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Chapter 1 Introduction to Electronics

Chapter 1 Introduction to Electronics. Microelectronic Circuit Design Richard C. Jaeger Travis N. Blalock Modified by Ming Ouhyoung. Chapter Goals. Explore the history of electronics. Quantify the impact of integrated circuit technologies. Describe classification of electronic signals.

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Chapter 1 Introduction to Electronics

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  1. Chapter 1Introduction to Electronics Microelectronic Circuit Design Richard C. JaegerTravis N. Blalock Modified by Ming Ouhyoung Microelectronic Circuit Design, 4E McGraw-Hill

  2. Chapter Goals • Explore the history of electronics. • Quantify the impact of integrated circuit technologies. • Describe classification of electronic signals. • Review circuit notation and theory. • Introduce tolerance impacts and analysis. • Describe problem solving approach Microelectronic Circuit Design, 4E McGraw-Hill

  3. The Start of the Modern Electronics Era Bardeen, Shockley, and Brattain at Bell Labs - Brattain and Bardeen invented the bipolar transistor in 1947. The first germanium bipolar transistor. Roughly 50 years later, electronics account for 10% (4 trillion dollars) of the world GDP. Microelectronic Circuit Design, 4E McGraw-Hill

  4. Braun invents the solid-state rectifier. DeForest invents triode vacuum tube. 1907-1927 First radio circuits developed from diodes and triodes. 1925 Lilienfeld field-effect device patent filed. Bardeen and Brattain at Bell Laboratories invent bipolar transistors. Commercial bipolar transistor production at Texas Instruments. Bardeen, Brattain, and Shockley receive Nobel prize. Integrated circuits developed by Kilby and Noyce First commercial IC from Fairchild Semiconductor IEEE formed from merger of IRE and AIEE First commercial IC opamp One transistor DRAM cell invented by Dennard at IBM. 4004 Intel microprocessor introduced. First commercial 1-kilobit memory. 1974 8080 microprocessor introduced. Megabit memory chip introduced. 2000 Alferov, Kilby, and Kromer share Nobel prize Electronics Milestones Microelectronic Circuit Design, 4E McGraw-Hill

  5. The Nobel Prize in Physics 2000 was awarded "for basic work on information and communication technology" with one half jointly to Zhores I. Alferov and Herbert Kroemer "for developing semiconductor heterostructures used in high-speed- and opto-electronics" and the other half to Jack S. Kilby "for his part in the invention of the integrated circuit“. Microelectronic Circuit Design, 4E McGraw-Hill

  6. Evolution of Electronic Devices Vacuum Tubes Discrete Transistors SSI and MSI Integrated Circuits VLSI Surface-Mount Circuits Microelectronic Circuit Design, 4E McGraw-Hill

  7. Microelectronics Proliferation • The integrated circuit was invented in 1958. • World transistor production has more than doubled every year for the past twenty years. • Every year, more transistors are produced than in all previous years combined. • Approximately 1018 transistors were produced in a recent year. • Roughly 50 transistors for every ant in the world. *Source: Gordon Moore’s Plenary address at the 2003 International Solid State Circuits Conference. Microelectronic Circuit Design, 4E McGraw-Hill

  8. Device Feature Size • Feature size reductions enabled by process innovations. • Smaller features lead to more transistors per unit area and therefore higher density. Microelectronic Circuit Design, 4E McGraw-Hill

  9. Rapid Increase in Density of Microelectronics Memory chip density versus time. Microprocessor complexity versus time. Microelectronic Circuit Design, 4E McGraw-Hill

  10. Signal Types • Analog signals take on continuous values - typically current or voltage. • Digital signals appear at discrete levels. Usually we use binary signals which utilize only two levels. • One level is referred to as logical 1 and logical 0 is assigned to the other level. Microelectronic Circuit Design, 4E McGraw-Hill

  11. Analog signals are continuous in time and voltage or current. (Charge can also be used as a signal conveyor.) After digitization, the continuous analog signal becomes a set of discrete values, typically separated by fixed time intervals. Analog and Digital Signals Microelectronic Circuit Design, 4E McGraw-Hill

  12. For an n-bit D/A converter, the output voltage is expressed as: The smallest possible voltage change is known as the least significant bit or LSB. Digital-to-Analog (D/A) Conversion Microelectronic Circuit Design, 4E McGraw-Hill

  13. Analog input voltage vx is converted to the nearest n-bit number. For a four bit converter, 0 → vx input yields a 0000 → 1111 digital output. Output is approximation of input due to the limited resolution of the n-bit output. Error is expressed as: Analog-to-Digital (A/D) Conversion Microelectronic Circuit Design, 4E McGraw-Hill

  14. A/D Converter Transfer Characteristic Microelectronic Circuit Design, 4E McGraw-Hill

  15. Notational Conventions • Total signal = DC bias + time varying signal • Resistance and conductance - R and G with same subscripts will denote reciprocal quantities. Most convenient form will be used within expressions. Microelectronic Circuit Design, 4E McGraw-Hill

  16. Problem-Solving Approach • Make a clear problem statement. • List known information and given data. • Define the unknowns required to solve the problem. • List assumptions. • Develop an approach to the solution. • Perform the analysis based on the approach. • Check the results and the assumptions. • Has the problem been solved? Have all the unknowns been found? • Is the math correct? Have the assumptions been satisfied? • Evaluate the solution. • Do the results satisfy reasonableness constraints? • Are the values realizable? • Use computer-aided analysis to verify hand analysis Microelectronic Circuit Design, 4E McGraw-Hill

  17. What are Reasonable Numbers? • If the power supply is ± 10 V, a calculated DC bias value of 15 V (not within the range of the power supply voltages) is unreasonable. • Generally, our bias current levels will be between 1 μ A and a few hundred milliamps. • A calculated bias current of 3.2 amps is probably unreasonable and should be reexamined. • Peak-to-peak ac voltages should be within the power supply voltage range. • A calculated component value that is unrealistic should be rechecked. For example, a resistance equal to 0.013 ohms. • Given the inherent variations in most electronic components, three significant digits are adequate for representation of results. Three significant digits are used throughout the text. Microelectronic Circuit Design, 4E McGraw-Hill

  18. Circuit Theory: Voltage Division (9/19) and Applying KVL (Kirchhoff’s voltage law) to the loop, and Combining these yields the basic voltage division formula: Microelectronic Circuit Design, 4E McGraw-Hill

  19. Circuit Theory: Voltage Division (cont.) Using the derived equations with the indicated values, Design Note: Voltage division only applies when both resistors are carrying the same current. Microelectronic Circuit Design, 4E McGraw-Hill

  20. Kirchhoff's voltage law (KVL) • The principle of conservation of energy implies that • The directed sum of the electrical potential differences (voltage) around any closed circuit is zero. Microelectronic Circuit Design, 4E McGraw-Hill

  21. Circuit Theory: Current Division where and Combining and solving for vs, Combining these yields the basic current division formula: and Microelectronic Circuit Design, 4E McGraw-Hill

  22. Circuit Theory: Current Division (cont.) Using the derived equations with the indicated values, Design Note: Current division only applies when the same voltage appears across both resistors. Microelectronic Circuit Design, 4E McGraw-Hill

  23. Kirchhoff's current law (KCL) • The principle of conservation of electric charge implies that: • At any node (junction) in an electrical circuit, the sum of currents flowing into that node is equal to the sum of currents flowing out of that node. Microelectronic Circuit Design, 4E McGraw-Hill

  24. Circuit Theory: Thévenin and Norton Equivalent Circuits Thévenin Norton Microelectronic Circuit Design, 4E McGraw-Hill

  25. Thévenin Equivalent Circuits(戴維寧等效電路) • The Thévenin-equivalent voltage is the voltage at the output terminals of the original circuit. Microelectronic Circuit Design, 4E McGraw-Hill

  26. Thévenin Equivalent Circuits • The Thévenin-equivalent resistance is the resistance measured across points A and B "looking back" into the circuit. • It is important to first replace all voltage- and current-sources with their internal resistances. • For an ideal voltage source, this means replace the voltage source with a short circuit. • For an ideal current source, this means replace the current source with an open circuit. Microelectronic Circuit Design, 4E McGraw-Hill

  27. Problem: Find the Thévenin equivalent voltage at the output. Solution: Known Information and Given Data: Circuit topology and values in figure. Unknowns: Thévenin equivalent voltage vth. Approach: Voltage source vth is defined as the output voltage with no load. Assumptions: None. Analysis: Next slide… Circuit Theory: Find the Thévenin Equivalent Voltage Microelectronic Circuit Design, 4E McGraw-Hill

  28. Circuit Theory: Find the Thévenin Equivalent Voltage Applying KCL at the output node, Current i1 can be written as: Combining the previous equations Microelectronic Circuit Design, 4E McGraw-Hill

  29. Circuit Theory: Find the Thévenin Equivalent Voltage (cont.) Using the given component values: and Microelectronic Circuit Design, 4E McGraw-Hill

  30. Problem: Find the Thévenin equivalent resistance. Solution: Known Information and Given Data: Circuit topology and values in figure. Unknowns: Thévenin equivalent Resistance Rth. Approach: Find Rth as the output equivalent resistance with independent sources set to zero. Assumptions: None. Analysis: Next slide… Circuit Theory: Find the Thévenin Equivalent Resistance Test voltage vx has been added to the previous circuit. Applying vx and solving for ix allows us to find the Thévenin resistance as vx/ix. Microelectronic Circuit Design, 4E McGraw-Hill

  31. Circuit Theory: Find the Thévenin Equivalent Resistance (cont.) Applying KCL, Microelectronic Circuit Design, 4E McGraw-Hill

  32. Norton Equivalent Circuits • Calculate the output current, IAB, with a shortcircuit as the load. Microelectronic Circuit Design, 4E McGraw-Hill

  33. Problem: Find the Norton equivalent circuit. Solution: Known Information and Given Data: Circuit topology and values in figure. Unknowns: Norton equivalent short circuit current in. Approach: Evaluate current through output short circuit. Assumptions: None. Analysis: Next slide… Circuit Theory: Find the Norton Equivalent Circuit A short circuit has been applied across the output. The Norton current is the current flowing through the short circuit at the output. Microelectronic Circuit Design, 4E McGraw-Hill

  34. Circuit Theory: Find the Norton Equivalent Circuit (cont.) Applying KCL, Short circuit at the output causes zero current to flow through RS. Rth is equal to Rth found earlier. Microelectronic Circuit Design, 4E McGraw-Hill

  35. Final Thévenin and Norton Circuits Check of Results: Note that vth = inRth and this can be used to check the calculations: inRth=(2.55 mS)vi(282 ) = 0.719vi, accurate within round-off error. While the two circuits are identical in terms of voltages and currents at the output terminals, there is one difference between the two circuits. With no load connected, the Norton circuit still dissipates power! Microelectronic Circuit Design, 4E McGraw-Hill

  36. Ω ℧ • The SI unit of electrical conductance is the siemens, also known as the mho (ohm spelled backwards, symbol is ℧); it is the reciprocal of resistance in ohms. Microelectronic Circuit Design, 4E McGraw-Hill

  37. Frequency Spectrum of Electronic Signals • Non repetitive signals have continuous spectra often occupying a broad range of frequencies • Fourier theory tells us that repetitive signals are composed of a set of sinusoidal signals with distinct amplitude, frequency, and phase. • The set of sinusoidal signals is known as a Fourier series. • The frequency spectrum of a signal is the amplitude and phase components of the signal versus frequency. Microelectronic Circuit Design, 4E McGraw-Hill

  38. Frequencies of Some Common Signals • Audible sounds 20 Hz - 20 KHz • Baseband TV 0 - 4.5 MHz • FM Radio 88 - 108 MHz • Television (Channels 2-6) 54 - 88 MHz • Television (Channels 7-13) 174 - 216 MHz • Maritime and Govt. Comm. 216 - 450 MHz • Cell phones and other wireless 1710 - 2690 MHz • Satellite TV 3.7 - 4.2 GHz • Wireless Devices 5.0 - 5.5 GHz Microelectronic Circuit Design, 4E McGraw-Hill

  39. Fourier Series • Any periodic signal contains spectral components only at discrete frequencies related to the period of the original signal. • A square wave is represented by the following Fourier series: 0=2/T (rad/s) is the fundamental radian frequency and f0=1/T (Hz) is the fundamental frequency of the signal. 2f0, 3f0, 4f0 and called the second, third, and fourth harmonic frequencies. Microelectronic Circuit Design, 4E McGraw-Hill

  40. Microelectronic Circuit Design, 4E McGraw-Hill

  41. Microelectronic Circuit Design, 4E McGraw-Hill

  42. Amplifier Basics • Analog signals are typically manipulated with linear amplifiers. • Although signals may be comprised of several different components, linearity permits us to use the superposition principle. • Superposition allows us to calculate the effect of each of the different components of a signal individually and then add the individual contributions to the output. Microelectronic Circuit Design, 4E McGraw-Hill

  43. Amplifier Linearity Given an input sinusoid: For a linear amplifier, the output is at the same frequency, but different amplitude and phase. In phasor notation: Amplifier gain is: Microelectronic Circuit Design, 4E McGraw-Hill

  44. Amplifier Input/Output Response vi = sin2000t V Av = -5 Note: negative gain is equivalent to 180 degrees of phase shift. Microelectronic Circuit Design, 4E McGraw-Hill

  45. Ideal Operational Amplifier (Op Amp) • Ideal op amps are assumed to have • infinite voltage gain, and • infinite input resistance. • These conditions lead to two assumptions useful in analyzing ideal op-amp circuits: • 1. The voltage difference across the input terminals is zero. • 2. The input currents are zero. Microelectronic Circuit Design, 4E McGraw-Hill

  46. Ideal Op Amp Example Writing a loop equation: From assumption 2, we know that i- = 0. Assumption 1 requires v- = v+ = 0. Combining these equations yields: Assumption 1 requiring v- = v+ = 0 creates what is known as a virtual ground. Microelectronic Circuit Design, 4E McGraw-Hill

  47. Ideal Op Amp Example (Alternative Approach) From Assumption 2, i2 = ii: Yielding: Design Note: The virtual ground is not an actual ground. Do not short the inverting input to ground to simplify analysis. Microelectronic Circuit Design, 4E McGraw-Hill

  48. Amplifier Frequency Response Amplifiers can be designed to selectively amplify specific ranges of frequencies. Such an amplifier is known as a filter. Several filter types are shown below: Low Pass High Pass Band Pass Band Reject All Pass Microelectronic Circuit Design, 4E McGraw-Hill

  49. Circuit Element Variations • All electronic components have manufacturing tolerances. • Resistors can be purchased with  10%,  5%, and  1% tolerance. (IC resistors are often  10%.) • Capacitors can have asymmetrical tolerances such as +20%/-50%. • Power supply voltages typically vary from 1% to 10%. • Device parameters will also vary with temperature and age. • Circuits must be designed to accommodate these variations. • We will use worst-case and Monte Carlo (statistical) analysis to examine the effects of component parameter variations. Microelectronic Circuit Design, 4E McGraw-Hill

  50. Tolerance Modeling • For symmetrical parameter variations Pnom(1 - )  P  Pnom(1 + ) • For example, a 10K resistor with 5% percent tolerance could take on the following range of values: 10k(1 - 0.05)  R  10k(1 + 0.05) 9,500   R  10,500  Microelectronic Circuit Design, 4E McGraw-Hill

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