Top Banner
Chapter 6 – Parallel Circuits Introductory Circuit Analysis Robert L. Boylestad
23

Chapter 6 – Parallel Circuits Introductory Circuit Analysis Robert L. Boylestad.

Mar 29, 2015

Download

Documents

Ethan Hess
Welcome message from author
This document is posted to help you gain knowledge. Please leave a comment to let me know what you think about it! Share it to your friends and learn new things together.
Transcript
Page 1: Chapter 6 – Parallel Circuits Introductory Circuit Analysis Robert L. Boylestad.

Chapter 6 – Parallel Circuits

Introductory Circuit AnalysisRobert L. Boylestad

Page 2: Chapter 6 – Parallel Circuits Introductory Circuit Analysis Robert L. Boylestad.

6.1 - Introduction

There are two network configurations – series and parallel

In Chapter 5 we covered a series network, and in this chapter we will cover the parallel circuit and all the methods and laws associated with it

Page 3: Chapter 6 – Parallel Circuits Introductory Circuit Analysis Robert L. Boylestad.

6.2 - Parallel Elements

Two elements, branches, or networks are in parallel if they have two points in common as in the figure below

Insert Fig 6.2Insert Fig 6.2

Page 4: Chapter 6 – Parallel Circuits Introductory Circuit Analysis Robert L. Boylestad.

6.3 - Total Conductance and Resistance

For parallel elements, the total conductance is the sum of the individual conductances.

GT = + G1 + G2 + G3 +… + Gn As the number of resistors in parallel increases, the

input current level will increase for the same applied voltage

This is the opposite effect of increasing the number of resistors in a series circuit

Page 5: Chapter 6 – Parallel Circuits Introductory Circuit Analysis Robert L. Boylestad.

Total Conductance and Resistance

Since G = 1/R the total resistance for a network can be determined by the equation below

Note that the equation is for 1 divided by the total resistance rather than the total resistance

Once the right side of the equation has been determined, it is necessary to divide the result into 1 to determine the total resistance

Page 6: Chapter 6 – Parallel Circuits Introductory Circuit Analysis Robert L. Boylestad.

Total Conductance and Resistance

The total resistance of a parallel resistor is always less than the value of the smallest resistor

Additionally, the wider the spread in numerical value between two parallel resistors, the closer the total resistance will be to the smaller resistor

The equation becomes significantly easier to apply for equal resistors in parallel

Total resistance of N parallel resistors of equal value is the resistance of one resistor divided by the number (N) of parallel elements

Page 7: Chapter 6 – Parallel Circuits Introductory Circuit Analysis Robert L. Boylestad.

Total Conductance and Resistance

The total resistance of two resistors is the product of the two divided by their sum

The equation was developed to reduce the effects of the inverse relationship when determining RT

Page 8: Chapter 6 – Parallel Circuits Introductory Circuit Analysis Robert L. Boylestad.

Total Conductance and Resistance

Parallel elements can be interchanged without changing the total resistance or input current

For parallel resistors, the total resistance will always decrease as additional elements are added in parallel

Page 9: Chapter 6 – Parallel Circuits Introductory Circuit Analysis Robert L. Boylestad.

6.4 - Parallel Circuits Total resistance is determined by RT = R1 R2 / (R1 + R2 )

and the source current by Is = E / RT . The subscript s will be used to denote a property of the

source The voltage across parallel elements is the same

V1 = V2 = E Voltage across resistor 1 is equal to the voltage across

resistor 2

Page 10: Chapter 6 – Parallel Circuits Introductory Circuit Analysis Robert L. Boylestad.

Parallel Circuits For single-source parallel networks, the source

current (Is) is equal to the sum of the individual branch currents

Is = I1 + I2

Page 11: Chapter 6 – Parallel Circuits Introductory Circuit Analysis Robert L. Boylestad.

6.5 - Kirchhoff’s Current Law

Kirchhoff’s voltage law provides an important relationship among voltage levels around any closed loop of a network

Now consider Kirchhoff’s current law (KCL) Kirchhoff’s current law states that the algebraic sum of the

currents entering and leaving an area, system, or junction is zero The sum of the current entering an area, system or junction

must equal the sum of the current leaving the area, system, or junction

Ientering = Ileaving

Page 12: Chapter 6 – Parallel Circuits Introductory Circuit Analysis Robert L. Boylestad.

Kirchhoff’s Current Law Most common application of the law will be at the junction

of two or more paths of current flow Determining whether a current is entering or leaving a

junction is sometimes the most difficult task One approach to understanding the flow is to picture

yourself as standing on the junction point and treating the path currents as arrows

If the arrow appears to be heading toward you, the current is entering the junction

If you see the tail of the arrow as it travels down its path away from you, the current is leaving the junction

Page 13: Chapter 6 – Parallel Circuits Introductory Circuit Analysis Robert L. Boylestad.

6.6 - Current Divider Rule The current divider rule (CDR) will determine how

the current entering a set of parallel branches will split between the elements

For two parallel elements of equal value, the current will divide equally

For parallel elements with different values, the smaller the resistance, the greater the share of input current

For parallel elements of different values, the current will split with a ratio equal to the inverse of their resistor values

Page 14: Chapter 6 – Parallel Circuits Introductory Circuit Analysis Robert L. Boylestad.

Current Divider Rule

Current seeks the path of least resistanceThe current entering any number of parallel resistors divides

into these resistors as the inverse ratio of their ohmic value

Page 15: Chapter 6 – Parallel Circuits Introductory Circuit Analysis Robert L. Boylestad.

Voltage sources are placed in parallel only if they have the same voltage rating

The purpose for placing two or more batteries in parallel would be to increase the current rating

The formula to determine the total current is:

Is = I1 + I2 +… INat the same terminal voltage

6.7 - Voltage Sources in Parallel

Page 16: Chapter 6 – Parallel Circuits Introductory Circuit Analysis Robert L. Boylestad.

Voltage Sources in Parallel

Two batteries of different terminal voltages placed in parallel

When two batteries of different terminal voltages are placed in parallel, the larger battery tries to drop rapidly to the lower supply

The result is the larger battery quickly discharges to the lower voltage battery, causing the damage to both batteries

Page 17: Chapter 6 – Parallel Circuits Introductory Circuit Analysis Robert L. Boylestad.

6.8 - Open and Short Circuits

An open circuit can have a potential difference (voltage) across its terminal, but the current is always zero amperes

Two isolated terminals not connected by any element:

Page 18: Chapter 6 – Parallel Circuits Introductory Circuit Analysis Robert L. Boylestad.

Open and Short Circuits

A short circuit can carry a current of a level determined by the external circuit, but the potential difference (voltage) across its terminals is always zero volts

Insert Fig 6.44Insert Fig 6.44

Page 19: Chapter 6 – Parallel Circuits Introductory Circuit Analysis Robert L. Boylestad.

6.9 - Voltmeters: Loading Effect

Voltmeters are always placed across an element to measure the potential difference

The resistance of two parallel resistors will always be less than the resistance of the smallest resistor

A DMM has internal resistance which will alter, somewhat, the network being measured

The loading of a network by the insertion a meter is not to be taken lightly, especially if accuracy is a primary consideration

Page 20: Chapter 6 – Parallel Circuits Introductory Circuit Analysis Robert L. Boylestad.

Voltmeters: Loading Effect

A good practice is to always check the meter resistance level against the resistive elements of the network before making a measurement

Most DMMs have internal resistance levels in excess of 10 MW on all voltage scales

Internal resistance of VOMs is sensitive to the scale chosen Internal resistance is determined by multiplying the maximum

voltage of the scale setting by the ohm/volt ( / V) rating of the meter, normally found at the bottom of the face of the meter

Page 21: Chapter 6 – Parallel Circuits Introductory Circuit Analysis Robert L. Boylestad.

6.10 - Troubleshooting Techniques

Troubleshooting is a process by which acquired knowledge and experience are employed to localize a problem and offer or implement a solution

Experience and a clear understanding of the basic laws of electrical circuits is vital

First step should always be knowing what to expect

Page 22: Chapter 6 – Parallel Circuits Introductory Circuit Analysis Robert L. Boylestad.

6.11 - Applications

Car system The electrical system on a car is essentially a

parallel system Parallel computer bus connections

The bus connectors are connected in parallel with common connections to the power supply, address and data buses, control signals, and ground

Page 23: Chapter 6 – Parallel Circuits Introductory Circuit Analysis Robert L. Boylestad.

Applications

House wiring Except in some very special circumstances the basic

wiring of a house is done in a parallel configuration Each parallel branch, however, can have a

combination of parallel and series elements Each branch receives a full 120 V or 208 V, with the

current determined by the applied load