7: Fourier Transforms: Convolution and Parseval s Theorem

Size: px
Start display at page:

Download "7: Fourier Transforms: Convolution and Parseval s Theorem"

Transcription

1 Convolution Parseval s E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 /

2 Multiplication of Signals Question: What is the Fourier transform ofw(t) = u(t)v(t)? Convolution Parseval s E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 2 /

3 Multiplication of Signals Convolution Parseval s Question: What is the Fourier transform ofw(t) = u(t)v(t)? Letu(t) = + h= U(h)ei2πht dh and v(t) = + g= V(g)ei2πgt dg E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 2 /

4 Multiplication of Signals Convolution Parseval s Question: What is the Fourier transform ofw(t) = u(t)v(t)? Letu(t) = + h= U(h)ei2πht dh and v(t) = + g= V(g)ei2πgt dg w(t) = u(t)v(t) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 2 /

5 Multiplication of Signals Convolution Parseval s Question: What is the Fourier transform ofw(t) = u(t)v(t)? Letu(t) = + h= U(h)ei2πht dh and v(t) = + g= V(g)ei2πgt dg w(t) = u(t)v(t) [Note use of different dummy variables] = + h= U(h)ei2πht dh + g= V(g)ei2πgt dg E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 2 /

6 Multiplication of Signals Convolution Parseval s Question: What is the Fourier transform ofw(t) = u(t)v(t)? Letu(t) = + h= U(h)ei2πht dh and v(t) = + g= V(g)ei2πgt dg w(t) = u(t)v(t) [Note use of different dummy variables] = + h= U(h)ei2πht dh + g= V(g)ei2πgt dg = + h= U(h) + g= V(g)ei2π(h+g)t dgdh [mergee ( ) ] E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 2 /

7 Multiplication of Signals Convolution Parseval s Question: What is the Fourier transform ofw(t) = u(t)v(t)? Letu(t) = + h= U(h)ei2πht dh and v(t) = + g= V(g)ei2πgt dg w(t) = u(t)v(t) [Note use of different dummy variables] = + h= U(h)ei2πht dh + g= V(g)ei2πgt dg = + h= U(h) + g= V(g)ei2π(h+g)t dgdh [mergee ( ) ] Now we make a change of variable in the second integral: g = f h = + h= U(h) + f= V(f h)ei2πft df dh E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 2 /

8 Multiplication of Signals Convolution Parseval s Question: What is the Fourier transform ofw(t) = u(t)v(t)? Letu(t) = + h= U(h)ei2πht dh and v(t) = + g= V(g)ei2πgt dg w(t) = u(t)v(t) [Note use of different dummy variables] = + h= U(h)ei2πht dh + g= V(g)ei2πgt dg = + h= U(h) + g= V(g)ei2π(h+g)t dgdh [mergee ( ) ] Now we make a change of variable in the second integral: g = f h = + h= U(h) + = f= f= V(f h)ei2πft df dh + h= U(h)V(f h)ei2πft dhdf [swap ] E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 2 /

9 Multiplication of Signals Convolution Parseval s Question: What is the Fourier transform ofw(t) = u(t)v(t)? Letu(t) = + h= U(h)ei2πht dh and v(t) = + g= V(g)ei2πgt dg w(t) = u(t)v(t) [Note use of different dummy variables] = + h= U(h)ei2πht dh + g= V(g)ei2πgt dg = + h= U(h) + g= V(g)ei2π(h+g)t dgdh [mergee ( ) ] Now we make a change of variable in the second integral: g = f h = + h= U(h) + = f= f= V(f h)ei2πft df dh + h= U(h)V(f h)ei2πft dhdf [swap ] = + f= W(f)ei2πft df E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 2 /

10 Multiplication of Signals Convolution Parseval s Question: What is the Fourier transform ofw(t) = u(t)v(t)? Letu(t) = + h= U(h)ei2πht dh and v(t) = + g= V(g)ei2πgt dg w(t) = u(t)v(t) [Note use of different dummy variables] = + h= U(h)ei2πht dh + g= V(g)ei2πgt dg = + h= U(h) + g= V(g)ei2π(h+g)t dgdh [mergee ( ) ] Now we make a change of variable in the second integral: g = f h = + h= U(h) + = f= f= V(f h)ei2πft df dh + h= U(h)V(f h)ei2πft dhdf [swap ] = + f= W(f)ei2πft df wherew(f) = + U(h)V(f h)dh h= E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 2 /

11 Multiplication of Signals Convolution Parseval s Question: What is the Fourier transform ofw(t) = u(t)v(t)? Letu(t) = + h= U(h)ei2πht dh and v(t) = + g= V(g)ei2πgt dg w(t) = u(t)v(t) [Note use of different dummy variables] = + h= U(h)ei2πht dh + g= V(g)ei2πgt dg = + h= U(h) + g= V(g)ei2π(h+g)t dgdh [mergee ( ) ] Now we make a change of variable in the second integral: g = f h = + h= U(h) + = f= f= V(f h)ei2πft df dh + h= U(h)V(f h)ei2πft dhdf [swap ] = + f= W(f)ei2πft df wherew(f) = + U(h)V(f h)dh U(f) V(f) h= E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 2 /

12 Multiplication of Signals Convolution Parseval s Question: What is the Fourier transform ofw(t) = u(t)v(t)? Letu(t) = + h= U(h)ei2πht dh and v(t) = + g= V(g)ei2πgt dg w(t) = u(t)v(t) [Note use of different dummy variables] = + h= U(h)ei2πht dh + g= V(g)ei2πgt dg = + h= U(h) + g= V(g)ei2π(h+g)t dgdh [mergee ( ) ] Now we make a change of variable in the second integral: g = f h = + h= U(h) + = f= f= V(f h)ei2πft df dh + h= U(h)V(f h)ei2πft dhdf [swap ] = + f= W(f)ei2πft df wherew(f) = + h= U(h)V(f h)dh U(f) V(f) This is the convolution of the two spectrau(f) andv(f). E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 2 /

13 Multiplication of Signals Convolution Parseval s Question: What is the Fourier transform ofw(t) = u(t)v(t)? Letu(t) = + h= U(h)ei2πht dh and v(t) = + g= V(g)ei2πgt dg w(t) = u(t)v(t) [Note use of different dummy variables] = + h= U(h)ei2πht dh + g= V(g)ei2πgt dg = + h= U(h) + g= V(g)ei2π(h+g)t dgdh [mergee ( ) ] Now we make a change of variable in the second integral: g = f h = + h= U(h) + = f= f= V(f h)ei2πft df dh + h= U(h)V(f h)ei2πft dhdf [swap ] = + f= W(f)ei2πft df wherew(f) = + U(h)V(f h)dh U(f) V(f) h= This is the convolution of the two spectrau(f) andv(f). w(t) = u(t)v(t) W(f) = U(f) V(f) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 2 /

14 Multiplication Example Convolution Parseval s u(t) = e at t a= t < Time (s) u(t) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 3 /

15 Multiplication Example u(t) = e at t t < u(t) a= Time (s) Convolution U(f) = a+i2πf [from before] Parseval s E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 3 /

16 Multiplication Example Convolution Parseval s u(t) = U(f) = a+i2πf e at t t < [from before] u(t) U(f) a= Time (s) Frequency (Hz) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 3 /

17 Multiplication Example Convolution Parseval s u(t) = U(f) = a+i2πf e at t t < [from before] u(t) U(f) <U(f) (rad/pi a= Time (s) Frequency (Hz) Frequence (Hz) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 3 /

18 Multiplication Example Convolution Parseval s u(t) = U(f) = a+i2πf e at t t < v(t) = cos2πft [from before] u(t) U(f) <U(f) (rad/pi a= Time (s) Frequency (Hz) Frequence (Hz) v(t) Time (s) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 3 /

19 Multiplication Example Convolution Parseval s u(t) = U(f) = a+i2πf e at t t < v(t) = cos2πft [from before] V(f) =.5(δ(f +F)+δ(f F)) u(t) U(f) <U(f) (rad/pi a= Time (s) Frequency (Hz) Frequence (Hz) v(t) Time (s) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 3 /

20 Multiplication Example Convolution Parseval s u(t) = U(f) = a+i2πf e at t t < v(t) = cos2πft [from before] V(f) =.5(δ(f +F)+δ(f F)) u(t) U(f) <U(f) (rad/pi a= Time (s) Frequency (Hz) Frequence (Hz) v(t) V(f) Time (s).4 F= Frequency (Hz) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 3 /

21 Multiplication Example Convolution Parseval s u(t) = U(f) = a+i2πf e at t t < v(t) = cos2πft [from before] V(f) =.5(δ(f +F)+δ(f F)) w(t) = u(t)v(t) u(t) U(f) <U(f) (rad/pi a= Time (s) Frequency (Hz) Frequence (Hz) v(t) V(f) w(t) Time (s).4 F= Frequency (Hz) a=2, F=2-5 5 Time (s) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 3 /

22 Multiplication Example Convolution Parseval s u(t) = U(f) = a+i2πf e at t t < v(t) = cos2πft [from before] V(f) =.5(δ(f +F)+δ(f F)) w(t) = u(t)v(t) W(f) = U(f) V(f) u(t) U(f) <U(f) (rad/pi a= Time (s) Frequency (Hz) Frequence (Hz) v(t) V(f) w(t) Time (s).4 F= Frequency (Hz) a=2, F=2-5 5 Time (s) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 3 /

23 Multiplication Example Convolution Parseval s u(t) = U(f) = a+i2πf e at t t < v(t) = cos2πft [from before] V(f) =.5(δ(f +F)+δ(f F)) w(t) = u(t)v(t) W(f) = U(f) V(f) =.5 a+i2π(f+f) +.5 a+i2π(f F) u(t) U(f) <U(f) (rad/pi a= Time (s) Frequency (Hz) Frequence (Hz) v(t) V(f) w(t) Time (s).4 F= Frequency (Hz) a=2, F=2-5 5 Time (s) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 3 /

24 Multiplication Example Convolution Parseval s u(t) = U(f) = a+i2πf e at t t < v(t) = cos2πft [from before] V(f) =.5(δ(f +F)+δ(f F)) w(t) = u(t)v(t) W(f) = U(f) V(f) =.5 a+i2π(f+f) +.5 a+i2π(f F) u(t) U(f) <U(f) (rad/pi a= Time (s) Frequency (Hz) Frequence (Hz) v(t) V(f) w(t) W(f) Time (s).4 F= Frequency (Hz) a=2, F=2-5 5 Time (s) Frequency (Hz) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 3 /

25 Multiplication Example Convolution Parseval s u(t) = U(f) = a+i2πf e at t t < v(t) = cos2πft [from before] V(f) =.5(δ(f +F)+δ(f F)) w(t) = u(t)v(t) W(f) = U(f) V(f) =.5 a+i2π(f+f) +.5 a+i2π(f F) u(t) U(f) <U(f) (rad/pi a= Time (s) Frequency (Hz) Frequence (Hz) v(t) V(f) w(t) W(f) <W(f) (rad/pi Time (s).4 F= Frequency (Hz) a=2, F=2-5 5 Time (s) Frequency (Hz) Frequence (Hz) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 3 /

26 Multiplication Example Convolution Parseval s u(t) = U(f) = a+i2πf e at t t < v(t) = cos2πft [from before] V(f) =.5(δ(f +F)+δ(f F)) w(t) = u(t)v(t) W(f) = U(f) V(f) =.5 a+i2π(f+f) +.5 a+i2π(f F) IfV(f) consists entirely of Dirac impulses thenu(f) V(f) iust replaces each impulse with a complete copy ofu(f) scaled by the area of the impulse and shifted so thathz lies on the impulse. Then add the overlapping complex spectra. u(t) U(f) <U(f) (rad/pi a= Time (s) Frequency (Hz) Frequence (Hz) v(t) V(f) w(t) W(f) <W(f) (rad/pi Time (s).4 F= Frequency (Hz) a=2, F=2-5 5 Time (s) Frequency (Hz) Frequence (Hz) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 3 /

27 Convolution Convolution Parseval s Convolution : w(t) = u(t)v(t) W(f) = U(f) V(f) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 4 /

28 Convolution Convolution Parseval s Convolution : w(t) = u(t)v(t) W(f) = U(f) V(f) w(t) = u(t) v(t) W(f) = U(f)V(f) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 4 /

29 Convolution Convolution Parseval s Convolution : w(t) = u(t)v(t) W(f) = U(f) V(f) w(t) = u(t) v(t) W(f) = U(f)V(f) Convolution in the time domain is equivalent to multiplication in the frequency domain and vice versa. E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 4 /

30 Convolution Convolution Parseval s Convolution : w(t) = u(t)v(t) W(f) = U(f) V(f) w(t) = u(t) v(t) W(f) = U(f)V(f) Convolution in the time domain is equivalent to multiplication in the frequency domain and vice versa. Proof of second line: Given u(t), v(t) and w(t) satisfying w(t) = u(t)v(t) W(f) = U(f) V(f) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 4 /

31 Convolution Convolution Parseval s Convolution : w(t) = u(t)v(t) W(f) = U(f) V(f) w(t) = u(t) v(t) W(f) = U(f)V(f) Convolution in the time domain is equivalent to multiplication in the frequency domain and vice versa. Proof of second line: Given u(t), v(t) and w(t) satisfying w(t) = u(t)v(t) W(f) = U(f) V(f) define dual waveforms x(t), y(t) and z(t) as follows: x(t) = U(t) X(f) = u( f) [duality] E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 4 /

32 Convolution Convolution Parseval s Convolution : w(t) = u(t)v(t) W(f) = U(f) V(f) w(t) = u(t) v(t) W(f) = U(f)V(f) Convolution in the time domain is equivalent to multiplication in the frequency domain and vice versa. Proof of second line: Given u(t), v(t) and w(t) satisfying w(t) = u(t)v(t) W(f) = U(f) V(f) define dual waveforms x(t), y(t) and z(t) as follows: x(t) = U(t) X(f) = u( f) y(t) = V(t) Y(f) = v( f) [duality] E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 4 /

33 Convolution Convolution Parseval s Convolution : w(t) = u(t)v(t) W(f) = U(f) V(f) w(t) = u(t) v(t) W(f) = U(f)V(f) Convolution in the time domain is equivalent to multiplication in the frequency domain and vice versa. Proof of second line: Given u(t), v(t) and w(t) satisfying w(t) = u(t)v(t) W(f) = U(f) V(f) define dual waveforms x(t), y(t) and z(t) as follows: x(t) = U(t) X(f) = u( f) y(t) = V(t) Y(f) = v( f) z(t) = W(t) Z(f) = w( f) [duality] E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 4 /

34 Convolution Convolution Parseval s Convolution : w(t) = u(t)v(t) W(f) = U(f) V(f) w(t) = u(t) v(t) W(f) = U(f)V(f) Convolution in the time domain is equivalent to multiplication in the frequency domain and vice versa. Proof of second line: Given u(t), v(t) and w(t) satisfying w(t) = u(t)v(t) W(f) = U(f) V(f) define dual waveforms x(t), y(t) and z(t) as follows: x(t) = U(t) X(f) = u( f) y(t) = V(t) Y(f) = v( f) z(t) = W(t) Z(f) = w( f) [duality] Now the convolution property becomes: w( f) = u( f)v( f) W(t) = U(t) V(t) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 4 /

35 Convolution Convolution Parseval s Convolution : w(t) = u(t)v(t) W(f) = U(f) V(f) w(t) = u(t) v(t) W(f) = U(f)V(f) Convolution in the time domain is equivalent to multiplication in the frequency domain and vice versa. Proof of second line: Given u(t), v(t) and w(t) satisfying w(t) = u(t)v(t) W(f) = U(f) V(f) define dual waveforms x(t), y(t) and z(t) as follows: x(t) = U(t) X(f) = u( f) y(t) = V(t) Y(f) = v( f) z(t) = W(t) Z(f) = w( f) [duality] Now the convolution property becomes: w( f) = u( f)v( f) W(t) = U(t) V(t) [subt ±f] E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 4 /

36 Convolution Convolution Parseval s Convolution : w(t) = u(t)v(t) W(f) = U(f) V(f) w(t) = u(t) v(t) W(f) = U(f)V(f) Convolution in the time domain is equivalent to multiplication in the frequency domain and vice versa. Proof of second line: Given u(t), v(t) and w(t) satisfying w(t) = u(t)v(t) W(f) = U(f) V(f) define dual waveforms x(t), y(t) and z(t) as follows: x(t) = U(t) X(f) = u( f) y(t) = V(t) Y(f) = v( f) z(t) = W(t) Z(f) = w( f) [duality] Now the convolution property becomes: w( f) = u( f)v( f) W(t) = U(t) V(t) [subt ±f] Z(f) = X(f)Y(f) z(t) = x(t) y(t) [duality] E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 4 /

37 Convolution Example Convolution Parseval s u(t) = t t < otherwise E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 5 /

38 Convolution Example Convolution Parseval s u(t) = t t < otherwise u(t).5 Time t (s) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 5 /

39 Convolution Example Convolution Parseval s u(t) = v(t) = t t < otherwise e t t t < u(t) Time t (s) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 5 /

40 Convolution Example Convolution Parseval s u(t) = v(t) = t t < otherwise e t t t < v(t) u(t) Time t (s) Time t (s) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 5 /

41 Convolution Example Convolution Parseval s u(t) = v(t) = t t < otherwise e t t t < v(t) u(t) Time t (s) Time t (s) w(t) = u(t) v(t) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 5 /

42 Convolution Example Convolution Parseval s u(t) = v(t) = t t < otherwise e t t t < v(t) u(t) Time t (s) Time t (s) w(t) = u(t) v(t) = u(τ)v(t τ)dτ E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 5 /

43 Convolution Example Convolution Parseval s u(t) = v(t) = t t < otherwise e t t t < v(t) u(t) Time t (s) Time t (s) w(t) = u(t) v(t) = u(τ)v(t τ)dτ = min(t,) ( τ)e τ t dτ E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 5 /

44 Convolution Example Convolution Parseval s u(t) = v(t) = t t < otherwise e t t t < v(t) u(t) Time t (s) Time t (s) w(t) = u(t) v(t) = u(τ)v(t τ)dτ = min(t,) ( τ)e τ t dτ = [(2 τ)e τ t ] min(t,) τ= E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 5 /

45 Convolution Example Convolution Parseval s u(t) = v(t) = t t < otherwise e t t t < v(t) u(t) Time t (s) Time t (s) w(t) = u(t) v(t) = u(τ)v(t τ)dτ = min(t,) ( τ)e τ t dτ = [(2 τ)e τ t ] min(t,) τ= t < = 2 t 2e t t < (e 2)e t t E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 5 /

46 Convolution Example Convolution Parseval s t t < u(t) = otherwise e t t v(t) = t < w(t) = u(t) v(t) = u(τ)v(t τ)dτ = min(t,) ( τ)e τ t dτ = [(2 τ)e τ t ] min(t,) τ= t < = 2 t 2e t t < (e 2)e t t u(t) v(t) w(t) Time t (s) Time t (s) Time t (s) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 5 /

47 Convolution Example Convolution Parseval s t t < u(t) = otherwise e t t v(t) = t < w(t) = u(t) v(t) = u(τ)v(t τ)dτ = min(t,) ( τ)e τ t dτ = [(2 τ)e τ t ] min(t,) τ= t < = 2 t 2e t t < (e 2)e t t u(t) v(t) w(t) = Time t (s) Time t (s) Time t (s) u(τ) v(.7-τ) t= Time τ (s) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 5 /

48 Convolution Example Convolution Parseval s t t < u(t) = otherwise e t t v(t) = t < w(t) = u(t) v(t) = u(τ)v(t τ)dτ = min(t,) ( τ)e τ t dτ = [(2 τ)e τ t ] min(t,) τ= t < = 2 t 2e t t < (e 2)e t t u(t) v(t) w(t) =.37.5 = Time t (s) Time t (s) Time t (s) u(τ) v(.7-τ) t= Time τ (s) u(τ) v(.5-τ) t= Time τ (s) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 5 /

49 Convolution Example Convolution Parseval s t t < u(t) = otherwise e t t v(t) = t < w(t) = u(t) v(t) = u(τ)v(t τ)dτ = min(t,) ( τ)e τ t dτ = [(2 τ)e τ t ] min(t,) τ= t < = 2 t 2e t t < (e 2)e t t u(t) v(t) w(t) =.37.5 =.6.5 = Time t (s) Time t (s) Time t (s) u(τ) v(.7-τ) t= Time τ (s) u(τ) v(.5-τ) t= Time τ (s) u(τ) v(2.5-τ) t= Time τ (s) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 5 /

50 Convolution Example Convolution Parseval s t t < u(t) = otherwise e t t v(t) = t < w(t) = u(t) v(t) = u(τ)v(t τ)dτ = min(t,) ( τ)e τ t dτ = [(2 τ)e τ t ] min(t,) τ= t < = 2 t 2e t t < (e 2)e t t u(t) v(t) w(t) =.37.5 =.6.5 = Time t (s) Time t (s) Time t (s) u(τ) v(.7-τ) t= Time τ (s) u(τ) v(.5-τ) t= Time τ (s) u(τ) v(2.5-τ) t= Time τ (s) Note howv(t τ) is time-reversed (because of the τ ) and time-shifted to put the time origin atτ = t. E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 5 /

51 Convolution Properties Convloution: w(t) = u(t) v(t) u(τ)v(t τ)dτ Convolution Parseval s E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 6 /

52 Convolution Properties Convolution Parseval s Convloution: w(t) = u(t) v(t) u(τ)v(t τ)dτ Convolution behaves algebraically like multiplication: ) Commutative: u(t) v(t) = v(t) u(t) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 6 /

53 Convolution Properties Convolution Parseval s Convloution: w(t) = u(t) v(t) u(τ)v(t τ)dτ Convolution behaves algebraically like multiplication: ) Commutative: u(t) v(t) = v(t) u(t) 2) Associative: u(t) v(t) w(t) = (u(t) v(t)) w(t) = u(t) (v(t) w(t)) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 6 /

54 Convolution Properties Convolution Parseval s Convloution: w(t) = u(t) v(t) u(τ)v(t τ)dτ Convolution behaves algebraically like multiplication: ) Commutative: u(t) v(t) = v(t) u(t) 2) Associative: u(t) v(t) w(t) = (u(t) v(t)) w(t) = u(t) (v(t) w(t)) 3) Distributive over addition: w(t) (u(t)+v(t)) = w(t) u(t)+w(t) v(t) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 6 /

55 Convolution Properties Convolution Parseval s Convloution: w(t) = u(t) v(t) u(τ)v(t τ)dτ Convolution behaves algebraically like multiplication: ) Commutative: u(t) v(t) = v(t) u(t) 2) Associative: u(t) v(t) w(t) = (u(t) v(t)) w(t) = u(t) (v(t) w(t)) 3) Distributive over addition: w(t) (u(t)+v(t)) = w(t) u(t)+w(t) v(t) 4) Identity Element or : u(t) δ(t) = δ(t) u(t) = u(t) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 6 /

56 Convolution Properties Convolution Parseval s Convloution: w(t) = u(t) v(t) u(τ)v(t τ)dτ Convolution behaves algebraically like multiplication: ) Commutative: u(t) v(t) = v(t) u(t) 2) Associative: u(t) v(t) w(t) = (u(t) v(t)) w(t) = u(t) (v(t) w(t)) 3) Distributive over addition: w(t) (u(t)+v(t)) = w(t) u(t)+w(t) v(t) 4) Identity Element or : u(t) δ(t) = δ(t) u(t) = u(t) 5) Bilinear: (au(t)) (bv(t)) = ab(u(t) v(t)) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 6 /

57 Convolution Properties Convolution Parseval s Convloution: w(t) = u(t) v(t) u(τ)v(t τ)dτ Convolution behaves algebraically like multiplication: ) Commutative: u(t) v(t) = v(t) u(t) 2) Associative: u(t) v(t) w(t) = (u(t) v(t)) w(t) = u(t) (v(t) w(t)) 3) Distributive over addition: w(t) (u(t)+v(t)) = w(t) u(t)+w(t) v(t) 4) Identity Element or : u(t) δ(t) = δ(t) u(t) = u(t) 5) Bilinear: (au(t)) (bv(t)) = ab(u(t) v(t)) Proof: In the frequency domain, convolution is multiplication. E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 6 /

58 Convolution Properties Convolution Parseval s Convloution: w(t) = u(t) v(t) u(τ)v(t τ)dτ Convolution behaves algebraically like multiplication: ) Commutative: u(t) v(t) = v(t) u(t) 2) Associative: u(t) v(t) w(t) = (u(t) v(t)) w(t) = u(t) (v(t) w(t)) 3) Distributive over addition: w(t) (u(t)+v(t)) = w(t) u(t)+w(t) v(t) 4) Identity Element or : u(t) δ(t) = δ(t) u(t) = u(t) 5) Bilinear: (au(t)) (bv(t)) = ab(u(t) v(t)) Proof: In the frequency domain, convolution is multiplication. Also, ifu(t) v(t) = w(t), then 6) Time Shifting: u(t+a) v(t+b) = w(t+a+b) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 6 /

59 Convolution Properties Convolution Parseval s Convloution: w(t) = u(t) v(t) u(τ)v(t τ)dτ Convolution behaves algebraically like multiplication: ) Commutative: u(t) v(t) = v(t) u(t) 2) Associative: u(t) v(t) w(t) = (u(t) v(t)) w(t) = u(t) (v(t) w(t)) 3) Distributive over addition: w(t) (u(t)+v(t)) = w(t) u(t)+w(t) v(t) 4) Identity Element or : u(t) δ(t) = δ(t) u(t) = u(t) 5) Bilinear: (au(t)) (bv(t)) = ab(u(t) v(t)) Proof: In the frequency domain, convolution is multiplication. Also, ifu(t) v(t) = w(t), then 6) Time Shifting: u(t+a) v(t+b) = w(t+a+b) 7) Time Scaling: u(at) v(at) = a w(at) How to recognise a convolution integral: the arguments ofu( ) andv( ) sum to a constant. E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 6 /

60 Parseval s Convolution Parseval s Lemma: X(f) = δ(f g) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 7 /

61 Parseval s Convolution Parseval s Lemma: X(f) = δ(f g) x(t) = δ(f g)e i2πft df E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 7 /

62 Parseval s Convolution Parseval s Lemma: X(f) = δ(f g) x(t) = δ(f g)e i2πft df = e i2πgt E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 7 /

63 Parseval s Convolution Parseval s Lemma: X(f) = δ(f g) x(t) = δ(f g)e i2πft df = e i2πgt X(f) = e i2πgt e i2πft dt E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 7 /

64 Parseval s Convolution Parseval s Lemma: X(f) = δ(f g) x(t) = δ(f g)e i2πft df = e i2πgt X(f) = e i2πgt e i2πft dt= e i2π(g f)t dt E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 7 /

65 Parseval s Convolution Parseval s Lemma: X(f) = δ(f g) x(t) = δ(f g)e i2πft df = e i2πgt X(f) = e i2πgt e i2πft dt= e i2π(g f)t dt= δ(g f) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 7 /

66 Parseval s Convolution Parseval s Lemma: X(f) = δ(f g) x(t) = δ(f g)e i2πft df = e i2πgt X(f) = e i2πgt e i2πft dt= e i2π(g f)t dt= δ(g f) Parseval s : t= u (t)v(t)dt = + f= U (f)v(f)df E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 7 /

67 Parseval s Convolution Parseval s Lemma: X(f) = δ(f g) x(t) = δ(f g)e i2πft df = e i2πgt X(f) = e i2πgt e i2πft dt= e i2π(g f)t dt= δ(g f) Parseval s : t= u (t)v(t)dt = + f= U (f)v(f)df Proof: Letu(t) = + f= U(f)ei2πft df and v(t) = + g= V(g)ei2πgt dg E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 7 /

68 Parseval s Convolution Parseval s Lemma: X(f) = δ(f g) x(t) = δ(f g)e i2πft df = e i2πgt X(f) = e i2πgt e i2πft dt= e i2π(g f)t dt= δ(g f) Parseval s : t= u (t)v(t)dt = + f= U (f)v(f)df Proof: Letu(t) = + f= U(f)ei2πft df and v(t) = + g= V(g)ei2πgt dg Now multiplyu (t) = u(t) andv(t) together and integrate over time: E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 7 /

69 Parseval s Convolution Parseval s Lemma: X(f) = δ(f g) x(t) = δ(f g)e i2πft df = e i2πgt X(f) = e i2πgt e i2πft dt= e i2π(g f)t dt= δ(g f) Parseval s : t= u (t)v(t)dt = + f= U (f)v(f)df Proof: Letu(t) = + f= U(f)ei2πft df and v(t) = + g= V(g)ei2πgt dg Now multiplyu (t) = u(t) andv(t) together and integrate over time: t= u (t)v(t)dt E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 7 /

70 Parseval s Convolution Parseval s Lemma: X(f) = δ(f g) x(t) = δ(f g)e i2πft df = e i2πgt X(f) = e i2πgt e i2πft dt= e i2π(g f)t dt= δ(g f) Parseval s : t= u (t)v(t)dt = + f= U (f)v(f)df Proof: Letu(t) = + f= U(f)ei2πft df and v(t) = + g= V(g)ei2πgt dg [Note use of different dummy variables] Now multiplyu (t) = u(t) andv(t) together and integrate over time: t= u (t)v(t)dt = t= + f= U (f)e i2πft df + g= V(g)ei2πgt dgdt E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 7 /

71 Parseval s Convolution Parseval s Lemma: X(f) = δ(f g) x(t) = δ(f g)e i2πft df = e i2πgt X(f) = e i2πgt e i2πft dt= e i2π(g f)t dt= δ(g f) Parseval s : t= u (t)v(t)dt = + f= U (f)v(f)df Proof: Letu(t) = + f= U(f)ei2πft df and v(t) = + g= V(g)ei2πgt dg [Note use of different dummy variables] Now multiplyu (t) = u(t) andv(t) together and integrate over time: t= u (t)v(t)dt = t= + f= U (f)e i2πft df + g= V(g)ei2πgt dgdt = + f= U (f) + g= V(g) t= ei2π(g f)t dtdgdf E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 7 /

72 Parseval s Convolution Parseval s Lemma: X(f) = δ(f g) x(t) = δ(f g)e i2πft df = e i2πgt X(f) = e i2πgt e i2πft dt= e i2π(g f)t dt= δ(g f) Parseval s : t= u (t)v(t)dt = + f= U (f)v(f)df Proof: Letu(t) = + f= U(f)ei2πft df and v(t) = + g= V(g)ei2πgt dg [Note use of different dummy variables] Now multiplyu (t) = u(t) andv(t) together and integrate over time: t= u (t)v(t)dt = t= + f= U (f)e i2πft df + g= V(g)ei2πgt dgdt = + f= U (f) + g= V(g) t= ei2π(g f)t dtdgdf = + f= U (f) + V(g)δ(g f)dgdf g= [lemma] E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 7 /

73 Parseval s Convolution Parseval s Lemma: X(f) = δ(f g) x(t) = δ(f g)e i2πft df = e i2πgt X(f) = e i2πgt e i2πft dt= e i2π(g f)t dt= δ(g f) Parseval s : t= u (t)v(t)dt = + f= U (f)v(f)df Proof: Letu(t) = + f= U(f)ei2πft df and v(t) = + g= V(g)ei2πgt dg [Note use of different dummy variables] Now multiplyu (t) = u(t) andv(t) together and integrate over time: t= u (t)v(t)dt = t= + f= U (f)e i2πft df + g= V(g)ei2πgt dgdt = + f= U (f) + g= V(g) t= ei2π(g f)t dtdgdf = + f= U (f) + V(g)δ(g f)dgdf g= [lemma] = + f= U (f)v(f)df E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 7 /

74 Energy Conservation Parseval s : t= u (t)v(t)dt = + f= U (f)v(f)df Convolution Parseval s E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 8 /

75 Energy Conservation Convolution Parseval s Parseval s : t= u (t)v(t)dt = + f= U (f)v(f)df For the special case v(t) = u(t), Parseval s theorem becomes: t= u (t)u(t)dt = + f= U (f)u(f)df E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 8 /

76 Energy Conservation Convolution Parseval s Parseval s : t= u (t)v(t)dt = + f= U (f)v(f)df For the special case v(t) = u(t), Parseval s theorem becomes: t= u (t)u(t)dt = + f= U (f)u(f)df E u = t= u(t) 2 dt = + f= U(f) 2 df E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 8 /

77 Energy Conservation Convolution Parseval s Parseval s : t= u (t)v(t)dt = + f= U (f)v(f)df For the special case v(t) = u(t), Parseval s theorem becomes: t= u (t)u(t)dt = + f= U (f)u(f)df E u = t= u(t) 2 dt = + f= U(f) 2 df Energy Conservation: The energy inu(t) equals the energy inu(f). E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 8 /

78 Energy Conservation Convolution Parseval s Parseval s : t= u (t)v(t)dt = + f= U (f)v(f)df For the special case v(t) = u(t), Parseval s theorem becomes: t= u (t)u(t)dt = + f= U (f)u(f)df E u = t= u(t) 2 dt = + f= U(f) 2 df Energy Conservation: The energy inu(t) equals the energy inu(f). Example: u(t) = e at t t < u(t) a= Time (s) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 8 /

79 Energy Conservation Convolution Parseval s Parseval s : t= u (t)v(t)dt = + f= U (f)v(f)df For the special case v(t) = u(t), Parseval s theorem becomes: t= u (t)u(t)dt = + f= U (f)u(f)df E u = t= u(t) 2 dt = + f= U(f) 2 df Energy Conservation: The energy inu(t) equals the energy inu(f). Example: u(t) = e at t t < E u = u(t) 2 dt = [ ] e 2at 2a u(t) a= Time (s) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 8 /

80 Energy Conservation Convolution Parseval s Parseval s : t= u (t)v(t)dt = + f= U (f)v(f)df For the special case v(t) = u(t), Parseval s theorem becomes: t= u (t)u(t)dt = + f= U (f)u(f)df E u = t= u(t) 2 dt = + f= U(f) 2 df Energy Conservation: The energy inu(t) equals the energy inu(f). Example: u(t) = e at t t < E u = u(t) 2 dt = [ ] e 2at 2a = 2a u(t) a= Time (s) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 8 /

81 Energy Conservation Convolution Parseval s Parseval s : t= u (t)v(t)dt = + f= U (f)v(f)df For the special case v(t) = u(t), Parseval s theorem becomes: t= u (t)u(t)dt = + f= U (f)u(f)df E u = t= u(t) 2 dt = + f= U(f) 2 df Energy Conservation: The energy inu(t) equals the energy inu(f). Example: u(t) = e at t t < E u = u(t) 2 dt = [ ] e 2at 2a = 2a U(f) = a+i2πf [from before] u(t) U(f) a= Time (s) Frequency (Hz) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 8 /

82 Energy Conservation Convolution Parseval s Parseval s : t= u (t)v(t)dt = + f= U (f)v(f)df For the special case v(t) = u(t), Parseval s theorem becomes: t= u (t)u(t)dt = + f= U (f)u(f)df E u = t= u(t) 2 dt = + f= U(f) 2 df Energy Conservation: The energy inu(t) equals the energy inu(f). Example: u(t) = e at t t < E u = u(t) 2 dt = [ ] e 2at 2a = 2a U(f) = a+i2πf U(f) 2 df = [from before] u(t) a=2.5 df -5 5 a 2 +4π 2 f 2 Time (s) U(f) Frequency (Hz) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 8 /

83 Energy Conservation Convolution Parseval s Parseval s : t= u (t)v(t)dt = + f= U (f)v(f)df For the special case v(t) = u(t), Parseval s theorem becomes: t= u (t)u(t)dt = + f= U (f)u(f)df E u = t= u(t) 2 dt = + f= U(f) 2 df Energy Conservation: The energy inu(t) equals the energy inu(f). Example: u(t) = e at t t < E u = u(t) 2 dt = [ ] e 2at 2a = 2a U(f) = a+i2πf U(f) 2 df = [ tan = ( 2πf a ) 2πa df a 2 +4π 2 f ] 2 [from before] u(t) U(f) a= Time (s) Frequency (Hz) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 8 /

84 Energy Conservation Convolution Parseval s Parseval s : t= u (t)v(t)dt = + f= U (f)v(f)df For the special case v(t) = u(t), Parseval s theorem becomes: t= u (t)u(t)dt = + f= U (f)u(f)df E u = t= u(t) 2 dt = + f= U(f) 2 df Energy Conservation: The energy inu(t) equals the energy inu(f). Example: u(t) = e at t t < E u = u(t) 2 dt = [ ] e 2at 2a = 2a U(f) = a+i2πf U(f) 2 df = [ tan = ( 2πf a ) 2πa df a 2 +4π 2 f ] 2 = π 2πa [from before] u(t) U(f) a= Time (s) Frequency (Hz) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 8 /

85 Energy Conservation Convolution Parseval s Parseval s : t= u (t)v(t)dt = + f= U (f)v(f)df For the special case v(t) = u(t), Parseval s theorem becomes: t= u (t)u(t)dt = + f= U (f)u(f)df E u = t= u(t) 2 dt = + f= U(f) 2 df Energy Conservation: The energy inu(t) equals the energy inu(f). Example: u(t) = e at t t < E u = u(t) 2 dt = [ ] e 2at 2a = 2a U(f) = a+i2πf U(f) 2 df = [ tan = ( 2πf a ) 2πa df a 2 +4π 2 f ] 2 [from before] = π 2πa = 2a u(t) U(f) a= Time (s) Frequency (Hz) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 8 /

86 Energy Spectrum Convolution Parseval s Example from before: w(t) = e at cos2πft t t < E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 9 /

87 Energy Spectrum Convolution Parseval s Example from before: w(t) = e at cos2πft t t < w(t) a=2, F=2-5 5 Time (s) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 9 /

88 Energy Spectrum Convolution Parseval s Example from before: w(t) = e at cos2πft t t < W(f) =.5 a+i2π(f+f) +.5 a+i2π(f F) w(t) a=2, F=2-5 5 Time (s) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 9 /

89 Energy Spectrum Convolution Parseval s Example from before: w(t) = e at cos2πft t t < W(f) =.5 a+i2π(f+f) +.5 a+i2π(f F) = a+i2πf a 2 +i4πaf 4π 2 (f 2 F 2 ) w(t) a=2, F=2-5 5 Time (s) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 9 /

90 Energy Spectrum Convolution Parseval s Example from before: w(t) = e at cos2πft t t < W(f) =.5 a+i2π(f+f) +.5 a+i2π(f F) = a+i2πf a 2 +i4πaf 4π 2 (f 2 F 2 ) w(t) W(f) <W(f) (rad/pi a=2, F=2-5 5 Time (s) Frequency (Hz) Frequence (Hz) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 9 /

91 Energy Spectrum Convolution Parseval s Example from before: w(t) = e at cos2πft t t < W(f) =.5 a+i2π(f+f) +.5 a+i2π(f F) = a+i2πf a 2 +i4πaf 4π 2 (f 2 F 2 ) w(t) W(f) <W(f) (rad/pi a=2, F=2-5 5 Time (s) Frequency (Hz) Frequence (Hz) W(f) 2 = a 2 +4π 2 f 2 (a 2 4π 2 (f 2 F 2 )) 2 +6π 2 a 2 f 2 E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 9 /

92 Energy Spectrum Convolution Parseval s Example from before: w(t) = e at cos2πft t t < W(f) =.5 a+i2π(f+f) +.5 a+i2π(f F) = W(f) 2 = a+i2πf a 2 +i4πaf 4π 2 (f 2 F 2 ) a 2 +4π 2 f 2 (a 2 4π 2 (f 2 F 2 )) 2 +6π 2 a 2 f 2 w(t) W(f) <W(f) (rad/pi W(f) a=2, F=2-5 5 Time (s) Frequency (Hz) Frequence (Hz) Frequency (Hz) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 9 /

93 Energy Spectrum Convolution Parseval s Example from before: w(t) = e at cos2πft t t < W(f) =.5 a+i2π(f+f) +.5 a+i2π(f F) = W(f) 2 = a+i2πf a 2 +i4πaf 4π 2 (f 2 F 2 ) a 2 +4π 2 f 2 (a 2 4π 2 (f 2 F 2 )) 2 +6π 2 a 2 f 2 w(t) W(f) <W(f) (rad/pi W(f) a=2, F=2-5 5 Time (s) Frequency (Hz) Frequence (Hz) Frequency (Hz) The units of W(f) 2 are energy per Hz so that its integral, E w = W(f) 2 df, has units of energy. E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 9 /

94 Energy Spectrum Convolution Parseval s Example from before: w(t) = e at cos2πft t t < W(f) =.5 a+i2π(f+f) +.5 a+i2π(f F) = W(f) 2 = a+i2πf a 2 +i4πaf 4π 2 (f 2 F 2 ) a 2 +4π 2 f 2 (a 2 4π 2 (f 2 F 2 )) 2 +6π 2 a 2 f 2 w(t) W(f) <W(f) (rad/pi W(f) a=2, F=2-5 5 Time (s) Frequency (Hz) Frequence (Hz) Frequency (Hz) Energy Spectrum The units of W(f) 2 are energy per Hz so that its integral, E w = W(f) 2 df, has units of energy. The quantity W(f) 2 is called the energy spectral density ofw(t) at frequency f and its graph is the energy spectrum ofw(t). E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 9 /

95 Energy Spectrum Convolution Parseval s Example from before: w(t) = e at cos2πft t t < W(f) =.5 a+i2π(f+f) +.5 a+i2π(f F) = W(f) 2 = a+i2πf a 2 +i4πaf 4π 2 (f 2 F 2 ) a 2 +4π 2 f 2 (a 2 4π 2 (f 2 F 2 )) 2 +6π 2 a 2 f 2 w(t) W(f) <W(f) (rad/pi W(f) a=2, F=2-5 5 Time (s) Frequency (Hz) Frequence (Hz) Frequency (Hz) Energy Spectrum The units of W(f) 2 are energy per Hz so that its integral, E w = W(f) 2 df, has units of energy. The quantity W(f) 2 is called the energy spectral density ofw(t) at frequency f and its graph is the energy spectrum ofw(t). It shows how the energy of w(t) is distributed over frequencies. E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 9 /

96 Energy Spectrum Convolution Parseval s Example from before: w(t) = e at cos2πft t t < W(f) =.5 a+i2π(f+f) +.5 a+i2π(f F) = W(f) 2 = a+i2πf a 2 +i4πaf 4π 2 (f 2 F 2 ) a 2 +4π 2 f 2 (a 2 4π 2 (f 2 F 2 )) 2 +6π 2 a 2 f 2 w(t) W(f) <W(f) (rad/pi W(f) a=2, F=2-5 5 Time (s) Frequency (Hz) Frequence (Hz) Frequency (Hz) Energy Spectrum The units of W(f) 2 are energy per Hz so that its integral, E w = W(f) 2 df, has units of energy. The quantity W(f) 2 is called the energy spectral density ofw(t) at frequency f and its graph is the energy spectrum ofw(t). It shows how the energy of w(t) is distributed over frequencies. If you divide W(f) 2 by the total energy,e w, the result is non-negative and integrates to unity like a probability distribution. E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 9 /

97 Summary Convolution Parseval s Convolution: u(t) v(t) u(τ)v(t τ)dτ E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 /

98 Summary Convolution Parseval s Convolution: u(t) v(t) u(τ)v(t τ)dτ Arguments ofu( ) andv( ) sum tot E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 /

99 Summary Convolution Parseval s Convolution: u(t) v(t) u(τ)v(t τ)dτ Arguments ofu( ) andv( ) sum tot Acts like multiplication + time scaling/shifting formulae E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 /

100 Summary Convolution Parseval s Convolution: u(t) v(t) u(τ)v(t τ)dτ Arguments ofu( ) andv( ) sum tot Acts like multiplication + time scaling/shifting formulae Convolution : multiplication convolution E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 /

101 Summary Convolution Parseval s Convolution: u(t) v(t) u(τ)v(t τ)dτ Arguments ofu( ) andv( ) sum tot Acts like multiplication + time scaling/shifting formulae Convolution : multiplication convolution w(t) = u(t)v(t) W(f) = U(f) V(f) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 /

102 Summary Convolution Parseval s Convolution: u(t) v(t) u(τ)v(t τ)dτ Arguments ofu( ) andv( ) sum tot Acts like multiplication + time scaling/shifting formulae Convolution : multiplication convolution w(t) = u(t)v(t) W(f) = U(f) V(f) w(t) = u(t) v(t) W(f) = U(f)V(f) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 /

103 Summary Convolution Parseval s Convolution: u(t) v(t) u(τ)v(t τ)dτ Arguments ofu( ) andv( ) sum tot Acts like multiplication + time scaling/shifting formulae Convolution : multiplication convolution w(t) = u(t)v(t) W(f) = U(f) V(f) w(t) = u(t) v(t) W(f) = U(f)V(f) Parseval s : t= u (t)v(t)dt = + f= U (f)v(f)df E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 /

104 Summary Convolution Parseval s Convolution: u(t) v(t) u(τ)v(t τ)dτ Arguments ofu( ) andv( ) sum tot Acts like multiplication + time scaling/shifting formulae Convolution : multiplication convolution w(t) = u(t)v(t) W(f) = U(f) V(f) w(t) = u(t) v(t) W(f) = U(f)V(f) Parseval s : t= u (t)v(t)dt = + f= U (f)v(f)df : E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 /

105 Summary Convolution Parseval s Convolution: u(t) v(t) u(τ)v(t τ)dτ Arguments ofu( ) andv( ) sum tot Acts like multiplication + time scaling/shifting formulae Convolution : multiplication convolution w(t) = u(t)v(t) W(f) = U(f) V(f) w(t) = u(t) v(t) W(f) = U(f)V(f) Parseval s : t= u (t)v(t)dt = + f= U (f)v(f)df : Energy spectral density: U(f) 2 (energy/hz) E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 /

106 Summary Convolution Parseval s Convolution: u(t) v(t) u(τ)v(t τ)dτ Arguments ofu( ) andv( ) sum tot Acts like multiplication + time scaling/shifting formulae Convolution : multiplication convolution w(t) = u(t)v(t) W(f) = U(f) V(f) w(t) = u(t) v(t) W(f) = U(f)V(f) Parseval s : t= u (t)v(t)dt = + f= U (f)v(f)df : Energy spectral density: U(f) 2 (energy/hz) Parseval: E u = u(t) 2 dt = U(f) 2 df E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 /

107 Summary Convolution Parseval s Convolution: u(t) v(t) u(τ)v(t τ)dτ Arguments ofu( ) andv( ) sum tot Acts like multiplication + time scaling/shifting formulae Convolution : multiplication convolution w(t) = u(t)v(t) W(f) = U(f) V(f) w(t) = u(t) v(t) W(f) = U(f)V(f) Parseval s : t= u (t)v(t)dt = + f= U (f)v(f)df : Energy spectral density: U(f) 2 (energy/hz) Parseval: E u = u(t) 2 dt = U(f) 2 df For further details see RHB Chapter 3. E. Fourier Series and Transforms ( ) Fourier Transform - Parseval and Convolution: 7 /

Lecture 8 ELE 301: Signals and Systems

Lecture 8 ELE 301: Signals and Systems Lecture 8 ELE 3: Signals and Systems Prof. Paul Cuff Princeton University Fall 2-2 Cuff (Lecture 7) ELE 3: Signals and Systems Fall 2-2 / 37 Properties of the Fourier Transform Properties of the Fourier

More information

EE 179 April 21, 2014 Digital and Analog Communication Systems Handout #16 Homework #2 Solutions

EE 179 April 21, 2014 Digital and Analog Communication Systems Handout #16 Homework #2 Solutions EE 79 April, 04 Digital and Analog Communication Systems Handout #6 Homework # Solutions. Operations on signals (Lathi& Ding.3-3). For the signal g(t) shown below, sketch: a. g(t 4); b. g(t/.5); c. g(t

More information

Review of Fourier series formulas. Representation of nonperiodic functions. ECE 3640 Lecture 5 Fourier Transforms and their properties

Review of Fourier series formulas. Representation of nonperiodic functions. ECE 3640 Lecture 5 Fourier Transforms and their properties ECE 3640 Lecture 5 Fourier Transforms and their properties Objective: To learn about Fourier transforms, which are a representation of nonperiodic functions in terms of trigonometric functions. Also, to

More information

5 Signal Design for Bandlimited Channels

5 Signal Design for Bandlimited Channels 225 5 Signal Design for Bandlimited Channels So far, we have not imposed any bandwidth constraints on the transmitted passband signal, or equivalently, on the transmitted baseband signal s b (t) I[k]g

More information

Lecture 18: The Time-Bandwidth Product

Lecture 18: The Time-Bandwidth Product WAVELETS AND MULTIRATE DIGITAL SIGNAL PROCESSING Lecture 18: The Time-Bandwih Product Prof.Prof.V.M.Gadre, EE, IIT Bombay 1 Introduction In this lecture, our aim is to define the time Bandwih Product,

More information

How To Understand The Discrete Fourier Transform

How To Understand The Discrete Fourier Transform The Fast Fourier Transform (FFT) and MATLAB Examples Learning Objectives Discrete Fourier transforms (DFTs) and their relationship to the Fourier transforms Implementation issues with the DFT via the FFT

More information

Class Note for Signals and Systems. Stanley Chan University of California, San Diego

Class Note for Signals and Systems. Stanley Chan University of California, San Diego Class Note for Signals and Systems Stanley Chan University of California, San Diego 2 Acknowledgement This class note is prepared for ECE 101: Linear Systems Fundamentals at the University of California,

More information

How To Understand The Nyquist Sampling Theorem

How To Understand The Nyquist Sampling Theorem Nyquist Sampling Theorem By: Arnold Evia Table of Contents What is the Nyquist Sampling Theorem? Bandwidth Sampling Impulse Response Train Fourier Transform of Impulse Response Train Sampling in the Fourier

More information

Chapter 8 - Power Density Spectrum

Chapter 8 - Power Density Spectrum EE385 Class Notes 8/8/03 John Stensby Chapter 8 - Power Density Spectrum Let X(t) be a WSS random process. X(t) has an average power, given in watts, of E[X(t) ], a constant. his total average power is

More information

9 Fourier Transform Properties

9 Fourier Transform Properties 9 Fourier Transform Properties The Fourier transform is a major cornerstone in the analysis and representation of signals and linear, time-invariant systems, and its elegance and importance cannot be overemphasized.

More information

Convolution, Correlation, & Fourier Transforms. James R. Graham 10/25/2005

Convolution, Correlation, & Fourier Transforms. James R. Graham 10/25/2005 Convolution, Correlation, & Fourier Transforms James R. Graham 10/25/2005 Introduction A large class of signal processing techniques fall under the category of Fourier transform methods These methods fall

More information

The Calculation of G rms

The Calculation of G rms The Calculation of G rms QualMark Corp. Neill Doertenbach The metric of G rms is typically used to specify and compare the energy in repetitive shock vibration systems. However, the method of arriving

More information

SGN-1158 Introduction to Signal Processing Test. Solutions

SGN-1158 Introduction to Signal Processing Test. Solutions SGN-1158 Introduction to Signal Processing Test. Solutions 1. Convolve the function ( ) with itself and show that the Fourier transform of the result is the square of the Fourier transform of ( ). (Hints:

More information

CHAPTER 7 APPLICATIONS TO MARKETING. Chapter 7 p. 1/54

CHAPTER 7 APPLICATIONS TO MARKETING. Chapter 7 p. 1/54 CHAPTER 7 APPLICATIONS TO MARKETING Chapter 7 p. 1/54 APPLICATIONS TO MARKETING State Equation: Rate of sales expressed in terms of advertising, which is a control variable Objective: Profit maximization

More information

Conceptual similarity to linear algebra

Conceptual similarity to linear algebra Modern approach to packing more carrier frequencies within agivenfrequencyband orthogonal FDM Conceptual similarity to linear algebra 3-D space: Given two vectors x =(x 1,x 2,x 3 )andy = (y 1,y 2,y 3 ),

More information

The continuous and discrete Fourier transforms

The continuous and discrete Fourier transforms FYSA21 Mathematical Tools in Science The continuous and discrete Fourier transforms Lennart Lindegren Lund Observatory (Department of Astronomy, Lund University) 1 The continuous Fourier transform 1.1

More information

ELE745 Assignment and Lab Manual

ELE745 Assignment and Lab Manual ELE745 Assignment and Lab Manual August 22, 2010 CONTENTS 1. Assignment 1........................................ 1 1.1 Assignment 1 Problems................................ 1 1.2 Assignment 1 Solutions................................

More information

Probability and Random Variables. Generation of random variables (r.v.)

Probability and Random Variables. Generation of random variables (r.v.) Probability and Random Variables Method for generating random variables with a specified probability distribution function. Gaussian And Markov Processes Characterization of Stationary Random Process Linearly

More information

Lecture 7: Finding Lyapunov Functions 1

Lecture 7: Finding Lyapunov Functions 1 Massachusetts Institute of Technology Department of Electrical Engineering and Computer Science 6.243j (Fall 2003): DYNAMICS OF NONLINEAR SYSTEMS by A. Megretski Lecture 7: Finding Lyapunov Functions 1

More information

CONTROLLABILITY. Chapter 2. 2.1 Reachable Set and Controllability. Suppose we have a linear system described by the state equation

CONTROLLABILITY. Chapter 2. 2.1 Reachable Set and Controllability. Suppose we have a linear system described by the state equation Chapter 2 CONTROLLABILITY 2 Reachable Set and Controllability Suppose we have a linear system described by the state equation ẋ Ax + Bu (2) x() x Consider the following problem For a given vector x in

More information

CONVOLUTION Digital Signal Processing

CONVOLUTION Digital Signal Processing CONVOLUTION Digital Signal Processing Introduction As digital signal processing continues to emerge as a major discipline in the field of electrical engineering an even greater demand has evolved to understand

More information

1.1 Discrete-Time Fourier Transform

1.1 Discrete-Time Fourier Transform 1.1 Discrete-Time Fourier Transform The discrete-time Fourier transform has essentially the same properties as the continuous-time Fourier transform, and these properties play parallel roles in continuous

More information

Lecture 7 ELE 301: Signals and Systems

Lecture 7 ELE 301: Signals and Systems Lecture 7 ELE 3: Signals and Systems Prof. Paul Cuff Princeton University Fall 2-2 Cuff (Lecture 7) ELE 3: Signals and Systems Fall 2-2 / 22 Introduction to Fourier Transforms Fourier transform as a limit

More information

From Fundamentals of Digital Communication Copyright by Upamanyu Madhow, 2003-2006

From Fundamentals of Digital Communication Copyright by Upamanyu Madhow, 2003-2006 Chapter Introduction to Modulation From Fundamentals of Digital Communication Copyright by Upamanyu Madhow, 003-006 Modulation refers to the representation of digital information in terms of analog waveforms

More information

SPECTRAL ANALYSIS OF PARABOLIC RANGE GATE PULL-OFF SIGNALS IN DIGITAL RADIO FREQUENCY MEMORY

SPECTRAL ANALYSIS OF PARABOLIC RANGE GATE PULL-OFF SIGNALS IN DIGITAL RADIO FREQUENCY MEMORY SPECTRAL ANALYSIS OF PARABOLIC RANGE GATE PULL-OFF SIGNALS IN DIGITAL RADIO FREQUENCY MEMORY A MASTER S THESIS in Electrical and Electronics Engineering Atilim University by MUSTAFA TALHA ÖZTÜRK JANUARY

More information

Experiment 3: Double Sideband Modulation (DSB)

Experiment 3: Double Sideband Modulation (DSB) Experiment 3: Double Sideband Modulation (DSB) This experiment examines the characteristics of the double-sideband (DSB) linear modulation process. The demodulation is performed coherently and its strict

More information

Linear Parameter Measurement (LPM)

Linear Parameter Measurement (LPM) (LPM) Module of the R&D SYSTEM FEATURES Identifies linear transducer model Measures suspension creep LS-fitting in impedance LS-fitting in displacement (optional) Single-step measurement with laser sensor

More information

Analysis/resynthesis with the short time Fourier transform

Analysis/resynthesis with the short time Fourier transform Analysis/resynthesis with the short time Fourier transform summer 2006 lecture on analysis, modeling and transformation of audio signals Axel Röbel Institute of communication science TU-Berlin IRCAM Analysis/Synthesis

More information

3.5.1 CORRELATION MODELS FOR FREQUENCY SELECTIVE FADING

3.5.1 CORRELATION MODELS FOR FREQUENCY SELECTIVE FADING Environment Spread Flat Rural.5 µs Urban 5 µs Hilly 2 µs Mall.3 µs Indoors.1 µs able 3.1: ypical delay spreads for various environments. If W > 1 τ ds, then the fading is said to be frequency selective,

More information

UNIVERSITY OF CALIFORNIA, SAN DIEGO Electrical & Computer Engineering Department ECE 101 - Fall 2010 Linear Systems Fundamentals

UNIVERSITY OF CALIFORNIA, SAN DIEGO Electrical & Computer Engineering Department ECE 101 - Fall 2010 Linear Systems Fundamentals UNIVERSITY OF CALIFORNIA, SAN DIEGO Electrical & Computer Engineering Department ECE 101 - Fall 2010 Linear Systems Fundamentals FINAL EXAM WITH SOLUTIONS (YOURS!) You are allowed one 2-sided sheet of

More information

PYKC Jan-7-10. Lecture 1 Slide 1

PYKC Jan-7-10. Lecture 1 Slide 1 Aims and Objectives E 2.5 Signals & Linear Systems Peter Cheung Department of Electrical & Electronic Engineering Imperial College London! By the end of the course, you would have understood: Basic signal

More information

Tables of Common Transform Pairs

Tables of Common Transform Pairs ble of Common rnform Pir 0 by Mrc Ph. Stoecklin mrc toecklin.net http://www.toecklin.net/ 0--0 verion v.5.3 Engineer nd tudent in communiction nd mthemtic re confronted with tion uch the -rnform, the ourier,

More information

UNIVERSITY OF CALIFORNIA, SAN DIEGO Electrical & Computer Engineering Department ECE 101 - Fall 2009 Linear Systems Fundamentals

UNIVERSITY OF CALIFORNIA, SAN DIEGO Electrical & Computer Engineering Department ECE 101 - Fall 2009 Linear Systems Fundamentals UNIVERSITY OF CALIFORNIA, SAN DIEGO Electrical & Computer Engineering Department ECE 101 - Fall 2009 Linear Systems Fundamentals MIDTERM EXAM You are allowed one 2-sided sheet of notes. No books, no other

More information

ORDINARY DIFFERENTIAL EQUATIONS

ORDINARY DIFFERENTIAL EQUATIONS ORDINARY DIFFERENTIAL EQUATIONS GABRIEL NAGY Mathematics Department, Michigan State University, East Lansing, MI, 48824. SEPTEMBER 4, 25 Summary. This is an introduction to ordinary differential equations.

More information

BSEE Degree Plan Bachelor of Science in Electrical Engineering: 2015-16

BSEE Degree Plan Bachelor of Science in Electrical Engineering: 2015-16 BSEE Degree Plan Bachelor of Science in Electrical Engineering: 2015-16 Freshman Year ENG 1003 Composition I 3 ENG 1013 Composition II 3 ENGR 1402 Concepts of Engineering 2 PHYS 2034 University Physics

More information

NRZ Bandwidth - HF Cutoff vs. SNR

NRZ Bandwidth - HF Cutoff vs. SNR Application Note: HFAN-09.0. Rev.2; 04/08 NRZ Bandwidth - HF Cutoff vs. SNR Functional Diagrams Pin Configurations appear at end of data sheet. Functional Diagrams continued at end of data sheet. UCSP

More information

SIGNAL PROCESSING & SIMULATION NEWSLETTER

SIGNAL PROCESSING & SIMULATION NEWSLETTER 1 of 10 1/25/2008 3:38 AM SIGNAL PROCESSING & SIMULATION NEWSLETTER Note: This is not a particularly interesting topic for anyone other than those who ar e involved in simulation. So if you have difficulty

More information

Waves in a short cable at low frequencies, or just hand-waving?

Waves in a short cable at low frequencies, or just hand-waving? Invited paper at the 23'rd International Conference on Noise and Fluctuations, 2015 Waves in a short cable at low frequencies, or just hand-waving? What does physics say? (Invited paper) L.B. Kish Department

More information

chapter Introduction to Digital Signal Processing and Digital Filtering 1.1 Introduction 1.2 Historical Perspective

chapter Introduction to Digital Signal Processing and Digital Filtering 1.1 Introduction 1.2 Historical Perspective Introduction to Digital Signal Processing and Digital Filtering chapter 1 Introduction to Digital Signal Processing and Digital Filtering 1.1 Introduction Digital signal processing (DSP) refers to anything

More information

Lecture 7 Circuit analysis via Laplace transform

Lecture 7 Circuit analysis via Laplace transform S. Boyd EE12 Lecture 7 Circuit analysis via Laplace transform analysis of general LRC circuits impedance and admittance descriptions natural and forced response circuit analysis with impedances natural

More information

Sensor Performance Metrics

Sensor Performance Metrics Sensor Performance Metrics Michael Todd Professor and Vice Chair Dept. of Structural Engineering University of California, San Diego mdtodd@ucsd.edu Email me if you want a copy. Outline Sensors as dynamic

More information

Lecture 10. Finite difference and finite element methods. Option pricing Sensitivity analysis Numerical examples

Lecture 10. Finite difference and finite element methods. Option pricing Sensitivity analysis Numerical examples Finite difference and finite element methods Lecture 10 Sensitivities and Greeks Key task in financial engineering: fast and accurate calculation of sensitivities of market models with respect to model

More information

TCOM 370 NOTES 99-4 BANDWIDTH, FREQUENCY RESPONSE, AND CAPACITY OF COMMUNICATION LINKS

TCOM 370 NOTES 99-4 BANDWIDTH, FREQUENCY RESPONSE, AND CAPACITY OF COMMUNICATION LINKS TCOM 370 NOTES 99-4 BANDWIDTH, FREQUENCY RESPONSE, AND CAPACITY OF COMMUNICATION LINKS 1. Bandwidth: The bandwidth of a communication link, or in general any system, was loosely defined as the width of

More information

Research Article Time-Frequency Analysis of Horizontal Vibration for Vehicle-Track System Based on Hilbert-Huang Transform

Research Article Time-Frequency Analysis of Horizontal Vibration for Vehicle-Track System Based on Hilbert-Huang Transform Hindawi Publishing Corporation Advances in Mechanical Engineering Volume 3, Article ID 954, 5 pages http://dx.doi.org/.55/3/954 Research Article Time-Frequency Analysis of Horizontal Vibration for Vehicle-Track

More information

Adding Sinusoids of the Same Frequency. Additive Synthesis. Spectrum. Music 270a: Modulation

Adding Sinusoids of the Same Frequency. Additive Synthesis. Spectrum. Music 270a: Modulation Adding Sinusoids of the Same Frequency Music 7a: Modulation Tamara Smyth, trsmyth@ucsd.edu Department of Music, University of California, San Diego (UCSD) February 9, 5 Recall, that adding sinusoids of

More information

ANALYZER BASICS WHAT IS AN FFT SPECTRUM ANALYZER? 2-1

ANALYZER BASICS WHAT IS AN FFT SPECTRUM ANALYZER? 2-1 WHAT IS AN FFT SPECTRUM ANALYZER? ANALYZER BASICS The SR760 FFT Spectrum Analyzer takes a time varying input signal, like you would see on an oscilloscope trace, and computes its frequency spectrum. Fourier's

More information

Periodic wave in spatial domain - length scale is wavelength Given symbol l y

Periodic wave in spatial domain - length scale is wavelength Given symbol l y 1.4 Periodic Waves Often have situations where wave repeats at regular intervals Electromagnetic wave in optical fibre Sound from a guitar string. These regularly repeating waves are known as periodic

More information

Spectrum Level and Band Level

Spectrum Level and Band Level Spectrum Level and Band Level ntensity, ntensity Level, and ntensity Spectrum Level As a review, earlier we talked about the intensity of a sound wave. We related the intensity of a sound wave to the acoustic

More information

1. Let X and Y be normed spaces and let T B(X, Y ).

1. Let X and Y be normed spaces and let T B(X, Y ). Uppsala Universitet Matematiska Institutionen Andreas Strömbergsson Prov i matematik Funktionalanalys Kurs: NVP, Frist. 2005-03-14 Skrivtid: 9 11.30 Tillåtna hjälpmedel: Manuella skrivdon, Kreyszigs bok

More information

Power Spectral Density

Power Spectral Density C H A P E R 0 Power Spectral Density INRODUCION Understanding how the strength of a signal is distributed in the frequency domain, relative to the strengths of other ambient signals, is central to the

More information

Systems with Persistent Memory: the Observation Inequality Problems and Solutions

Systems with Persistent Memory: the Observation Inequality Problems and Solutions Chapter 6 Systems with Persistent Memory: the Observation Inequality Problems and Solutions Facts that are recalled in the problems wt) = ut) + 1 c A 1 s ] R c t s)) hws) + Ks r)wr)dr ds. 6.1) w = w +

More information

VCO Phase noise. Characterizing Phase Noise

VCO Phase noise. Characterizing Phase Noise VCO Phase noise Characterizing Phase Noise The term phase noise is widely used for describing short term random frequency fluctuations of a signal. Frequency stability is a measure of the degree to which

More information

RESONANCE PASSAGE OF CYCLIC SYMMETRIC STRUCTURES

RESONANCE PASSAGE OF CYCLIC SYMMETRIC STRUCTURES 11 th International Conference on Vibration Problems Z. Dimitrovová et.al. (eds.) Lisbon, Portugal, 9 12 September 213 RESONANCE PASSAGE OF CYCLIC SYMMETRIC STRUCTURES Marius Bonhage* 1, Lars Panning-v.Scheidt

More information

T = 10-' s. p(t)= ( (t-nt), T= 3. n=-oo. Figure P16.2

T = 10-' s. p(t)= ( (t-nt), T= 3. n=-oo. Figure P16.2 16 Sampling Recommended Problems P16.1 The sequence x[n] = (-1)' is obtained by sampling the continuous-time sinusoidal signal x(t) = cos oot at 1-ms intervals, i.e., cos(oont) = (-1)", Determine three

More information

Fermi National Accelerator Laboratory. The Measurements and Analysis of Electromagnetic Interference Arising from the Booster GMPS

Fermi National Accelerator Laboratory. The Measurements and Analysis of Electromagnetic Interference Arising from the Booster GMPS Fermi National Accelerator Laboratory Beams-Doc-2584 Version 1.0 The Measurements and Analysis of Electromagnetic Interference Arising from the Booster GMPS Phil S. Yoon 1,2, Weiren Chou 1, Howard Pfeffer

More information

Time Domain and Frequency Domain Techniques For Multi Shaker Time Waveform Replication

Time Domain and Frequency Domain Techniques For Multi Shaker Time Waveform Replication Time Domain and Frequency Domain Techniques For Multi Shaker Time Waveform Replication Thomas Reilly Data Physics Corporation 1741 Technology Drive, Suite 260 San Jose, CA 95110 (408) 216-8440 This paper

More information

Frequency Response of FIR Filters

Frequency Response of FIR Filters Frequency Response of FIR Filters Chapter 6 This chapter continues the study of FIR filters from Chapter 5, but the emphasis is frequency response, which relates to how the filter responds to an input

More information

The integrating factor method (Sect. 2.1).

The integrating factor method (Sect. 2.1). The integrating factor method (Sect. 2.1). Overview of differential equations. Linear Ordinary Differential Equations. The integrating factor method. Constant coefficients. The Initial Value Problem. Variable

More information

Scalar Valued Functions of Several Variables; the Gradient Vector

Scalar Valued Functions of Several Variables; the Gradient Vector Scalar Valued Functions of Several Variables; the Gradient Vector Scalar Valued Functions vector valued function of n variables: Let us consider a scalar (i.e., numerical, rather than y = φ(x = φ(x 1,

More information

Lecture 3: Derivatives and extremes of functions

Lecture 3: Derivatives and extremes of functions Lecture 3: Derivatives and extremes of functions Lejla Batina Institute for Computing and Information Sciences Digital Security Version: spring 2011 Lejla Batina Version: spring 2011 Wiskunde 1 1 / 16

More information

6 J - vector electric current density (A/m2 )

6 J - vector electric current density (A/m2 ) Determination of Antenna Radiation Fields Using Potential Functions Sources of Antenna Radiation Fields 6 J - vector electric current density (A/m2 ) M - vector magnetic current density (V/m 2 ) Some problems

More information

Digital Transmission (Line Coding)

Digital Transmission (Line Coding) Digital Transmission (Line Coding) Pulse Transmission Source Multiplexer Line Coder Line Coding: Output of the multiplexer (TDM) is coded into electrical pulses or waveforms for the purpose of transmission

More information

Optimal Auctions. Jonathan Levin 1. Winter 2009. Economics 285 Market Design. 1 These slides are based on Paul Milgrom s.

Optimal Auctions. Jonathan Levin 1. Winter 2009. Economics 285 Market Design. 1 These slides are based on Paul Milgrom s. Optimal Auctions Jonathan Levin 1 Economics 285 Market Design Winter 29 1 These slides are based on Paul Milgrom s. onathan Levin Optimal Auctions Winter 29 1 / 25 Optimal Auctions What auction rules lead

More information

LECTURE 1: DIFFERENTIAL FORMS. 1. 1-forms on R n

LECTURE 1: DIFFERENTIAL FORMS. 1. 1-forms on R n LECTURE 1: DIFFERENTIAL FORMS 1. 1-forms on R n In calculus, you may have seen the differential or exterior derivative df of a function f(x, y, z) defined to be df = f f f dx + dy + x y z dz. The expression

More information

Fast-Fourier-Transform-Based Electrical Noise Measurements

Fast-Fourier-Transform-Based Electrical Noise Measurements Technische Universität München Fakultät für Physik Walther-Meißner-Institut für Tieftemperaturforschung Abschlussarbeit im Bachelorstudiengang Physik Fast-Fourier-Transform-Based Electrical Noise Measurements

More information

Manual for SOA Exam MLC.

Manual for SOA Exam MLC. Chapter 4. Life Insurance. c 29. Miguel A. Arcones. All rights reserved. Extract from: Arcones Manual for the SOA Exam MLC. Fall 29 Edition. available at http://www.actexmadriver.com/ c 29. Miguel A. Arcones.

More information

Lecture 1-6: Noise and Filters

Lecture 1-6: Noise and Filters Lecture 1-6: Noise and Filters Overview 1. Periodic and Aperiodic Signals Review: by periodic signals, we mean signals that have a waveform shape that repeats. The time taken for the waveform to repeat

More information

The Fourier Analysis Tool in Microsoft Excel

The Fourier Analysis Tool in Microsoft Excel The Fourier Analysis Tool in Microsoft Excel Douglas A. Kerr Issue March 4, 2009 ABSTRACT AD ITRODUCTIO The spreadsheet application Microsoft Excel includes a tool that will calculate the discrete Fourier

More information

The Black-Scholes pricing formulas

The Black-Scholes pricing formulas The Black-Scholes pricing formulas Moty Katzman September 19, 2014 The Black-Scholes differential equation Aim: Find a formula for the price of European options on stock. Lemma 6.1: Assume that a stock

More information

A characterization of trace zero symmetric nonnegative 5x5 matrices

A characterization of trace zero symmetric nonnegative 5x5 matrices A characterization of trace zero symmetric nonnegative 5x5 matrices Oren Spector June 1, 009 Abstract The problem of determining necessary and sufficient conditions for a set of real numbers to be the

More information

Fourier Analysis. u m, a n u n = am um, u m

Fourier Analysis. u m, a n u n = am um, u m Fourier Analysis Fourier series allow you to expand a function on a finite interval as an infinite series of trigonometric functions. What if the interval is infinite? That s the subject of this chapter.

More information

Linear Control Systems

Linear Control Systems Chapter 3 Linear Control Systems Topics : 1. Controllability 2. Observability 3. Linear Feedback 4. Realization Theory Copyright c Claudiu C. Remsing, 26. All rights reserved. 7 C.C. Remsing 71 Intuitively,

More information

2 The wireless channel

2 The wireless channel CHAPTER The wireless channel A good understanding of the wireless channel, its key physical parameters and the modeling issues, lays the foundation for the rest of the book. This is the goal of this chapter.

More information

OPTIMAL CONTROL OF A COMMERCIAL LOAN REPAYMENT PLAN. E.V. Grigorieva. E.N. Khailov

OPTIMAL CONTROL OF A COMMERCIAL LOAN REPAYMENT PLAN. E.V. Grigorieva. E.N. Khailov DISCRETE AND CONTINUOUS Website: http://aimsciences.org DYNAMICAL SYSTEMS Supplement Volume 2005 pp. 345 354 OPTIMAL CONTROL OF A COMMERCIAL LOAN REPAYMENT PLAN E.V. Grigorieva Department of Mathematics

More information

Time Series Analysis: Introduction to Signal Processing Concepts. Liam Kilmartin Discipline of Electrical & Electronic Engineering, NUI, Galway

Time Series Analysis: Introduction to Signal Processing Concepts. Liam Kilmartin Discipline of Electrical & Electronic Engineering, NUI, Galway Time Series Analysis: Introduction to Signal Processing Concepts Liam Kilmartin Discipline of Electrical & Electronic Engineering, NUI, Galway Aims of Course To introduce some of the basic concepts of

More information

Degenerated operator equations of higher order L. Tepoyan November 14, 1 Introduction The main object of the present paper is the dierential{operator equation L u (;1) m D m t (t D m t u)+ad m;1 t (t ;1

More information

Short-time FFT, Multi-taper analysis & Filtering in SPM12

Short-time FFT, Multi-taper analysis & Filtering in SPM12 Short-time FFT, Multi-taper analysis & Filtering in SPM12 Computational Psychiatry Seminar, FS 2015 Daniel Renz, Translational Neuromodeling Unit, ETHZ & UZH 20.03.2015 Overview Refresher Short-time Fourier

More information

FUNDAMENTALS OF ENGINEERING (FE) EXAMINATION REVIEW

FUNDAMENTALS OF ENGINEERING (FE) EXAMINATION REVIEW FE: Electric Circuits C.A. Gross EE1-1 FUNDAMENTALS OF ENGINEERING (FE) EXAMINATION REIEW ELECTRICAL ENGINEERING Charles A. Gross, Professor Emeritus Electrical and Comp Engineering Auburn University Broun

More information

it is easy to see that α = a

it is easy to see that α = a 21. Polynomial rings Let us now turn out attention to determining the prime elements of a polynomial ring, where the coefficient ring is a field. We already know that such a polynomial ring is a UF. Therefore

More information

Methods for Vibration Analysis

Methods for Vibration Analysis . 17 Methods for Vibration Analysis 17 1 Chapter 17: METHODS FOR VIBRATION ANALYSIS 17 2 17.1 PROBLEM CLASSIFICATION According to S. H. Krandall (1956), engineering problems can be classified into three

More information

Introduction to Frequency Domain Processing 1

Introduction to Frequency Domain Processing 1 MASSACHUSETTS INSTITUTE OF TECHNOLOGY DEPARTMENT OF MECHANICAL ENGINEERING 2.151 Advanced System Dynamics and Control Introduction to Frequency Domain Processing 1 1 Introduction - Superposition In this

More information

Payment streams and variable interest rates

Payment streams and variable interest rates Chapter 4 Payment streams and variable interest rates In this chapter we consider two extensions of the theory Firstly, we look at payment streams A payment stream is a payment that occurs continuously,

More information

Worksheet 1. What You Need to Know About Motion Along the x-axis (Part 1)

Worksheet 1. What You Need to Know About Motion Along the x-axis (Part 1) Worksheet 1. What You Need to Know About Motion Along the x-axis (Part 1) In discussing motion, there are three closely related concepts that you need to keep straight. These are: If x(t) represents the

More information

Network Theory Question Bank

Network Theory Question Bank Network Theory Question Bank Unit-I JNTU SYLLABUS: Three Phase Circuits Three phase circuits: Phase sequence Star and delta connection Relation between line and phase voltages and currents in balanced

More information

Chapter 29 Alternating-Current Circuits

Chapter 29 Alternating-Current Circuits hapter 9 Alternating-urrent ircuits onceptual Problems A coil in an ac generator rotates at 6 Hz. How much time elapses between successive emf values of the coil? Determine the oncept Successive s are

More information

1.(6pts) Find symmetric equations of the line L passing through the point (2, 5, 1) and perpendicular to the plane x + 3y z = 9.

1.(6pts) Find symmetric equations of the line L passing through the point (2, 5, 1) and perpendicular to the plane x + 3y z = 9. .(6pts Find symmetric equations of the line L passing through the point (, 5, and perpendicular to the plane x + 3y z = 9. (a x = y + 5 3 = z (b x (c (x = ( 5(y 3 = z + (d x (e (x + 3(y 3 (z = 9 = y 3

More information

1 Norms and Vector Spaces

1 Norms and Vector Spaces 008.10.07.01 1 Norms and Vector Spaces Suppose we have a complex vector space V. A norm is a function f : V R which satisfies (i) f(x) 0 for all x V (ii) f(x + y) f(x) + f(y) for all x,y V (iii) f(λx)

More information

MATH 425, PRACTICE FINAL EXAM SOLUTIONS.

MATH 425, PRACTICE FINAL EXAM SOLUTIONS. MATH 45, PRACTICE FINAL EXAM SOLUTIONS. Exercise. a Is the operator L defined on smooth functions of x, y by L u := u xx + cosu linear? b Does the answer change if we replace the operator L by the operator

More information

Section IV.21. The Field of Quotients of an Integral Domain

Section IV.21. The Field of Quotients of an Integral Domain IV.21 Field of Quotients 1 Section IV.21. The Field of Quotients of an Integral Domain Note. This section is a homage to the rational numbers! Just as we can start with the integers Z and then build the

More information

Semester 2, Unit 4: Activity 21

Semester 2, Unit 4: Activity 21 Resources: SpringBoard- PreCalculus Online Resources: PreCalculus Springboard Text Unit 4 Vocabulary: Identity Pythagorean Identity Trigonometric Identity Cofunction Identity Sum and Difference Identities

More information

Phasors. Phasors. by Prof. Dr. Osman SEVAİOĞLU Electrical and Electronics Engineering Department. ^ V cos (wt + θ) ^ V sin (wt + θ)

Phasors. Phasors. by Prof. Dr. Osman SEVAİOĞLU Electrical and Electronics Engineering Department. ^ V cos (wt + θ) ^ V sin (wt + θ) V cos (wt θ) V sin (wt θ) by Prof. Dr. Osman SEVAİOĞLU Electrical and Electronics Engineering Department EE 209 Fundamentals of Electrical and Electronics Engineering, Prof. Dr. O. SEVAİOĞLU, Page 1 Vector

More information

Lab 1. The Fourier Transform

Lab 1. The Fourier Transform Lab 1. The Fourier Transform Introduction In the Communication Labs you will be given the opportunity to apply the theory learned in Communication Systems. Since this is your first time to work in the

More information

Signal Detection C H A P T E R 14 14.1 SIGNAL DETECTION AS HYPOTHESIS TESTING

Signal Detection C H A P T E R 14 14.1 SIGNAL DETECTION AS HYPOTHESIS TESTING C H A P T E R 4 Signal Detection 4. SIGNAL DETECTION AS HYPOTHESIS TESTING In Chapter 3 we considered hypothesis testing in the context of random variables. The detector resulting in the minimum probability

More information

Properties of Real Numbers

Properties of Real Numbers 16 Chapter P Prerequisites P.2 Properties of Real Numbers What you should learn: Identify and use the basic properties of real numbers Develop and use additional properties of real numbers Why you should

More information

Test for I-DEAS FEATURES APPLICATIONS 83-0056-000 14A TRANSIENT POST-PROCESSING SOFTWARE FOR FIXED SAMPLE ORDER TRACKING

Test for I-DEAS FEATURES APPLICATIONS 83-0056-000 14A TRANSIENT POST-PROCESSING SOFTWARE FOR FIXED SAMPLE ORDER TRACKING 83-0056-000 14A Test for I-DEAS TRANSIENT POST-PROCESSING SOFTWARE FOR FIXED SAMPLE ORDER TRACKING FEATURES Advanced User Interface Providing Ease-of-Use In Post-Processing Time History Data Real-Time

More information

CONTINUOUS-TIME MODEL IDENTIFICATION USING REINITIALIZED PARTIAL MOMENTS - APPLICATION TO POWER AMPLIFIER MODELING

CONTINUOUS-TIME MODEL IDENTIFICATION USING REINITIALIZED PARTIAL MOMENTS - APPLICATION TO POWER AMPLIFIER MODELING CONINUOUS-IME MODEL IDENIFICAION USING REINIIALIZED PARIAL MOMENS - APPLICAION O POWER AMPLIFIER MODELING Régis Ouvrard Mourad Djamai Smail Bachir Jean-Claude rigeassou LAII-ESIP, Bâtiment de Mécanique,

More information

Section 3.7. Rolle s Theorem and the Mean Value Theorem. Difference Equations to Differential Equations

Section 3.7. Rolle s Theorem and the Mean Value Theorem. Difference Equations to Differential Equations Difference Equations to Differential Equations Section.7 Rolle s Theorem and the Mean Value Theorem The two theorems which are at the heart of this section draw connections between the instantaneous rate

More information

Sampling Theorem Notes. Recall: That a time sampled signal is like taking a snap shot or picture of signal periodically.

Sampling Theorem Notes. Recall: That a time sampled signal is like taking a snap shot or picture of signal periodically. Sampling Theorem We will show that a band limited signal can be reconstructed exactly from its discrete time samples. Recall: That a time sampled signal is like taking a snap shot or picture of signal

More information

THE CENTRAL LIMIT THEOREM TORONTO

THE CENTRAL LIMIT THEOREM TORONTO THE CENTRAL LIMIT THEOREM DANIEL RÜDT UNIVERSITY OF TORONTO MARCH, 2010 Contents 1 Introduction 1 2 Mathematical Background 3 3 The Central Limit Theorem 4 4 Examples 4 4.1 Roulette......................................

More information