Sinusoidal Steady-state Analysis of Transmission Lines Flashcards

1
Q

steady state

A

transients have settled

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2
Q

Most RF signals are

A

Narrowband, their bandwidth is only 1-2% of their center frequency

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3
Q

Fourier analysis allows us to

A

extend to narrowband to wideband or baseband signals

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4
Q

Propagation constant

A

γ = α +jβ (1/m)

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5
Q

Attenuation constant

A

α (Np/m), the sine wave decays with α, measure of the attenuation of the amplitude of the fields in electromagnetic wave propagation

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6
Q

Phase constant

A

β (rad/m), 2pi/λ, As the wave moves forward, its phase may undergo variations, and this factor that indicates this variation

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7
Q

Attenuation increases with

A

frequency

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8
Q

Line attenuation

A

10log[Pin/Pout], 8.686αL (dB). Often quoted in dB/m

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9
Q

Lossless medium attenuation and phase

A

α = 0 and β = ω√L’C’

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10
Q

Standing wave cause

A

Counter propagating sine waves with different amplitudes and phases due to the reflection at the load will lead to standing waves on the line

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11
Q

Standing wave maximum

A

2βz + ∠ΓL = (2n)π

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12
Q

Standing wave minimum

A

2βz + ∠ΓL = (2n+1)π

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13
Q

VSWR

A

Voltage standing wave ratio, a real number that tells us how close we are to a match

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14
Q

Return Loss

A

-20log|ΓL| (dB)

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15
Q

Power delivered to the load

A

A fraction of the available power will be delivered to the load, the rest will be reflected and turned to heat in the transmission line, unless there is a perfect match

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16
Q

Power available at the load

A

(|V+|^2)/2Zo

17
Q

Wave impedance

A

the ratio of the voltage to current at any point along a (potentially mismatched) transmission line

18
Q

Distortion will occur on a transmission line unless

A

the antennation constant (amplitude distortion) and propagation speed (phase distortion) are independent of frequency.

19
Q

An infinite lossy line will appear

A

matched, but very little power may be reaching the load

20
Q

Impedance special cases

A

1) when d = nλ/2, tan(npi) = 0 We will see the load again Z(d) = ZL
2) when d = (2n+1)λ/4, tan() -> infinity and we have impedance inversion Z(d) = (Zo^2)/ZL
3) Short Circuit Load
4) Open Circuit Load

21
Q

Impedance of a quarter waveform transformer

A

Z0A = √Z0RL

22
Q

Short Circuit Stub

A
23
Q

Open Circuit Stub

A
24
Q

Distortion less conditon

A

R’/L’ = G’/C’