Ứng dụng đồ thị Smith để giải bài tập trường điện từ, siêu cao tần Điện tử viễn thông
Trang 2The Smith Chart: I plot in the Complex Plane
¢ Smith’s chart is a graphical representation in the complex I’ plane of the input impedance, the load impedance, and the reflection
coefficient I’ of a /oss-free TL ImL'
¢ it contains two families
of curves (circles) in
the complex I’ plane
¢ each circle corresponds
to a fixed normalized
resistance or reactance |
Rel
Trang 3
The Smith Chart: Normalized Impedance and I
relation #1: normalized load impedance z, and reflection I’
Trang 4The Smith Chart: Resistance and Reactance Circles
resistance circles reactance circles
let the abscissa be I’ and the ordinate be I’, (the I’ complex plane)
¢ resistance and reactance equations are circles in the I’
complex plane
¢ resistance circles have centers lying on the I axis (I; = 0 or ordinate = 0)
e reactance circles have centers with abscissa coordinate = 1
¢a complex normalized impedance z, =r, + jx, 1S a point on the Smith chart where the circle r, intersects the circle x,
Lecture 08: The Smith Chart 4
Trang 5The Smith Chart: Resistance Circles
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Trang 6The Smith Chart: Reactance Circles
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Trang 7The Smith Chart: Nomographs
at the bottom of Smith’s chart, a nomograph is added to determine
¢ SWR and SWR in dB, 20 log, SWR
¢ return loss in dB, —20log,o | T |
¢ power reflection |I|* (P)
¢ reflection coefficient |I| (E or J), etc
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Trang 8The Smith Chart: SWR Circles
> acircle of radius I’, centered
at I’ = 0 is the geometrical
place for load impedances
producing reflection of the
same magnitude, | I] =I,
Trang 9
The Smith Chart: Plotting Impedance and Reading Out I
Trang 10relation #2: input impedance versus the TL length L
>» on the Smith chart, the point corresponding to z,, is rotated by
—2L (decreasing angle, clockwise rotation) with respect to the point corresponding to z; along an SWR circle
> one full circle on the Smith chart is 2Z,,, = 27, 1.€., Lina = 2/23 this reflects the periodicity of z,,
Lecture 08: The Smith Chart 10
Trang 11The Smith Chart: Tracking Impedance Changes with L — 2
`
R for Z2 = 50 Q, the
transforms a load of Z¡=25- 725
Trang 12The Smith Chart: Read Out Distance to Load
Trang 13The Smith Chart: Reading Out SWR
Trang 14*® normalized load admittance
* the relation between y,„ and y; 1s the same as that between z,„ and z
— one can get from load to input terminals (and vice versa) by
following a circle clockwise (counter-clockwise)
¢ standard Smith chart gives resistance and reactance values
¢ admittance Smith chart is exactly the same as the “impedance” (or standard) Smith chart but rotated by 180° [see eq (*) and sl 17]
Lecture 08: The Smith Chart 14
Trang 15The Smith Chart: Admittance Interpretation — 2
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Trang 16The Smith Chart: Admittance Interpretation — 3
combined impedance and conductance Smith Chart
zy, (on impedance scales) 0}
: Ale
y,, (on admittance scales) 2}?
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16
Trang 17¢ impedance values from a standard Smith chart can be easily
converted to admittance (conductance + susceptance) values by
rotation along a circle of exactly 180°
¢ rotation by 180° on the impedance Smith chart corresponds to
impedance transformation by a quarter-wavelength "2 8: 4 - z)
¢ the value diametrically opposite on the Smith chart from
an impedance value is the respective “admittance” value
Lecture 08: The Smith Chart 17
Trang 18The Smith Chart: Admittance Interpretation — 5
Check whether in this
example the y, found
from the Smith chart
Trang 19>» in this case the TL must be designed to have this specific Z,
Lecture 08: The Smith Chart 19
Trang 20> the impedance match with the 4/4 transformer holds perfectly at one frequency only, fo, where L = 1,/4
> this impedance-match device is narrow-band
Trang 21Optimal Power Delivery: Review (Homework)
> at the generator’s terminals, a loaded TL is equivalently represented
by its input impedance Z.,
> active (or average) power delivered to the loaded TL (this is also
the powel delivered to the load Z, if the line is loss-free) ,
Trang 22> assume generator’s impedance Z,, = R, + jX, is known and fixed
> optimal matching is achieved when maximum active power 1s
delivered to the load Z,, — what is this optimal value of Z,,,?
Zi — Max Fin (Zin )
Lecture 08: The Smith Chart 22