

3

Flashback to passive sign convention (a topic covered in the past weeks):

• The Passive Sign Convention: If the reference direction of the current in a circuit element

is in the direction of the reference voltage drop across the circuit element, use a

positive sign in any expression that relates the voltage to the current. Otherwise, use a

negative sign.

• Basically, positive current enters the positive

voltage terminal.

Flashback to passive sign convention (a topic covered in the past weeks):

• An example:

Electrical Resistance (Ohm’s Law)

27

3

+-5 V

0.5 A

+

-𝑣1

𝑖1+ -𝑣2

𝑖2

𝑖3+

-

𝑣3

+

-

𝑣4𝑖4

After calculating the values for each, the negative values mean that the related parameter is in

the inverse direction than your assumption (which is ok).

Electrical Resistance (Ohm’s Law)

28

3

• The reciprocal of resistance is conductance:

• The SI unit for conductance is Siemens (S).

• Sometimes it is also referred to as Mho ().

RG

1

Electrical Resistance (Ohm’s Law)

29

3

• Calculation of the power dissipated by a resistor (always positive, always absorbs power):

R

vi

R

vi

Riv Riv

vip vip

Rip 2

R

vp

2

Rip 2

R

vp

2

iiRp )( iiRp )(

Electrical Resistance (Ohm’s Law)

30

3

• Power equations using conductance:

G

ip

2

Gvp 2

iG

ip )1

(R

vR

R

vp )(

vGG

vGp )1

(

G

Gvp

22

31

End of the Lesson (13.10.21)

Any questions?Supplementary videos: Enter Youtube-> Search for ‘Alparslan Zehir’ -> Go to Playlists -> Watch ‘Electrical Circuits’ playlist

Asst. Prof. Dr. M. Alparslan Zehir

E-mail : [email protected]

Room : M4-228 (2nd floor)