ee210 digital electronics class lecture 2 september 03, 2008

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EE210 Digital Electronics Class Lecture 2 September 03, 2008

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EE210 Digital Electronics Class Lecture 2 September 03, 2008. Sedra/Smith Microelectronic Circuits 5/e Oxford University Press. Introduction to Electronics. 3. In This Class. We Will Discuss Following Topics : 1.1 Signals Thévenin & Norton Theorem (Append. C) - PowerPoint PPT Presentation

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Page 1: EE210 Digital Electronics Class Lecture 2 September 03, 2008

EE210 Digital Electronics

Class Lecture 2

September 03, 2008

Page 2: EE210 Digital Electronics Class Lecture 2 September 03, 2008

Sedra/SmithMicroelectronic Circuits 5/e

Oxford University Press

Page 3: EE210 Digital Electronics Class Lecture 2 September 03, 2008

Introduction to Electronics

3

Page 4: EE210 Digital Electronics Class Lecture 2 September 03, 2008

In This ClassWe Will Discuss Following Topics :

1.1 SignalsThévenin & Norton Theorem

(Append. C)1.2 Frequency Spectrum of Signals1.3 Analog and Digital Signals

Page 5: EE210 Digital Electronics Class Lecture 2 September 03, 2008

1.1 Signals1.1 Signals Signals Contain Information To Extract Information Signals Need to be

PROCESSED in Some Predetermined Manner

Electronic System Process Signals Conveniently

Signal Must be an Electric Entity, V or I Transducers Convert Physical Signal into

Electric Signal

Page 6: EE210 Digital Electronics Class Lecture 2 September 03, 2008

Two alternative representations of a signal source: (a) the Thévenin form, and (b) the Norton form.

vs (t) = Rs is(t)

Page 7: EE210 Digital Electronics Class Lecture 2 September 03, 2008

Thévenin’s theorem.

Appendix CAppendix C

Page 8: EE210 Digital Electronics Class Lecture 2 September 03, 2008

Norton’s Theorem

Page 9: EE210 Digital Electronics Class Lecture 2 September 03, 2008

Thévenin & Norton

Points to Note: Two Representations are Equivalent Parameters are Related as:

vs (t) = Rs is(t)

Thévenin Preferred When Rs Low

Norton Preferred When Rs High

Page 10: EE210 Digital Electronics Class Lecture 2 September 03, 2008

Apply Thévenin’s Theorem to Simplify A BJT Circuit

Example C.1

Page 11: EE210 Digital Electronics Class Lecture 2 September 03, 2008

An arbitrary voltage signal vs(t).

Signal is a Quantity That Varies in Time.

Information is Contained in the Change in Magnitude as Time Progresses.

Difficult to Characterize Mathematically

Page 12: EE210 Digital Electronics Class Lecture 2 September 03, 2008

1.2 Frequency Spectrum of Signals Signal (or Any Arb. Function of Time)

Characterization in Terms of Frequency Spectrum, using Fourier Series/Transform

FS and FT Help Represent Signal as Sum of Sine-wave Signals of Different Frequencies and Amplitudes

Use FS When Signal is Periodic in Time Use FT When Signal is Arbitrary in Time

Page 13: EE210 Digital Electronics Class Lecture 2 September 03, 2008

Sine-wave voltage signal of amplitude Va and frequency f = 1/T Hz. The angular frequency ω = 2πf rad/s. Continued

Page 14: EE210 Digital Electronics Class Lecture 2 September 03, 2008

Amplitude Va of Sine-wave Signal Commonly Expressed in RMS = Va / √2

Household 220 V is an RMS Value FS allows us to Express ANY Periodic

Function of Time as Sum of Infinite Number of Sinusoids Whose Frequencies are Harmonically Related, e.g., The Square-wave Signal in Next Slide.

Page 15: EE210 Digital Electronics Class Lecture 2 September 03, 2008

Using FS Square-wave Signal can be Expressed as:

v(t) = 4V/π (sin ωot + 1/3 sin 3 ωot + 1/5 sin 5 ωot + …) with ωo = 2 π/ T is Fundamental Frequency

Sinusoidal Components Makeup Frequency Spectrum

Page 16: EE210 Digital Electronics Class Lecture 2 September 03, 2008

• The Frequency Spectrum (Also Known As The Line Spectrum) Of The Previous Periodic Square Wave

• Note That Amplitude of Harmonics Progressively Decrease

• Infinite Series Can be Truncated for Approximation

Page 17: EE210 Digital Electronics Class Lecture 2 September 03, 2008

FT can be Applied to Non-Periodic Functions of time, such as:

And Provides Frequency Spectrum as a Continuous Function of Frequency, Such As:

Page 18: EE210 Digital Electronics Class Lecture 2 September 03, 2008

The Frequency Spectrum of Previous Arbitrary Non-periodic Waveform

Page 19: EE210 Digital Electronics Class Lecture 2 September 03, 2008

Periodic Signals Consists of Discrete Freq.

Non-Periodic Signals Contains ALL Freq.

HOWEVER, …

Periodic

Non-Periodic

Page 20: EE210 Digital Electronics Class Lecture 2 September 03, 2008

The Useful Parts of the Spectra of Practical Signals are Confined to Short Segments of Frequency, e.g., Audio Band is 20 Hz to 20kHz

In Summary, We can Represent A Signal : In Time-Domain va(t)

In Frequency-Domain Va(ω)

Page 21: EE210 Digital Electronics Class Lecture 2 September 03, 2008

1.3 Analog and Digital Signals1.3 Analog and Digital Signals

This is an Analog Signal as it is Analogous to Physical Signal it Represents

Its Amplitude Continuously Varies Over Its Range of Activity

Page 22: EE210 Digital Electronics Class Lecture 2 September 03, 2008

Digital Signal is Representation of the Analog Signal in Sequence of Numbers

Each Number Representing The Signal Magnitude at An Instant of Time

Let us Take the Analog Signal and Convert it To Digital Signal by SAMPLING

Sampling is a Process of Measuring The Magnitude of a Signal at an Instant of Time

Page 23: EE210 Digital Electronics Class Lecture 2 September 03, 2008

Sampling The Continuous-time Analog Signal in (a) Results in The Discrete-time Signal in (b)

Page 24: EE210 Digital Electronics Class Lecture 2 September 03, 2008

Original Signal is Now Only Defined at Sampling Instants – No More Continuous, Rather Discrete Time Signal, Still Analog as Mag. Is Cont.

If Magnitude of Each Sample is Represented by Finite Number of Digits Then Signal Amplitude will Also be Quantized, Discretized or Digitized

Then, Signal is Digital --- A Sequence of Numbers That Represent Mag. of Successive Signal Samples

Page 25: EE210 Digital Electronics Class Lecture 2 September 03, 2008

The Choice of Number System to Represent Signal Samples Affects the Type of Digital Signal Produced and Also Affects the Complexity of Dig. Circuits

The BINARY Number System Results in Simplest Possible Signals and Circuits

In a Binary Number Digit is Either 0 or 1 Correspondingly, Two Voltage Levels (Low

or High) for Digital Signal Most Digital Circuits Have 0 V or 5V

Page 26: EE210 Digital Electronics Class Lecture 2 September 03, 2008

• Time Variation of a Binary Digital Signal• Note That: Waveform is a Pulse Train with 0 V

Representing 0 or Logic 0 and 5V Rep. Logic 1

Page 27: EE210 Digital Electronics Class Lecture 2 September 03, 2008

Binary Rep. of Analog SignalTo use N Binary Digits (bits) to Represent Each

Sample of The Analog Signal, the Digitized Sample Value Can be as:

D = b0 20 + b1 21 + b2 22 + … + bN-1 2N-1

Where,

b0 , b1 ,… bN-1 are N bits with value 0 or 1

b0 is LSB and bN-1 is MSB

Binary Number Written as: bN-1 bN-2 … b0

Page 28: EE210 Digital Electronics Class Lecture 2 September 03, 2008

The Binary Rep (Cont…) Quantizes Analog Sample in 2N Levels Greater the Number of Bits (Larger N)

Closer the Digital Word D Approx. to the Magnitude of the Analog Sample

Large N Reduces the Quantization Error and Increases the Resolution of Analog-to-Digital Conversion (Increases Cost as Well)

Page 29: EE210 Digital Electronics Class Lecture 2 September 03, 2008

Block-diagram Representation Of The Analog-to-

digital Converter (ADC) – A Building Block of Modern Electronic Systems

Page 30: EE210 Digital Electronics Class Lecture 2 September 03, 2008

Once Signal is in Digital Form it Can be Processed by Digital Circuits

Digital Circuits also Process Signals which do Not Have Analog Origin, e.g., Signals Representing Digital Computer Instruction

As Digital Circuits Deal With Binary Signals Their Design is Simpler Than of Analog Circuits

While Digital Circuit Design has Its Own Challenges, It Provides Reliable and Economic Implementations of Many Signal Processing Functions not Possible With Analog Circuits

Page 31: EE210 Digital Electronics Class Lecture 2 September 03, 2008

In Next ClassWe Will Continue to Discuss:

Chapter 1: Introduction to Electronics

Topics:

1.4 Amplifiers

1.7 Logic Inverters

1.8 Circuit Simulation Using SPICE