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scZoUnD [109]
3 years ago
8

Use the convolutional integral to find the response of an LTI system with impulse response ℎ(????) and input x(????). Sketch the

output signal. a) x(????) = ????(????) and ℎ(????) = ????????(????) b) x(????) = ????????c???? ( ???? 2???? ) and ℎ(????) = exp(−????????) ????(????) (You may write ????????c???? ( ???? 2???? ) as ????(???? + ????) − ????(???? − ????).)
Engineering
1 answer:
Thepotemich [5.8K]3 years ago
8 0

Answer:

Use the convolution integral to determine the output of an LTI system with impulse response h(t) to input x(t) specified below.

h(t) = 4e^-6t-1 u(t+1) x(t)=2u(t – 2)

Explanation:

y(t)=∫0th(t−λ)f(λ)dλ

Start with a linear time-invariant (LTI) system (in box).  There is an input to the system, x(t), and an output from the system, y(t).

Now consider the same system with the input as an impulse, δ(t).  The output is then, by definition, the impulse response, h(t).

If we use a delayed impulse into the system, the output is just the impulse response with the same delay.

Because of linearity, if we scale the input by any factor, the output will be scaled by the same factor.  In particular, we can scale the input (and hence the output) by the factor x(λ)dλ.

If we integrate the input, the output is also integrated.  In this case we'll take the upper limit of the integration to be t+; but it could just as well have been positive infinity.  We could also take the lower lower limit to be negative infinity.

By the sifting property of the impulse function we know that (if λ>0, t>0):

     

∫0tδ(t−λ)x(λ)dλ=x(t)

Therefore the input to the system is x(t)

If the input is x(t), then the output must be y(t) (by definition, from the first diagram).  

Equating the outputs of the last two diagrams leads directly to the convolution theorem:

y(t)=∫0th(t−λ)f(λ)dλ

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A 75 ! coaxial transmission line has a length of 2.0 cm and is terminated with a load impedance of 37.5 j75 !. If the relative p
Cerrena [4.2K]

Answer:

4.26

Explanation:

The wavelength λ is given by:

\lambda=v/f=c/nf\\c=speed\ of\ light=3*10^8m/s,f=frequency=3*10^9Hz,n=permittivity=2.56\\\\\lambda=3*10^8/(2.56*3*10^9)=0.0625\ m\\

Phase constant (β) = 2π/λ

βl = 2π/λ × l

l = 2 cm = 0.02 m

βl = 2π/0.0625 × 0.02=2.01 rad = 115.3°

1 rad = 180/π degrees

Z_L=load\ impedance=37.5+j75\\\\Z_o=characteristic impedance = 75\ ohm\\\\\tilde {Z_L}=Z_L/Z_o=37.5+j75/75=0.5+j

\tilde {Z_{in}}=\frac{\tilde {Z_{L}}+jtan\beta l}{1+j\tilde {Z_{L}}tan\beta l}=\frac{0.5+j+jtan(115.2)}{1+j(0.5+j)tan(115.2)}=0.253-j0.274\\  \\Z_{in}=Z_o\tilde {Z_{in}}=75(0.253-j0.274)=19-j20.5\\\\\Gamma_L=\frac{Z_L-Z_0}{Z_L+Z_o}=\frac{37.5+j75-75}{37.5+j75+75}=0.62\angle 83^o\\\\\Gamma_{in}=\frac{Z_{in}-Z_0}{Z_{in}+Z_o}=\frac{19-j20.5-75}{19-j20.5+75}=0.62\angle -147^o\\\\VSWR=\frac{1+\rho}{1-\rho} =\frac{1+0.62}{1-0.62}=4.26

6 0
3 years ago
Consider a steady developing laminar flow of water in a constant-diameter horizontal discharge pipe attached to a tank. The flui
dalvyx [7]

Answer:

hello attached is the free body diagram of the missing figure

Fr = \frac{\pi }{4} D^2 [ ( P1 - P2) - pV^2 ]

Explanation:

Average velocity is constant i.e V1 = V2 = V

The momentum equation for the flow in the Z - direction can be expressed as

-Fr + P1 Ac - P2 Ac = mB2V2 - mB1V1 ------- equation 1

Fr = horizontal force on the bolts

P1 = pressure of fluid at entrance

V1 = velocity of fluid at entrance

Ac = cross section area of the pipe

P2 and V2 = pressure and velocity of fluid at some distance

m = mass flow rate of fluid

B1 = momentum flux at entrance , B2 = momentum flux correction factor

Note; average velocity is constant hence substitute V for V1 and V2

equation 1 becomes

Fr = ( P1 - P2 ) Ac + mV ( 1 - 2 )

Fr = ( P1 - P2 ) Ac - mV ---------------- equation 2

equation for mass flow rate

m = <em>p</em>AcV  

<em>p</em> = density of the fluid

insert this into equation 2 EQUATION 2 BECOMES

Fr = ( P1 - P2) Ac - <em>p</em>AcV^2

    = Ac [ (P1 - P2) - pV^2 ]  ---------- equation 3

Note Ac = \frac{\pi }{4} D^2

Equation 3 becomes

Fr = \frac{\pi }{4} D^2 [ (P1 -P2 ) - pV^2 ] ------- relation for the horizontal force acting on the bolts      

6 0
3 years ago
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