Abaque de Smith – Download as PDF File .pdf), Text File .txt) or read online. EXERCICE ABAQUE DE – Download as PDF File .pdf), Text File .txt) or read online. fr. abaque de Smith, m diagramme de Smith, m diagramme polaire d’impédance, m. représentation graphique en coordonnées polaires du facteur de réflexion.

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The choice of whether to use the Z Smith chart or the Y Smith chart for any particular calculation depends on which is more convenient.

Smith chart – Wikipedia

Capacitive admittances have positive imaginary parts dmith inductive admittances have negative imaginary parts. The length of the line would then be scaled to P 1 assuming abaquf Smith chart radius to be unity. Smith —[1] [2] is a graphical aid or nomogram designed for electrical and electronics engineers specializing in radio frequency RF engineering to assist in solving problems with transmission lines and matching circuits.

The Y Smith chart is constructed in a similar way to the Z Smith chart case but by expressing values of voltage reflection coefficient in terms of normalised admittance instead of normalised impedance.

The degrees scale represents the angle of the voltage reflection coefficient at that point. For each, the reflection coefficient is given in polar form together with the corresponding normalised impedance in rectangular form. If there were very different values of resistance present a value closer to these might be a better choice.

Alternatively, one type may be used and the scaling converted to the other when required.

This page was last edited on 15 Augustat Provided the frequencies are sufficiently close, the resulting Smith chart points may be joined by straight lines to create a locus. The following example shows how a transmission line, terminated with an arbitrary load, may be matched at one frequency either with a series or parallel reactive component in each case connected at precise positions.

For distributed components the effects on reflection coefficient and impedance of moving along the transmission line must be allowed for using the outer circumferential scale of the Smith chart which is calibrated in wavelengths.



Once a transformation from impedance to admittance has been performed, the scaling changes to normalised admittance until a later transformation back to normalised impedance is performed.

The accuracy of the Smith chart is reduced for problems involving a large locus of impedances or admittances, although the scaling can be magnified for individual areas to accommodate these.

Considering the point at infinity, the space of the new chart includes all possible loads. The magnitude of a complex number is the length of a straight line drawn from the origin to the point representing it. In order to change from normalised impedance to normalised admittance or vice versa, the point representing the value of reflection coefficient under consideration is moved through exactly degrees at the same radius.

As impedances and admittances change with frequency, problems using the Smith chart can only be solved manually using one frequency at a time, the result being represented by a point. The Smith chart may also be used for lumped element matching and analysis problems.

The normalised impedance Smith chart is composed of two families of circles: The region above the x -axis represents capacitive admittances and the region below the x -axis represents inductive admittances. While the use of paper Smith charts for solving the complex mathematics involved in matching problems has been largely replaced by software based methods, the Smith chart display is still the preferred method of displaying how RF parameters behave at one or more frequencies, an alternative to using tabular information.

The normalised admittance y T is the reciprocal of the normalised impedance z Tso.

Actual impedances and admittances must be normalised before using them on a Smith chart. In fact this value is not actually used. The Smith chart has circumferential scaling in wavelengths and degrees. In this case the wavelength scaling on the Smith chart circumference is not used. At point P 21 the circle intersects with the unity circle of constant normalised resistance at.

Reading from the Smith chart scaling, remembering xbaque this is now a normalised admittance sjith.

This occurs in microwave circuits and when high power requires large components in shortwave, FM and TV Broadcasting. By using this site, you agree to the Terms of Use and Privacy Policy. Substituting these into the equation relating abxque impedance and complex reflection coefficient:. Point Q 20 is the equivalent of P 20 but expressed as a normalised admittance.


Using the Smith chart, the normalised impedance may be obtained with appreciable accuracy by plotting the point representing the reflection coefficient treating the Smith chart as a polar diagram and then reading its value directly using the characteristic Smith chart scaling. Thus most RF circuit analysis software includes a Smith chart option for the display of results and all but abzque simplest impedance measuring instruments can display measured results on a Smith chart display.

This is the equation which describes how the complex reflection coefficient changes with the normalised impedance and may be used to construct both families of circles. In other projects Wikimedia Commons.

File:Smith chart bmd.gif

In RF abwque and matching problems sometimes it is more convenient to work with admittances representing conductances and susceptances and sometimes it is more convenient to work with impedances representing resistances and reactances. They both change with frequency so for any particular measurement, the frequency at which it was abawue must be stated together with the characteristic impedance.

The following table gives the complex expressions for baaque real and normalised and admittance real and normalised for each of the three basic passive circuit elements: The analysis of lumped element components assumes that the wavelength at the frequency of operation is much greater than the dimensions of the components themselves.

The path along the arc of the circle represents how the impedance changes whilst moving along the transmission line. Normalised impedance and normalised admittance are dimensionless. All terms are actually multiplied by this to obtain the instantaneous phasebut it is conventional and understood to omit it. If the termination was a perfect open circuit or short circuit abaqque magnitude of the reflection coefficient would be unity, all power would be reflected and the point would lie at some point on the unity circumference circle.

This is plotted on the Z Smith chart at point P