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PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

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Page 1: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 1

Resistors

Ohm’s Law and Combinations of Resistors

See Chapters 1 & 2 in

Electronics: The Easy Way

(Miller & Miller)

Page 2: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 2

Electric Charge

Electric charge is a fundamental property of some of the particles that make up matter, especially (but not only) electrons and protons.

Charge comes in two varieties: Positive (protons have positive charge) Negative (electrons have negative charge)

Charge is measured in units called Coulombs. A Coulomb is a rather large amount of charge. A proton has a charge 1.602 10-19 C.

Page 3: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 3

ESD

A small amount of charge can build up on one’s body – you especially notice it on winter days in carpeted rooms when it’s easy to build a charge and get or give a shock.

A shock is an example of electrostatic discharge (ESD) – the rapid movement of charge from a place where it was stored.

One must be careful of ESD when repairing a computer, since ESD can damage electronic components.

Page 4: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 4

Current

If charges are moving, there is a current. Current is rate of charge flowing by, that is, the

amount of charge going by a point each second. It is measured in units called amperes (amps) which

are Coulombs per second (A=C/s) The currents in computers are usually measured in

milliamps (1 mA = 0.001 A).

Currents are measured by ammeters.

Page 5: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 5

Ammeter in Multisim Electronics WorkBench

Ammeters are connected in series. Think of the charge as starting at the side of the battery with the long end and heading toward the side with the short end. If all of the charges passing through the first object (the resistor above ) must also pass through second object (the ammeter above), then the two objects are said to be in

series.

Page 6: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 6

Current Convention

Current has a direction. By convention the direction of the current is the direction in

which positive charge flows. The book is a little unconventional on this point.

If negative charges are flowing (which is often the case), the current’s direction is opposite to the particle’s direction.

(Blame Benjamin Franklin.)

Ie-

e-

e-

Negative charges moving to leftCurrent moving to right

Page 7: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 7

Potential Energy and Work

Potential energy is the ability to due work, such as lifting a weight.

Certain arrangements of charges, like that in a battery, have potential energy.

What’s important is the difference in potential energy between one arrangement and another.

Energy is measured in units called Joules.

Page 8: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 8

Voltage

With charge arrangements, the bigger the charges, the greater the energy.

It is convenient to define the potential energy per charge, known as the electric potential (or just potential).

The potential difference (a.k.a. the voltage) is the difference in potential energy per charge between two charge arrangements

Comes in volts (Joules per Coulomb, V=J/C). Measured by a voltmeter.

Page 9: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 9

Volt = Joule / Coulomb

=

Page 10: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 10

Voltmeter in Multisim EWB

Voltmeters are connected in parallel. If the “tops” of two objects are connected by wire and only wire and the same can be said for the “bottoms” , then the two objects are said to be in parallel.

Page 11: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 11

Voltage and Current

When a potential difference (voltage) such as that supplied by a battery is placed across a device, a common result is for a current to start flowing through the device.

Page 12: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 12

Resistance

The ratio of voltage to current is known as resistance

The resistance indicates whether it takes a lot of work (high resistance) or a little bit of work (low resistance) to move charges.

Comes in ohms (). Measured by ohmmeter.

R = V

I

Page 13: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 13

Multi-meter being used as ohmmeter in Multisim EWB

A resistor or combination of resistors is removed from a circuit before using an ohmmeter.

Page 14: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 14

Conductors and Insulators

It is easy to produce a current in a material with low resistance; such materials are called conductors. E.g. copper, gold, silver

It is difficult to produce a current in a material with high resistance; such materials are called insulators. E.g. glass, rubber, plastic

Page 15: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 15

Semiconductor

A semiconductor is a substance having a resistivity that falls between that of conductors and that of insulators. E.g. silicon, germanium

A process called doping can make them more like conductors or more like insulators This control plays a role in making diodes,

transistors, etc.

Page 16: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 16

Ohm’s Law

Ohm’s law says that the current produced by a voltage is directly proportional to that voltage. Doubling the voltage, doubles the current. Then, resistance is independent of voltage or

current

V

I Slope=I/V=1/R

Page 17: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 17

V = I R

=

Page 18: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 18

Ohmic

Ohm’s law is an empirical observation “Empirical” here means that it is something we

notice tends to be true, rather than something that must be true.

Ohm’s law is not always obeyed. For example, it is not true for diodes or transistors.

A device which does obey Ohm’s law is said to “ohmic.”

Page 19: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 19

Resistor

A resistor is an Ohmic device, the sole purpose of which is to provide resistance. By providing resistance, they lower voltage or

limit current

Page 20: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 20

Example

A light bulb has a resistance of 240 when lit. How much current will flow through it when it is connected across 120 V, its normal operating voltage?

V = I R 120 V = I (240 ) I = 0.5 V/ = 0.5 A

Page 21: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 21

Binary Numbers

Page 22: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 22

Why Binary?

Maximal distinction among values minimal corruption from noise

Imagine taking the same physical attribute of a circuit, e.g. a voltage lying between 0 and 5 volts, to represent a number

The overall range can be divided into any number of regions

Page 23: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 23

Don’t sweat the small stuff

For decimal numbers, fluctuations must be less than 0.25 volts

For binary numbers, fluctuations must be less than 1.25 volts

5 volts

0 voltsDecimal Binary

Page 24: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 24

Range actually split in three

High

Low

Forbidden range

Page 25: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 25

It doesn’t matter ….

Some of the standard voltages coming from a computer’s power are ideally supposed to be 3.30 volts, 5.00 volts and 12.00 volts

Typically they are 3.28 volts, 5.14 volts or 12.22 volts or some such value

So what, who cares

Page 26: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 26

How to represent big integers

Use positional weighting, same as with decimal numbers

205 = 2102 + 0101 + 5100

Decimal – powers of ten

11001101 = 127 + 126 + 025 + 024

+ 123 + 122 + 021 + 120 = 128 + 64 + 8 + 4 + 1 = 205 Binary – powers of two

Page 27: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 27

Converting 205 to Binary

205/2 = 102 with a remainder of 1, place the 1 in the least significant digit position

Repeat 102/2 = 51, remainder 01

0 1

Page 28: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 28

Iterate

51/2 = 25, remainder 1

25/2 = 12, remainder 1

12/2 = 6, remainder 0

1 0 1

1 1 0 1

0 1 1 0 1

Page 29: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 29

Iterate

6/2 = 3, remainder 0

3/2 = 1, remainder 1

1/2 = 0, remainder 1

0 0 1 1 0 1

1 0 0 1 1 0 1

1 1 0 0 1 1 0 1

Page 30: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 30

Recap

1 1 0 0 1 1 0 1

127 + 126 + 025 + 024

+ 123 + 122 + 021 + 120

205

Page 31: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 31

Finite representation

Typically we just think computers do binary math. But an important distinction between binary math

in the abstract and what computers do is that computers are finite.

There are only so many flip-flops or logic gates in the computer.

When we declare a variable, we set aside a certain number of flip-flops (bits of memory) to hold the value of the variable. And this limits the values the variable can have.

Page 32: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 32

Same number, different representation

5 using 8 bits 0000 0101 5 using 16 bits 0000 0000 0000 0101 5 using 32 bits 0000 0000 0000 0000 0000 0000 0000 0101

Page 33: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 33

Adding Binary Numbers

Same as decimal; if the sum of digits in a given position exceeds the base (10 for decimal, 2 for binary) then there is a carry into the next higher position

1

3 9

+ 3 5

7 4

Page 34: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 34

Adding Binary Numbers

1 1 1 1

0 1 0 0 1 1 1

+ 0 1 0 0 0 1 1

1 0 0 1 0 1 0

carries

Page 35: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 35

Uh oh, overflow*

What if you use a byte (8 bits) to represent an integer

A byte may not be enough to represent the sum of two such numbers.

*The End of the World as We Know It

1 1

1 0 1 0 1 0 1 0

+ 1 1 0 0 1 1 0 0

1 0 1 1 1 0 1 1 0

Page 36: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 36

Biggest unsigned integers

4 bit: 1111 15 = 24 - 1 8 bit: 11111111 255 = 28 – 1 16 bit: 1111111111111111 65535= 216 – 1 32 bit:

11111111111111111111111111111111 4294967295= 232 – 1

Etc.

Page 37: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 37

Bigger Numbers

You can represent larger numbers by using more words

You just have to keep track of the overflows to know how the lower numbers (less significant words) are affecting the larger numbers (more significant words)

Page 38: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 38

Negative numbers

Negative x is the number that when added to x gives zero

Ignoring overflow the two eight-bit numbers above sum to zero

1 1 1 1 1 1 1

0 0 1 0 1 0 1 0

1 1 0 1 0 1 1 0

1 0 0 0 0 0 0 0 0

Page 39: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 39

Two’s Complement

Step 1: exchange 1’s and 0’s

Step 2: add 1 (to the lowest bit only)

0 0 1 0 1 0 1 0

1 1 0 1 0 1 0 1

1 1 0 1 0 1 1 0

Page 40: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 40

Sign bit

With the two’s complement approach, all positive numbers start with a 0 in the left-most, most-significant bit and all negative numbers start with 1.

So the first bit is called the sign bit. But note you have to work harder than just

strip away the first bit. 10000001 IS NOT the 8-bit version of –1

Page 41: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 41

Add 1’s to the left to get the same negative number using more bits

-5 using 8 bits 11111011 -5 using 16 bits 1111111111111011 -5 using 32 bits 11111111111111111111111111111011 When the numbers represented are whole numbers

(positive or negative), they are called integers.

Page 42: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 42

Biggest signed integers

4 bit: 0111 7 = 23 - 1 8 bit: 01111111 127 = 27 – 1 16 bit: 0111111111111111 32767= 215 – 1 32 bit:

01111111111111111111111111111111 2147483647= 231 – 1

Etc.

Page 43: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 43

Most negative signed integers

4 bit: 1000 -8 = - 23

8 bit: 10000000 - 128 = - 27

16 bit: 1000000000000000 -32768= - 215

32 bit: 10000000000000000000000000000000 -2147483648= - 231

Etc.

Page 44: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 44

Riddle

Is it 214? Or is it – 42? Or is it Ö? Or is it …? It’s a matter of interpretation

How was it declared?

1 1 0 1 0 1 1 0

Page 45: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 45

3-bit unsigned and signed

7 1 1 1

6 1 1 0

5 1 0 1

4 1 0 0

3 0 1 1

2 0 1 0

1 0 0 1

0 0 0 0

3 0 1 1

2 0 1 0

1 0 0 1

0 0 0 0

-1 1 1 1

-2 1 1 0

-3 1 0 1

-4 1 0 0

Think of an odometer reading 999999 and the car travels one more mile.

Page 46: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 46

Fractions

Similar to what we’re used to with decimal numbers

3.14159 =

3 · 100 + 1 · 10-1 + 4 · 10-2 + 1 · 10-3 + 5 · 10-4 + 9 · 10-5

11.001001 =

1 · 21 + 1 · 20 + 0 · 2-1 + 0 · 2-2 + 1 · 2-3 + 0 · 2-4 + 0 · 2-5

+ 1 · 2-6

(11.001001

3.140625)

Page 47: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

Places

11.001001

PHY 201 (Blum) 47

Two’s placeOne’s place

Half’s place

Fourth’s place Eighth’s

place Sixteenth’s place

Page 48: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 48

Decimal to binary

98.61 Integer part

98 / 2 = 49 remainder 0 49 / 2 = 24 remainder 1 24 / 2 = 12 remainder 0 12 / 2 = 6 remainder 0 6 / 2 = 3 remainder 0 3 / 2 = 1 remainder 1 1 / 2 = 0 remainder 1

1100010

Page 49: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 49

Decimal to binary

98.61 Fractional part

0.61 2 = 1.22 0.22 2 = 0.44 0.44 2 = 0.88 0.88 2 = 1.76 0.76 2 = 1.52 0.52 2 = 1.04

.100111

Page 50: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 50

Decimal to binary

Put together the integral and fractional parts 98.61 1100010.100111

Page 51: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 51

Another Example (Whole number part)

123.456 Integer part

123 / 2 = 61 remainder 1 61 / 2 = 30 remainder 1 30 / 2 = 15 remainder 0 15 / 2 = 7 remainder 1 7 / 2 = 3 remainder 1 3 / 2 = 1 remainder 1 1 / 2 = 0 remainder 1

1111011.

Page 52: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 52

Checking: Go to All Programs/Accessories/Calculator

Page 53: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 53

Put the calculator in Programmer view

Page 54: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 54

Enter number, put into binary mode

Page 55: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 55

Another Example (fractional part)

123.456 Fractional part

0.456 2 = 0.912 0.912 2 = 1.824 0.824 2 = 1.648 0.648 2 = 1.296 0.296 2 = 0.592 0.592 2 = 1.184 0.184 2 = 0.368 …

.0111010…

Page 56: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 56

Checking fractional part: Enter digits found in binary mode

Note that the leading zero does not display.

Page 57: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 57

Convert to decimal mode, then

Page 58: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

Edit/Copy result. Switch to Scientific View. Edit/Paste

PHY 201 (Blum) 58

Page 59: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 59

Divide by 2 raised to the number of digits (in this case 7, including leading zero)

1 2

3 4

Page 60: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 60

Finally hit the equal sign. In most cases it will not be exact

Page 61: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 61

Other way around

Multiply fraction by 2 raised to the desired number of digits in the fractional part. For example .456 27 = 58.368

Throw away the fractional part and represent the whole number 58 111010

But note that we specified 7 digits and the result above uses only 6. Therefore we need to put in the leading 0. (Also the fraction is less than .5 so there’s a zero in the ½’s place.) 0111010

Page 62: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 62

Limits of the fixed point approach

Suppose you use 4 bits for the whole number part and 4 bits for the fractional part (ignoring sign for now).

The largest number would be 1111.1111 = 15.9375

The smallest, non-zero number would be 0000.0001 = .0625

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PHY 201 (Blum) 63

Floating point representation

Floating point representation allows one to represent a wider range of numbers using the same number of bits.

It is like scientific notation. We’ll do this later in the semester.

Page 64: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 64

Hexadecimal Numbers

Even moderately sized decimal numbers end up as long strings in binary

Hexadecimal numbers (base 16) are often used because the strings are shorter and the conversion to binary is easier

There are 16 digits: 0-9 and A-F

Page 65: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 65

Decimal Binary Hex

0 0000 0 1 0001 1 2 0010 2 3 0011 3 4 0100 4 5 0101 5 6 0110 6 7 0111 7

8 1000 8 9 1001 9 10 1010 A 11 1011 B 12 1100 C 13 1101 D 14 1110 E 15 1111 F

Page 66: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

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Binary to Hex

Break a binary string into groups of four bits (nibbles)

Convert each nibble separately

1 1 1 0 1 1 0 0 1 0 0 1

E C 9

Page 67: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

Digit grouping and Hex mode

PHY 201 (Blum) 67

Page 68: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

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Addresses

With user friendly computers, one rarely encounters binary, but we sometimes see hex, especially with addresses

To enable the computer to distinguish various parts, each is assigned an address, a number Distinguish among computers on a network Distinguish keyboard and mouse Distinguish among files Distinguish among statements in a program Distinguish among characters in a string

Page 69: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

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How many?

One bit can have two states and thus distinguish between two things

Two bits can be in four states and … Three bits can be in eight states, … N bits can be in 2N states

0 0 0

0 0 1

0 1 0

0 1 1

1 0 0

1 0 1

1 1 0

1 1 1

Page 70: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 70

IP(v4) Addresses

An IP(v4) address is used to identify a network and a host on the Internet

It is 32 bits long How many distinct IP addresses are there?

Page 71: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

PHY 201 (Blum) 71

Characters

We need to represent characters using numbers ASCII (American Standard Code for Information

Interchange) is a common way A string of eight bits (a byte) is used to correspond

to a character Thus 28=256 possible characters can be represented Actually ASCII only uses 7 bits, which is 128 characters;

the other 128 characters are not “standard”

Page 72: PHY 201 (Blum) 1 Resistors Ohm’s Law and Combinations of Resistors See Chapters 1 & 2 in Electronics: The Easy Way (Miller & Miller)

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Unicode

Unicode uses 16 bits, how many characters can be represented?

Enough for English, Chinese, Arabic and then some.

(Actually Unicode is extensible)

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PHY 201 (Blum) 73

ASCII

0 00110000 (48) 1 00110001 (49) … A 01000001 (65) B 01000010 (66) … a 01100001 (97) b 01100010 (98) …