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Sinusoidal Signal Described using three parameters Equation

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1 Sinusoidal Signal Described using three parameters Equation
Amplitude Frequency or period of oscillation Phase or time offset Equation 𝑔 𝑑 =π΄βˆ™ cos 2πœ‹ 𝑓 0 𝑑+πœƒ Variations

2 Real Exponential Signal
Described using two parameters Amplitude Rate of decay or growth Equation 𝑔 𝑑 =π΄βˆ™ 𝑒 𝜎 0 𝑑 Variations

3 Complex Exponential Signal
Described using three parameters Amplitude Rate of decay or growth Frequency of oscillation Equation 𝑔 𝑑 =π΄βˆ™ 𝑒 𝜎 0 +𝑗 πœ” 0 𝑑 Variations

4 Complex Exponential Signal
The complex exponential can be split into real and imaginary components that are expressed as combination of the real exponential and sinusoidal signals. Equation 𝑔 𝑑 =π΄βˆ™ 𝑒 𝜎 0 +𝑗 πœ” 0 𝑑 =π΄βˆ™ 𝑒 𝜎 0 𝑑 βˆ™ cos πœ” 0 𝑑 +𝑗 sin πœ” 0 𝑑 Angular Rotation in the complex plane as time increases

5 Complex Exponential Signal
Recovering sin and cos from the complex exponential Equation 𝑔 1 𝑑 =π΄βˆ™ 𝑒 𝑗 πœ” 0 𝑑 =π΄βˆ™ cos πœ” 0 𝑑 +𝑗 sin πœ” 0 𝑑 𝑔 2 𝑑 =π΄βˆ™ 𝑒 βˆ’π‘— πœ” 0 𝑑 =π΄βˆ™ cos πœ” 0 𝑑 βˆ’π‘— sin πœ” 0 𝑑 Evaluate g1 + g2 and g1 – g2 𝑔 1 + 𝑔 2 =2π΄βˆ™ cos πœ” 0 𝑑 𝑔 1 βˆ’ 𝑔 2 =𝑗2π΄βˆ™ sin πœ” 0 𝑑 Which also gives relationships for sinΟ‰0t and cosΟ‰0t.

6 Discontinuities There are a class of related functions that represent a discontinuities. lim πœ€β†’0 𝑔 𝑑 0 βˆ’πœ€ β‰  lim πœ€β†’0 𝑔 𝑑 0 +πœ€ The mathematical description of these functions require some type of limit or conditional inequality. These are useful because they can be used to model switching and sampling events as well.

7 Signum The signum function can be interpreted as a test that returns the sign of the input. 𝑠𝑔𝑛 𝑑 = βˆ’1, 𝑑<0 0, 𝑑=0 1, 𝑑>0 All other discontinuous function can be derived from this function (or visa versa).

8 Unit Step Function The unit step function signifies activation at time zero. It is zero for time less than zero and unity for time greater than zero. 𝑒 𝑑 = 0, 𝑑< , 𝑑= 0 βˆ— 1, 𝑑>0 In some cases, t=0 is ignored or included in one of the other cases. Express in terms of sgn(t).

9 Example with the Unit Step Function
RC circuit with a switch

10 Unit Ramp Function As the name implies, the unit ramp starts increasing from zero at time zero with a slope of one. ramp 𝑑 = 0, 𝑑≀0 𝑑, 𝑑>0 Can be express using the unit step function. Again.

11 Unit Rectangle Function
The unit rectangle function is similar to the unit step function except it is on for the time interval -1/2 to +1/2. rect 𝑑 = 0, 𝑑 > , 𝑑 = 1 2 βˆ— 1, 𝑑 < 1 2 Can be express using the unit step function. What is the area?

12 Impulse Function The impulse function has two important characteristics: Has a value of zero at every point except t=0. Has an area of unity. 𝛿 𝑑 =0, 𝑑≠0 and 𝑑 1 𝑑 2 𝛿 𝑑 𝑑𝑑 = 1, 𝑑 1 <0< 𝑑 1 0, otherwise As a result, the impulse function, Ξ΄(t), is somewhat difficult to express directly. Point 2 above, seems to indicate some relationship between the impulse and the unit rectangle function.

13 Impulse Function Deriving the impulse function using limits and the unit rectangle function. Graphical Representation.

14 Impulse Relationships
Relating the impulse to the unit step function.

15 Impulses and other functions
Multiply a function by an impulse. Multiply a function by a shifted impulse

16 Impulses and other functions
Sampling property of the impulse.

17 Impulses and other functions
Scaling property of the impulse. Related to the unit rectangle function (first).

18 The Impulse Train A series of impulse functions shifted by multiples of T. 𝛿 𝑇 𝑑 = 𝑛=βˆ’βˆž ∞ 𝛿 π‘‘βˆ’π‘›π‘‡ Apply scaling/time shift to the impulse train.

19

20 Manipulating Functions
We can manipulate function to represent or model more interesting signals. Think of the previous definitions as building blocks. Combinations of multiple functions are constructed using arithmetical operations (+,-,Γ—,Γ·). Be careful when dividing by zero. Functions can be scaled and shifted to make them more useful. Be careful when integrating. Integration and differentiation can be used to further manipulate functions. Nested functions

21 Combinations of Functions
Building Blocks Polynomial: g(t) = aNtN + aN-1tN a2t2 + a1t + a0 Sinusoidal Signal Exponential (real and complex) Signum Unit Step, Unit Ramp, and Unit Rectangle Impulse and impulse Train Operations Arithmetic Time Shifting Derivatives and Integrals Functions of functions Creativity

22 Examples: Binary (...,1,1,0,1,0,0,0,1,0,1,0,...)

23 Examples: Binary Amplitude Modulated CW

24 Examples: Binary Phase Modulated CW

25 Examples: Linear Chirp

26 Examples: 25% duty cycle PWM

27 Examples: Ξ”, 50% DC, 1 s period, +/-5 Amp

28 Examples: Derivative & Integral of Previous

29 Examples: Derivative & Integral of Previous

30 Examples: Heartbeat

31 Examples: Earthquake

32 Examples: Bats

33 Properties of Signals Symmetry Periodic Energy and Power
Even and odd signals Even and odd Components Sums and products of even and odd signals Periodic Fundamental period Combinations of periodic signals Energy and Power

34 Even and Odd Even Signal Odd Signal Examples

35 Even and Odd Components
A signal, g(t), can be broken down into an even, ge(t), and odd, go(t) components – where g(t) = ge(t) + go(t) with ge(t) = ge(-t) go(t) = -go(-t)

36 Even and Odd Components
Even component: ge(t) Odd component: go(t)

37 Combining Even and Odd Signals
Addition (subtraction): Stays the same Multiplication ge(t) * fe(t) = ge(t) * fo(t) = go(t) * fe(t) = go(t) * fo(t) = Derivate, Integral

38 Periodicity A signal is periodic if:
g(t) = g(t-nT) when T is a constant and n is an integer The mimimul value of T is considered the fundamental period, T0 (f0 = 1/T0). Sums of periodic signals are also periodic.

39 Power Power 𝑃 π‘₯ 𝑑 = π‘₯ 𝑑 2 A periodic signal has an average power
𝑃 π‘₯ 𝑑 = π‘₯ 𝑑 2 A periodic signal has an average power 𝑃 π‘₯ π‘Žπ‘£π‘” = 1 𝑇 π‘œ 𝑑 π‘œ 𝑑 π‘œ + 𝑇 π‘œ π‘₯ 𝑑 2 𝑑𝑑 The average power of an aperiodic signal is taken as the limit T β†’ ∞. 𝑃 π‘₯ π‘Žπ‘£π‘” = lim π‘‡β†’βˆž 1 𝑇 𝑑 π‘œ 𝑑 π‘œ +𝑇 π‘₯ 𝑑 2 𝑑𝑑

40 Energy The energy is the integral of power. 𝐸 π‘₯ = βˆ’βˆž ∞ π‘₯ 𝑑 2 𝑑𝑑
𝐸 π‘₯ = βˆ’βˆž ∞ π‘₯ 𝑑 2 𝑑𝑑 A signal with finite Energy is called an energy signal. What is the average power of an energy signal? A signal with infinite Energy and finite average power is called a power signal.


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