1 chapter 3 resistance ecet 1010 fundamentals. 2 3.1 resistance opposing force – due to collisions...
TRANSCRIPT
![Page 1: 1 Chapter 3 Resistance ECET 1010 Fundamentals. 2 3.1 Resistance Opposing force – due to collisions between electrons and between electrons and other atoms](https://reader034.vdocuments.site/reader034/viewer/2022052509/56649d945503460f94a7c07f/html5/thumbnails/1.jpg)
1
Chapter 3Resistance
ECET 1010 Fundamentals
![Page 2: 1 Chapter 3 Resistance ECET 1010 Fundamentals. 2 3.1 Resistance Opposing force – due to collisions between electrons and between electrons and other atoms](https://reader034.vdocuments.site/reader034/viewer/2022052509/56649d945503460f94a7c07f/html5/thumbnails/2.jpg)
2
3.1 Resistance Opposing force – due to collisions
between electrons and between electrons and other atoms
Converts electrical energy into another form of energy such as heat
![Page 3: 1 Chapter 3 Resistance ECET 1010 Fundamentals. 2 3.1 Resistance Opposing force – due to collisions between electrons and between electrons and other atoms](https://reader034.vdocuments.site/reader034/viewer/2022052509/56649d945503460f94a7c07f/html5/thumbnails/3.jpg)
3
Resistance Determined by
the following four factors Material Length Cross-sectional
area Temperature
R = ρ l / A
![Page 4: 1 Chapter 3 Resistance ECET 1010 Fundamentals. 2 3.1 Resistance Opposing force – due to collisions between electrons and between electrons and other atoms](https://reader034.vdocuments.site/reader034/viewer/2022052509/56649d945503460f94a7c07f/html5/thumbnails/4.jpg)
4
3.2 Resistance: Circular Wires The higher the resistivity, the more
the resistance The longer the length of the
conductor, the more the resistance The smaller the area of the
conductor, the more the resistance The higher the temperature of the
conductor, the more the resistance
![Page 5: 1 Chapter 3 Resistance ECET 1010 Fundamentals. 2 3.1 Resistance Opposing force – due to collisions between electrons and between electrons and other atoms](https://reader034.vdocuments.site/reader034/viewer/2022052509/56649d945503460f94a7c07f/html5/thumbnails/5.jpg)
5
Area of Circular Wires The area of the conductor is
measured in circular mils (CM) 1 mil is one one-thousandth of an
inch A wire with a diameter of 1 mil has
an area of 1 circular mil (CM) Area of Circle = π r2 = π d2 / 4
![Page 6: 1 Chapter 3 Resistance ECET 1010 Fundamentals. 2 3.1 Resistance Opposing force – due to collisions between electrons and between electrons and other atoms](https://reader034.vdocuments.site/reader034/viewer/2022052509/56649d945503460f94a7c07f/html5/thumbnails/6.jpg)
6
Area of Circular Wires Relationship between circular mils
(CM) and square mils 1 CM = π / 4 sq. mils
Relationship between area in circular mils (CM) and diameter in mils ACM = (dmils)2
![Page 7: 1 Chapter 3 Resistance ECET 1010 Fundamentals. 2 3.1 Resistance Opposing force – due to collisions between electrons and between electrons and other atoms](https://reader034.vdocuments.site/reader034/viewer/2022052509/56649d945503460f94a7c07f/html5/thumbnails/7.jpg)
7
Example 3.1What is the resistance of a 100-ft length
of copper wire with a diameter of 0.020 in. at 20°C?
l = 100 ftρ = 10.37 CM-Ω/ft (Table 3.1)d = 0.020 in = 20 milsA = d2 CM = 400 CMR = 10.37 * 100 / 400 = 2.59 Ω
![Page 8: 1 Chapter 3 Resistance ECET 1010 Fundamentals. 2 3.1 Resistance Opposing force – due to collisions between electrons and between electrons and other atoms](https://reader034.vdocuments.site/reader034/viewer/2022052509/56649d945503460f94a7c07f/html5/thumbnails/8.jpg)
8
Example 3.2You have been given a carton of wire where
an undetermined number of feet of the wire has been used. Find the length of the remaining copper wire if it has a diameter of 1/16 in. and a resistance of 0.5 Ω.
ρ = 10.37 CM-Ω/ftd = 1/16 in = 62.5 milsA = (62.5)2 CM = 3906.25 CMR = 0.5 Ωl = 3906.25 * 0.5 / 10.37 = 188.34 ft
![Page 9: 1 Chapter 3 Resistance ECET 1010 Fundamentals. 2 3.1 Resistance Opposing force – due to collisions between electrons and between electrons and other atoms](https://reader034.vdocuments.site/reader034/viewer/2022052509/56649d945503460f94a7c07f/html5/thumbnails/9.jpg)
9
Example 3.3What is the resistance of a copper bus-bar
(as used in the power distribution panel of a high-rise office building) 3 ft long, 5 in. wide, and 0.5 in. thick?
l = 3 ftρ = 10.37 CM-Ω/ftA = ½ in * 5 in = 500 mil * 5,000 mil = 2.5 * 106
mil2
ACM = 2.5 * 106 * (4/ π) = 3.183 * 106 CMR = 10.37 * 3 / 3.183 * 106 = 9.773 * 10-6 Ω
![Page 10: 1 Chapter 3 Resistance ECET 1010 Fundamentals. 2 3.1 Resistance Opposing force – due to collisions between electrons and between electrons and other atoms](https://reader034.vdocuments.site/reader034/viewer/2022052509/56649d945503460f94a7c07f/html5/thumbnails/10.jpg)
10
3.3 Wire Tables Standardize the size of wire produced
by manufacturers throughout the United States
See Table 3.2 – American Wire Gage (AWG) sizes AWG number Area in circular mils Resistance in Ω per 1,000 feet at 20°C Maximum allowable current
![Page 11: 1 Chapter 3 Resistance ECET 1010 Fundamentals. 2 3.1 Resistance Opposing force – due to collisions between electrons and between electrons and other atoms](https://reader034.vdocuments.site/reader034/viewer/2022052509/56649d945503460f94a7c07f/html5/thumbnails/11.jpg)
11
Example 3.4
Find the resistance of 650 ft of #8 copper wire (T = 20°C).
from Table 3.20.6282 Ω / 1,000 ft
R = 650 ft * (0.6282 Ω / 1,000 ft)= 0.408 Ω
![Page 12: 1 Chapter 3 Resistance ECET 1010 Fundamentals. 2 3.1 Resistance Opposing force – due to collisions between electrons and between electrons and other atoms](https://reader034.vdocuments.site/reader034/viewer/2022052509/56649d945503460f94a7c07f/html5/thumbnails/12.jpg)
12
Example 3.5
What is the diameter, in inches, of #12 copper wire?
from Table 3.2ACM = 6529 CM = (dmils)2
d = 80.8 mil = 0.0808 in ~ 1/12 in
![Page 13: 1 Chapter 3 Resistance ECET 1010 Fundamentals. 2 3.1 Resistance Opposing force – due to collisions between electrons and between electrons and other atoms](https://reader034.vdocuments.site/reader034/viewer/2022052509/56649d945503460f94a7c07f/html5/thumbnails/13.jpg)
13
Example 3.6
For the following system, the total resistance of each power line cannot be more than 0.025 Ω, and the maximum current to be drawn by the load is 95 A. What gage wire should be used?
Need a picture of an input connected to a load by two 100 ft lengths of solid round copper.
![Page 14: 1 Chapter 3 Resistance ECET 1010 Fundamentals. 2 3.1 Resistance Opposing force – due to collisions between electrons and between electrons and other atoms](https://reader034.vdocuments.site/reader034/viewer/2022052509/56649d945503460f94a7c07f/html5/thumbnails/14.jpg)
14
Example 3.6 (continued)From Table 3.2 we choose #3 wire since
its maximum allowable current is 100 A and this is greater than 95 A
We need to check and make sure 100 ft of #3 wire is NOT more than 0.025 Ω
R = 100 ft * (0.1970 Ω / 1,000 ft)= 0.01970 Ω ‹ 0.025 Ω
![Page 15: 1 Chapter 3 Resistance ECET 1010 Fundamentals. 2 3.1 Resistance Opposing force – due to collisions between electrons and between electrons and other atoms](https://reader034.vdocuments.site/reader034/viewer/2022052509/56649d945503460f94a7c07f/html5/thumbnails/15.jpg)
15
3.5 Temperature Effects Temperature has a significant
effect on the resistance of Conductors Semiconductors Insulators
![Page 16: 1 Chapter 3 Resistance ECET 1010 Fundamentals. 2 3.1 Resistance Opposing force – due to collisions between electrons and between electrons and other atoms](https://reader034.vdocuments.site/reader034/viewer/2022052509/56649d945503460f94a7c07f/html5/thumbnails/16.jpg)
16
Conductors For good conductors, an increase
in temperature will result in an increase in the resistance level (due to an increase in the random motion of the particles in the material). Consequently, conductors have a positive temperature coefficient.
![Page 17: 1 Chapter 3 Resistance ECET 1010 Fundamentals. 2 3.1 Resistance Opposing force – due to collisions between electrons and between electrons and other atoms](https://reader034.vdocuments.site/reader034/viewer/2022052509/56649d945503460f94a7c07f/html5/thumbnails/17.jpg)
17
Semiconductors For semiconductor materials, an
increase in temperature will result in a decrease in the resistance level (due to an increase in free carriers). Consequently, semiconductors have a negative temperature coefficient.
![Page 18: 1 Chapter 3 Resistance ECET 1010 Fundamentals. 2 3.1 Resistance Opposing force – due to collisions between electrons and between electrons and other atoms](https://reader034.vdocuments.site/reader034/viewer/2022052509/56649d945503460f94a7c07f/html5/thumbnails/18.jpg)
18
Insulators As with semiconductors, an
increase in temperature will result in a decrease in the resistance of an insulator. The result is a negative temperature coefficient.
![Page 19: 1 Chapter 3 Resistance ECET 1010 Fundamentals. 2 3.1 Resistance Opposing force – due to collisions between electrons and between electrons and other atoms](https://reader034.vdocuments.site/reader034/viewer/2022052509/56649d945503460f94a7c07f/html5/thumbnails/19.jpg)
19
Inferred Absolute Temperature Effect of temperature on the resistance of
copper R1,t1 and R2,t2
-234.5 °C Similar triangles yield
(234.5 + t1) / R1 = (234.5 + t2) / R2
Adapting to any material ( |T| + t1) / R1 = ( |T| + t2) / R2
![Page 20: 1 Chapter 3 Resistance ECET 1010 Fundamentals. 2 3.1 Resistance Opposing force – due to collisions between electrons and between electrons and other atoms](https://reader034.vdocuments.site/reader034/viewer/2022052509/56649d945503460f94a7c07f/html5/thumbnails/20.jpg)
20
Inferred Absolute Temperatures
Material °C α20
Silver -243 0.0038
Copper -234.5 0.00393
Gold -274 0.0034
Aluminum -236 0.00391
Tungsten -204 0.005
Nickel -147 0.006
Iron -162 0.0055
Nichrome -2,250 0.00044
Constantan -125,000 0.000008
![Page 21: 1 Chapter 3 Resistance ECET 1010 Fundamentals. 2 3.1 Resistance Opposing force – due to collisions between electrons and between electrons and other atoms](https://reader034.vdocuments.site/reader034/viewer/2022052509/56649d945503460f94a7c07f/html5/thumbnails/21.jpg)
21
Example 3.9
If the resistance of copper wire is 50 Ω at 20° C, what is its resistance at 100° C (boiling point of water)?
(234.5 + 20) / 50 Ω = (234.5 + 100) / R
R = 65.72 Ω
![Page 22: 1 Chapter 3 Resistance ECET 1010 Fundamentals. 2 3.1 Resistance Opposing force – due to collisions between electrons and between electrons and other atoms](https://reader034.vdocuments.site/reader034/viewer/2022052509/56649d945503460f94a7c07f/html5/thumbnails/22.jpg)
22
Example 3.10
If the resistance of copper wire at freezing (0° C) is 30 Ω, what is its resistance at -40° C?
(234.5 + 0) / 30 Ω = (234.5 - 40) / R
R = 24.88 Ω
![Page 23: 1 Chapter 3 Resistance ECET 1010 Fundamentals. 2 3.1 Resistance Opposing force – due to collisions between electrons and between electrons and other atoms](https://reader034.vdocuments.site/reader034/viewer/2022052509/56649d945503460f94a7c07f/html5/thumbnails/23.jpg)
23
Example 3.11
If the resistance of an aluminum wire at room temperature (20° C) is 100 mΩ (measured by a milliohmeter), at what temperature will its resistance increase to 120 mΩ?
(236 + 20) / 100 mΩ = (236 + t) / 120 mΩ
t = 71.2° C
![Page 24: 1 Chapter 3 Resistance ECET 1010 Fundamentals. 2 3.1 Resistance Opposing force – due to collisions between electrons and between electrons and other atoms](https://reader034.vdocuments.site/reader034/viewer/2022052509/56649d945503460f94a7c07f/html5/thumbnails/24.jpg)
24
Temperature Coefficient of Resistance Definition of temperature coefficient of
resistance at 20° C.
α20 = 1 / (|T| + 20° C)
For copper, α20 = 0.00393 Ω/° C/Ω
The higher the temperature coefficient of resistance for a material, the more sensitive the resistance level to changes in temperature.
![Page 25: 1 Chapter 3 Resistance ECET 1010 Fundamentals. 2 3.1 Resistance Opposing force – due to collisions between electrons and between electrons and other atoms](https://reader034.vdocuments.site/reader034/viewer/2022052509/56649d945503460f94a7c07f/html5/thumbnails/25.jpg)
25
Temperature Coefficient of Resistance Resistance R at a temperature t
given by:
R = R20 [1 + α20(t - 20° C)]
Which can be written as:
R = ρ (l/A) [1 + α20(ΔT)]
![Page 26: 1 Chapter 3 Resistance ECET 1010 Fundamentals. 2 3.1 Resistance Opposing force – due to collisions between electrons and between electrons and other atoms](https://reader034.vdocuments.site/reader034/viewer/2022052509/56649d945503460f94a7c07f/html5/thumbnails/26.jpg)
26
Example
If the nominal resistance of a copper wire is 5 Ω, what will its resistance be at 30 ° C?
R = 5 Ω [1 + 0.00393(30° C - 20° C)]
R = 5 Ω (1.0393) = 5.1965 Ω
![Page 27: 1 Chapter 3 Resistance ECET 1010 Fundamentals. 2 3.1 Resistance Opposing force – due to collisions between electrons and between electrons and other atoms](https://reader034.vdocuments.site/reader034/viewer/2022052509/56649d945503460f94a7c07f/html5/thumbnails/27.jpg)
27
PPM/°C Parts per million per degree Celsius For resistors
5000-PPM is high 20-PPM is low 1000-PPM/°C says a 1° C change in
temperature gives a change in resistance equal to 1000 parts per million or 1,000/1,000,1000 or 1/1,000 of its value.
ΔR = (Rnominal/106) (PPM) (ΔT)
![Page 28: 1 Chapter 3 Resistance ECET 1010 Fundamentals. 2 3.1 Resistance Opposing force – due to collisions between electrons and between electrons and other atoms](https://reader034.vdocuments.site/reader034/viewer/2022052509/56649d945503460f94a7c07f/html5/thumbnails/28.jpg)
28
Example 3.12For a 1-kΩ carbon composition resistor
with a PPM of 2500, determine the resistance at 60°C.
Rnominal = 1,000 ΩPPM = 2,500ΔT = t – 20° C = 60° C – 20° C = 40° CΔR = (1,000/106) (2,500) (40) = 100 Ω
R = Rnominal + ΔR = 1,100 Ω
![Page 29: 1 Chapter 3 Resistance ECET 1010 Fundamentals. 2 3.1 Resistance Opposing force – due to collisions between electrons and between electrons and other atoms](https://reader034.vdocuments.site/reader034/viewer/2022052509/56649d945503460f94a7c07f/html5/thumbnails/29.jpg)
29
3.8 Color Coding and Standard Resistor Values See Table 3.7 Way to identify
Resistance Tolerance Reliability
![Page 30: 1 Chapter 3 Resistance ECET 1010 Fundamentals. 2 3.1 Resistance Opposing force – due to collisions between electrons and between electrons and other atoms](https://reader034.vdocuments.site/reader034/viewer/2022052509/56649d945503460f94a7c07f/html5/thumbnails/30.jpg)
30
Color Code TableColor Band 1 Band 2 Band 3 Band 4 Band 5
Silver 10-2 10%
Gold 10-1 5%
Black 0 100
Brown 1 1 101 1% 1%
Red 2 2 102 2% 0.1%
Orange 3 3 103 3% 0.01%
Yellow 4 4 104 4% 0.001%
Green 5 5 105
Blue 6 6 106
Violet 7 7 107
Gray 8 8 108
White 9 9 109
None 20%
![Page 31: 1 Chapter 3 Resistance ECET 1010 Fundamentals. 2 3.1 Resistance Opposing force – due to collisions between electrons and between electrons and other atoms](https://reader034.vdocuments.site/reader034/viewer/2022052509/56649d945503460f94a7c07f/html5/thumbnails/31.jpg)
31
Bands First and second band give first two
digits Third band gives power-of-ten
multiplier Fourth band gives tolerance, ±percent Fifth band gives reliability, failures per
1,000 hours use See Table 3.8 for standard resistor
values
![Page 32: 1 Chapter 3 Resistance ECET 1010 Fundamentals. 2 3.1 Resistance Opposing force – due to collisions between electrons and between electrons and other atoms](https://reader034.vdocuments.site/reader034/viewer/2022052509/56649d945503460f94a7c07f/html5/thumbnails/32.jpg)
Standard Resistor Values
![Page 33: 1 Chapter 3 Resistance ECET 1010 Fundamentals. 2 3.1 Resistance Opposing force – due to collisions between electrons and between electrons and other atoms](https://reader034.vdocuments.site/reader034/viewer/2022052509/56649d945503460f94a7c07f/html5/thumbnails/33.jpg)
33
Example 3.13aFind the range in which a resistor having the
following color bands must exist to satisfy the manufacturer’s tolerance:
Gray, Red, Black, Gold, Brown
8 2 0 5% 1%
82 * 100 ± 5% Ω
77.9 – 86.1 Ω
![Page 34: 1 Chapter 3 Resistance ECET 1010 Fundamentals. 2 3.1 Resistance Opposing force – due to collisions between electrons and between electrons and other atoms](https://reader034.vdocuments.site/reader034/viewer/2022052509/56649d945503460f94a7c07f/html5/thumbnails/34.jpg)
34
Example 3.13bFind the range in which a resistor having the
following color bands must exist to satisfy the manufacturer’s tolerance:
Orange, White, Gold, Silver, No Color
3 9 -1 10%
39 * 10-1 ± 10% Ω
3.51 – 4.29 Ω
![Page 35: 1 Chapter 3 Resistance ECET 1010 Fundamentals. 2 3.1 Resistance Opposing force – due to collisions between electrons and between electrons and other atoms](https://reader034.vdocuments.site/reader034/viewer/2022052509/56649d945503460f94a7c07f/html5/thumbnails/35.jpg)
35
Conductance Reciprocal of resistance
G = 1 / R (Siemens, S)
As a function of area, length, and resistivity
G = A / (ρl)
![Page 36: 1 Chapter 3 Resistance ECET 1010 Fundamentals. 2 3.1 Resistance Opposing force – due to collisions between electrons and between electrons and other atoms](https://reader034.vdocuments.site/reader034/viewer/2022052509/56649d945503460f94a7c07f/html5/thumbnails/36.jpg)
36
Example 3.14What is the relative increase or decrease in
conductivity of a conductor if the area is reduced by 30% and the length is increased by 40%? (The resistivity is fixed.)
Gi = Ai / (ρili)
Gr = Ar / (ρrlr) = 0.7 Ai / (ρi (1.4) li)
= (0.7/1.4) Ai / (ρili) = 0.5 Gi
![Page 37: 1 Chapter 3 Resistance ECET 1010 Fundamentals. 2 3.1 Resistance Opposing force – due to collisions between electrons and between electrons and other atoms](https://reader034.vdocuments.site/reader034/viewer/2022052509/56649d945503460f94a7c07f/html5/thumbnails/37.jpg)
Fixed Composition Resistors of Different Wattage Ratings
![Page 38: 1 Chapter 3 Resistance ECET 1010 Fundamentals. 2 3.1 Resistance Opposing force – due to collisions between electrons and between electrons and other atoms](https://reader034.vdocuments.site/reader034/viewer/2022052509/56649d945503460f94a7c07f/html5/thumbnails/38.jpg)
Measuring the Resistance of a Single Element