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EE2420 – Digital Logic Summer II 2013 Set 2: Boolean Logic Hassan Salamy Ingram School of Engineering Texas State University Boolean Algebra 2     The basis for much of what we will do in this class is grounded in Boolean algebra, named for George Boole. In the early chapters of the textbook we will study the Theorems and Laws of Boolean Algebra and techniques for implementing Boolean functions using electronic circuits. In later chapters we will study how Boolean functions can be used to implement arithmetic and other useful functions. Later still we will adapt these techniques to create components critical to modern computing such as memory elements and sequence logic. Electrical Circuits (Over)simplified 3     For those of you who have had no experience with electrical circuits, the following is a vastly oversimplified primer. The simple model of matter is that it is made up of atoms which have positively-charged nuclei orbited by negatively-charged electrons. Given sufficient energy, an electron can be dislodged from its atom. Think of electricity as the flow of energy carried by the movement of electrons dislodged from atoms. An electrical circuit is formed when there is a closed path around which the electrons flow. Circuits Primer part 2 4        In electrical circuits, we are interested in the movement of energy from one location to another. Some elements in a circuit provide energy. These are sources. Some elements in a circuit expend energy. These are sinks. The total energy sourced must equal the total energy expended. We typically measure energy somewhat indirectly. Energy is measured in Joules (J). Power is energy per unit time. Power is measured in Watts (W). A Watt is one Joule per second. 1W = 1J/s A 100W light bulb expends 100 Joules each second. Circuits Primer part 3 5      We said a 100W light bulb expends 100 Joules each second. We also said to think of electricity as the flow of energy carried by the movement of electrons dislodged from atoms. To get energy to the light bulb, we make a circuit from the power producing plant to the light bulb. In that circuit each moving electron is charged with energy at the source. When an electron passes through the sink (light) that energy is expended. The amount of power that can be supplied depends on two factors:   The number of electrons that can move through the wires The amount of energy carried with each electron Circuits Primer part 4 6    The number of electrons flowing in a circuit is called current. Current is measured in Amperes (A). An Ampere is one Coulomb of electrons per second. A Coulomb is 6,241,507,648,655,549,400 (approx 6.24 x 1018) electrons. The amount of energy per electron is called voltage. Voltage is measured in Volts (V). One Volt is one Joule per Coulomb. So to determine power we take the product of the number of electrons flowing (current) and the energy per electron (voltage) and we should get a measure of power (wattage)  Voltage * Current = Power  In units V*A=W or (J/C)*(C/s) = (J/s) Circuits Primer part 5 7      Most of the devices that we will be dealing with in this class will operate using relatively low power circuits. However, this does not make them 100% safe. It also does not make it impossible to damage the equipment if used incorrectly. Electricity flows very easily through most metals, including jewelry. It would be wise when you are dealing with any circuitry to remove any jewelry from your hands (rings, watches, etc. ) or long necklaces that could contact the circuitry. Be careful how you wire the power supply to your circuits. If you reverse the polarity and try to drive current “backward” through the circuit, you are likely to cause damage. Ask your lab monitor if you are not sure. The Scope of Boolean Algebra 8     In common arithmetic, we are often concerned with the range of values that a variable may take. This is generally determined by the nature of the problem:  The integers 1-12 – the month of the year  A 7-digit decimal integer – local telephone number  A real number in the interval from 0 to 100 – a test grade  Imaginary numbers. For Boolean algebra, every variable is constrained to one of two values: True or False Any convenient two-valued pair can be used to represent the True/False pair: on/off, high/low, clockwise/counter-clockwise, closed/open, loud/soft, 1/0 We will commonly use the 1/0 notation with 1=True and 0=False Switches 9  A very early electronic implementation of Boolean algebra recognized that the state of a switch (open or closed) could be used to represent a Boolean variable (True or False) and that switches could be wired in combination to represent complex Boolean algebra equations. Open Switch Closed Switch Electrically-controlled Switches 10     A simple mechanical switch (like a light switch on a wall) requires physical effort to manually open or close the contact. An electrically-controlled switch is opened or closed based on the state of an input. For a normally-open switch, when the input is inactive, the switch is open and when the input is active, the switch closes. For a normally-closed switch, when the input is inactive, the switch is closed and when the input is active, the switch opens. Normally-open Normally-closed Types of Switches 11      The earliest devices used for electrically-controlled switching for Boolean algebra purposes were relays. A relay uses an input to generate an electromagnetic field that physically moves the switch contacts into position. Because relays depend on physical movement of the contacts, they are too slow for modern digital computing purposes. Modern systems use transistors to perform the function of switches without requiring mechanical movement. While transistors are complex devices capable of much more than digital switching, when used for switching they may be modeled as very simple electrically-controlled switches. Active-high Input Switching Devices 12  BJT – Bipolar Junction Transistor  MOSFET – Metal-Oxide Semiconductor Field Effect Transistor Switch NMOS: input NPN BJT +V=On Conducting path Normally-open Conducting path Conducting path input input N-channel MOSFET 0V=Off Lecture 2: Boolean Logic 12/28 Active-low Input Switching Devices 13  BJT – Bipolar Junction Transistor  MOSFET – Metal-Oxide Semiconductor Field Effect Transistor Switch input PNP BJT Conducting path Normally-closed Conducting path Conducting path input input P-channel MOSFET PMOS: +V=Off 0V =On 13/28 Switch Logic 14   In the following circuit, the battery is connected to the lamp if switch A is closed and switch B is closed. If either switch is open, there is not a complete circuit. This is the Boolean function AND Switch A Battery Switch B Lamp Switch Logic 15   In the following circuit, the battery is connected to the lamp if switch A is closed or switch B is closed. If either switch is closed, there is a complete circuit. This is the Boolean function OR Switch A Switch B Battery Lamp Switch Logic 16   In the following circuit, the battery is connected to the lamp and the output voltage is high if the input to the normally-closed switch is low. Conversely, when the input is high, the lamp is disconnected and the output drops to 0.  Therefore, the output is the opposite of the input.  This is the Boolean function NOT Input Output Battery Lamp Logic Gates 17  Special circuit symbols are used for the Boolean logic functions regardless of the type of switches used to implement the functions. AND OR NOT Logic circuits 18      Logic circuits perform operations on digital signals  Implemented as electronic circuits where signal values are restricted to a few discrete values In binary logic circuits there are only two values, 0 and 1 Switching Network The general form of a logic circuit is a switching network In the figure to the right, the inputs are labeled Xn and the outputs are labeled Yn Not shown in the figure are the required connections for providing power to the circuit. Y1 Y2 Y3 X1 X2 X3 Yn Xm discrete values Boolean algebra 19  Direct application to switching networks Work with 2-state devices  2-valued Boolean algebra (switching algebra)  Use a Boolean variable (X, Y, etc.) to represent an input or output of a switching network  Boolean variable may take on only two values (True, False)  We will use a notation of 0 for False and 1 for True  So the possibilities for a variable are: X=0, X=1  These symbols are not binary numbers, they simply represent the 2 states of a Boolean variable  They are not voltage levels, although they commonly refer to the low or high voltage input/output of some circuit element  Notation Conventions 20    Boolean AND  The raised dot “· ”  x· y  The intersection symbol “”  x  y  No symbol  xy Boolean OR  Plus sign “+”  x + y  The union symbol “”  x y Boolean NOT  Single quotation “ ’ ” following  x’  Bar over letter   Exclamation point preceding  !x  Tilde preceding  ~x x Inversion of a function 21  If a function is defined as  f(x1,  Then the complement of f is  f(x1,  x2)= x1+ x2 = (x1+ x2)’ Similarly, if  f(x1,  x2)= x1+ x2 x2)= x1 · x2 Then the complement of f is  f(x1, x2)= x1 · x2= (x1 · x2)’ Truth tables 22  Tabular listing that fully describes a logic function  Output x1 x2 0 0 0 value for all input combinations (valuations) x1· x2 x1 x2 0 0 0 0 0 1 1 0 0 1 1 1 0 1 0 0 1 0 1 1 1 1 1 1 1 AND x1 + x2 OR x1 x1’ NOT Truth tables 23  Truth table for AND and OR functions of three variables Truth tables of functions 24  If L(x,y,z)=x+yz, then the truth table for L is: + x 0 0 0 0 1 1 1 1 y 0 0 1 1 0 0 1 1 z 0 1 0 1 0 1 0 1 yz 0 0 0 1 0 0 0 1 x+yz 0 0 0 1 1 1 1 1 Logic gates and networks 25  A larger circuit is implemented by a network of gates  Called x x x a logic network or logic circuit 1 2 3 f = (x + x )  x 1 2 3 Logic gates and networks 26  Draw the truth table and the logic circuit for the following function  F(a,b,c) a 0 0 0 0 1 1 1 1 b 0 0 1 1 0 0 1 1 c 0 1 0 1 0 1 0 1 ac 0 0 0 0 0 1 0 1 = ac+bc’ bc' 0 0 1 0 0 0 1 0 ac+bc' 0 0 1 0 0 1 1 1 a c b Analysis of a logic network 27  To determine the functional behavior of a logic network, we can apply all possible input signals to it x x 0 01 1 1 10 0 1 A 0 10 1 0 00 1 11 0 1 B 2 Network that implements f = x1 + x1  x2 f Analysis of a logic network 28  The function of a logic network can also be described by a timing diagram (gives dynamic behavior of the network) 1 x 1 0 x 1 2 0 A 1 0 B 1 0 f 1 0 Time Timing diagram