Electric circuits-chapter-2 Basic Laws

Preview:

DESCRIPTION

 

Citation preview

Chapter 2Basic Laws

04/09/23

DKS1113 Electric Circuits

04/09/23 2/43

Introduction

Fundament laws that govern electric circuits: Ohm’s Law. Kirchoff’s Law.

These laws form the foundation upon which electric circuit analysis is built.

Common techniques in circuit analysis and design: Combining resistors in series and parallel. Voltage and current divisions. Wye to delta and delta to wye transformations.

These techniques are restricted to resistive circuits.

DKS1113 Electric Circuits

Ohm’s Law

04/09/23 3/43

DKS1113 Electric Circuits

04/09/23 4/43

Ohm’s Law

Relationship between current and voltage within a circuit element.

The voltage across an element is directly proportional to the current flowing through it v α i

Thus::v=iR and R=v/i Where:

R is called resistor. Has the ability to resist the flow of electric current. Measured in Ohms (Ω)

DKS1113 Electric Circuits

04/09/23 5/43

Ohm’s Law

v=iR

*pay careful attention to current direction

DKS1113 Electric Circuits

04/09/23 6/43

Ohm’s Law

Value of R :: varies from 0 to infinity

Extreme values == 0 & infinity.

Only linear resistors obey Ohm’s Law.

Short circuitShort circuit Open Circuit Open Circuit

DKS1113 Electric Circuits

04/09/23 7/43

Ohm’s Law

Conductance (G) Unit mho or Siemens (S).

Reciprocal of resistance R

G = 1 / R

Has the ability to conduct electric current

DKS1113 Electric Circuits

04/09/23 8/43

Ohm’s Law

Power:

P = iv i ( i R ) = i2R watts (v/R) v = v2/R watts

R and G are positive quantities, thus power is always positive.

R absorbs power from the circuit Passive element.

DKS1113 Electric Circuits

04/09/23 9/43

Ohm’s Law

Example 1: Determine voltage (v), conductance (G) and power

(p) from the figure below.

DKS1113 Electric Circuits

04/09/23 10/43

Ohm’s Law

Example 2: Calculate current i in figure below when the switch

is in position 1. Find the current when the switch is in position 2.

DKS1113 Electric Circuits

04/09/23 11/43

Nodes, Branches & Loops

Elements of electric circuits can be interconnected in several way.

Need to understand some basic concepts of network topology.

Branch: Represents a single element (i.e. voltage, resistor & etc)

Node: The meeting point between two or more branches.

Loop:Any closed path in a circuit.DKS1113 Electric Circuits

04/09/23 12/43

Nodes, Branches & Loops

Example 3: Determine how many branches and nodes for the

following circuit.

DKS1113 Electric Circuits

Nodes, Branches & Loops

5 Branches 1 Voltage Source 1 Current Source 3 Resistors

3 Nodes a b c

04/09/23 13/43

DKS1113 Electric Circuits

04/09/23 14/43

Nodes, Branches & Loops

Example 4: Determine how many branches and nodes for the

following circuit.

DKS1113 Electric Circuits

04/09/23 15/43

Kirchoff’s Laws

DKS1113 Electric Circuits

04/09/23 16/43

Kirchoff’s Laws

Kirchoff’s Current Law (KCL)

The algebraic sum of current entering / leaving a node (or closed boundary) is zero.

Current enters = +ve

Current leaves = -ve

∑ current entering = ∑ current leaving

DKS1113 Electric Circuits

04/09/23 17/43

Kirchoff’s Laws

Example 5: Given the following circuit, write the equation for

currents.

DKS1113 Electric Circuits

04/09/23 18/43

Kirchoff’s Laws

Example 6: Current in a closed boundary

DKS1113 Electric Circuits

04/09/23 19/43

Kirchoff’s Laws

Example 9: Use KCL to obtain currents i1, i2, and i3 in the circuit.

DKS1113 Electric Circuits

04/09/23 20/43

Kirchoff’s Laws

Kirchoff’s Voltage Law (KVL)

Applied to a loop in a circuit.

According to KVL The algebraic sum of voltage (rises and drops) in a loop is zero.

+

-

+ v1 -

- v3 +

+

V2

-

vs

DKS1113 Electric Circuits

04/09/23 21/43

Kirchoff’s Laws

Example 10: Use KVL to obtain v1, v2 and v3.

DKS1113 Electric Circuits

04/09/23 22/43

Kirchoff’s Laws

Example 11: Use KVL to obtain v1, and v2.

DKS1113 Electric Circuits

04/09/23 23/43

Kirchoff’s Laws

Example 12: Calculate power dissipated in 5Ω resistor.

10

DKS1113 Electric Circuits

04/09/23 24/43

Series Resistors & Voltage Division

Series resistors same current flowing through them.

v1= iR1 & v2 = iR2

KVL: v-v1-v2=0 v= i(R1+R2) i = v/(R1+R2 ) =v/Req

or v= i(R1+R2 ) =iReq iReq = R1+R2

DKS1113 Electric Circuits

04/09/23 25/43

Series Resistors & Voltage Division

Voltage Division:

Previously: v1 = iR1 & v2 = iR2 i = v/(R1+R2 )

Thus: v1=vR1/(R1+R2) v2=vR2/(R1+R2)

DKS1113 Electric Circuits

04/09/23 26/43

Parallel Resistors & Current Division

Parallel resistors Common voltage across it.

v = i1R1 = i2R2

i = i1+ i2

= v/R1+ v/R2

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

v =iReq

1/Req = 1/R1+1/R2

Req = R1R2 / (R1+R2 )

DKS1113 Electric Circuits

04/09/23 27/43

Parallel Resistors & Current Division

Current Division:

Previously: v = i1R1 = i2R2

v=iReq = iR1R2 / (R1+R2 ) and i1 = v /R1 & i2 =v/ R2

Thus: i1= iR2/(R1+R2) i2= iR1/(R1+R2 )

DKS1113 Electric Circuits

04/09/23 28/43

Conductance (G)

Series conductance: 1/Geq = 1/G1 +1/G2+…

Parallel conductance: Geq = G1 +G2+…

DKS1113 Electric Circuits

04/09/23 29/43

Voltage and Current Division

Example 13: Calculate v1, i1, v2 and i2.

DKS1113 Electric Circuits

04/09/23 30/43

Voltage and Current Division

Example 14: Determine i1 through i4.

DKS1113 Electric Circuits

04/09/23 31/43

Voltage and Current Division

Example 15: Determine v and i.

Answer v = 3v, I = 6 A.

DKS1113 Electric Circuits

04/09/23 32/43

Voltage and Current Division

Example 16: Determine I1 and Vs if the current through 3Ω

resistor = 2A.

DKS1113 Electric Circuits

04/09/23 33/43

Voltage and Current Division

Example 17: Determine Rab.

DKS1113 Electric Circuits

04/09/23 34/43

Voltage and Current Division

Example 18: Determine vx and power absorbed by the 12Ω

resistor. Answer v = 2v, p = 1.92w.

DKS1113 Electric Circuits

04/09/23 35/43

Wye-Delta Transformations

Given the circuit, how to combine R1 through R6? Resistors are neither in series nor parallel…

Use wye-delta transformationsDKS1113 Electric Circuits

04/09/23 36/43

Wye-Delta Transformations

Y network T network

DKS1113 Electric Circuits

04/09/23 37/43

Wye-Delta Transformations

Δ network π network

DKS1113 Electric Circuits

04/09/23 38/43

Wye-Delta Transformations

Delta (Δ) to wye (y) conversion.

DKS1113 Electric Circuits

04/09/23 39/43

Wye-Delta Transformations

Thus Δ to y conversion ::

R1 = RbRc/(Ra+Rb+Rc)

R2 = RaRc/(Ra+Rb+Rc)

R3 = RaRb/(Ra+Rb+Rc)

# Each resistors in y network is the product of two adjacent branches divide by the 3 Δ resistors

DKS1113 Electric Circuits

04/09/23 40/43

Wye-Delta Transformations

Y to Δ conversions:

Ra = (R1R2 +R2 R3 +R1R3)/R1

Rb = (R1R2 +R2 R3 +R1R3)/R2

Rc= (R1R2 +R2 R3 +R1R3)/R3

DKS1113 Electric Circuits

04/09/23 41/43

Wye-Delta Transformations

Example 19: Transform the circuit from Δ to y. Answer R1=18, R2=6, R3=3.

DKS1113 Electric Circuits

04/09/23 42/43

Wye-Delta Transformations

Example 20: Determine Rab. Answer Rab=142.32.

DKS1113 Electric Circuits

04/09/23 43/43

Wye-Delta Transformations

Example 21: Determine Io.

DKS1113 Electric Circuits

Recommended