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International Journal of Microwave Science and Technology
VolumeΒ 2012Β (2012), Article IDΒ 865625, 4 pages
http://dx.doi.org/10.1155/2012/865625
Research Article

Invariance Property of the πœ‡ Stability Test with respect to the Characteristic Impedance

1Electronics Engineering Department, American University in Cairo, Cairo, Egypt
2Army Research Laboratory, Adelphi, MD 20783, USA

Received 21 December 2011; Revised 18 February 2012; Accepted 20 February 2012

Academic Editor: Chien-JenΒ Wang

Copyright Β© 2012 Amr A. Ibrahim et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

Abstract

Stability of electrical amplifiers is of crucial importance. Among the popular stability tests is the ΞΌ-test which has many advantages over other tests like the K-Ξ” test. However, the value of ΞΌ parameter is dependent on the input/output terminal characteristic impedance π‘π‘œ used and this raises the concern that the predictions of the test are dependent on the choice of π‘π‘œ. This paper proves that the conclusions of the ΞΌ-test regarding stability/instability remain invariant with π‘π‘œ. This proof is necessary for gaining confidence in the results of the ΞΌ-test and should benefit circuit designers. Similar proofs should be extended to all other stability tests for additional insights into their validity under different circuit termination.

1. Introduction

The stability of a microwave amplifier, or equivalently its resistance to oscillations, is one of the main concerns when designing active microwave circuits. This classical problem of stability of linear two-port network has been intensively investigated in the technical literature over the last fifty years [1–7]. Several sets of conditions were proposed to check stability. All these sets of conditions, which were derived by steady state analysis, have been shown to be equivalent [1–6]. These tests determine whether it is possible to find a set of passive terminations that will cause the terminated two-port network to have unstable poles given that the network parameters do not have right-hand poles (Rollett’s proviso) [3]. If there are no such terminations, the two-port network is unconditionally stable. Among these tests, the most popular are the 𝐾-Ξ” test [3] and the ΞΌ-test [5]. These two tests are widely used in many CAD programs and textbooks discussing the design of both amplifiers as well as oscillators [8, 9]. The 𝐾-Ξ” relies on two conditions to assess the stability of microwave amplifiers. On the other hand, the ΞΌ-test relies only on one parameter to assess the stability of the amplifier circuit. Usually, the ΞΌ-test is calculated from the 𝑆-parameters of the circuits under test. However, in circuits composed of lumped components, the choice of π‘π‘œ is ambiguous and hence the ΞΌ-test value may change based on the value of π‘π‘œ. In this paper, it is proven that the ΞΌ-test result does not depend on the choice π‘π‘œ, as long as π‘π‘œ takes real positive values. Meaning that if the circuit is stable for a certain π‘π‘œ then it will be also stable for any other π‘π‘œ (i.e., ΞΌ value will always be greater than one), and vice versa. Moreover, it is shown that the worst case condition (ΞΌ value  ~ 1) will occur, when π‘π‘œ tends to zero or infinity. One of the benefits of this analysis is that the ΞΌ-test can also be applied to circuits composed of lumped components with arbitrary π‘π‘œ.

Some stability tests that vary with π‘π‘œ can yield misleading results. For example, a common oscillation test is to evaluate the round trip gain |Ξ“inΓ𝑆|. The test requires that |Ξ“inΓ𝑆| > 1 for oscillations [9], where Ξ“in is the input reflection coefficient of the oscillator circuit and Γ𝑆 is the source reflection coefficient as shown in Figure 1. Suppose we have a negative resistance oscillator with input impedance of βˆ’25 + j10 Ohm and source impedance of 50 βˆ’ j10 Ohm. Then |Ξ“inΓ𝑆| may be plotted, as a function of π‘π‘œ as in Figure 2. It is clear that |Ξ“inΓ𝑆|> 1 for small values of π‘π‘œ, and |Ξ“inΓ𝑆| < 1 otherwise. The variance of |Ξ“inΓ𝑆| with π‘π‘œ makes the test’s conclusions questionable. Thus, the invariance of a stability test with π‘π‘œ is crucial and cannot be assumed without a proof. This paper addresses this concern for the popular ΞΌ-test.

865625.fig.001
Figure 1: The amplifier circuit.
865625.fig.002
Figure 2: The round trip gain |Ξ“inΓ𝑆| as a function of π‘π‘œ used in the evaluation of Ξ“in and Γ𝑆.

2. Mathematical Treatment

In this section, it is proven that the ΞΌ-test does not depend on the choice of π‘π‘œ of terminal ports. It is convenient to start the proof from the impedance domain (𝑍) since it does not depend on the choice of π‘π‘œ. For an amplifier circuit to be stable (according to the ΞΌ-test), the condition||Ξ“in||<1(1) must be satisfied for any passive load termination (𝑍𝐿) [5]. The ΞΌ-test defines a parameter, ΞΌ, such that1πœ‡=||Ξ“max||,(2) where |Ξ“max| is the maximum reflection coefficient (for any possible load). If |Ξ“max| < 1, then the network is stable, ΞΌ is greater than 1, and no negative impedances can be produced, and vice versa.

The input impedance of the amplifier circuit is given by𝑍in=𝑍11βˆ’π‘12𝑍21𝑍𝐿+𝑍22=𝑍11𝑍𝐿+Δ𝑍𝑍𝐿+𝑍22,(3) where Δ𝑍 is the determinant of the impedance matrix.

Equation (3) has the form of a bilinear transformation. The bilinear transformation is a complex mapping technique and has the property of mapping circles in one domain into circles in another domain with lines as the limiting case. Under this transformation, the imaginary axis in the 𝑍𝐿 domain (Re(𝑍𝐿)=0) is mapped into a circle in the 𝑍in domain as shown in Figure 3 with centre 𝐢in and radius 𝑅in given by𝐢in=2𝑍11𝑍Re22ξ€Έβˆ’π‘12𝑍21𝑍2Re22ξ€Έ,𝑅in=||||𝑍12𝑍21𝑍2Re22ξ€Έ||||.(4) For the amplifier to be absolutely stable, the mapped circle in the 𝑍in domain must lie completely in the right half plane or𝐢Reinξ€Έ>𝑅in.(5) Furthermore, the greater the inequality Re(𝐢in)>𝑅in, the higher the stability. In the previous equation, it was assumed that the region (Re(𝑍𝐿)>0) is mapped to the interior of the circle in the 𝑍in domain which will happen given that the condition (Re(𝑍22)>0) is satisfied.

865625.fig.003
Figure 3: Mapping from the (𝑍𝐿) impedance plane into 𝑍in plane followed by mapping into Ξ“in plane.

Now assuming that (5) is satisfied and the amplifier is absolutely stable in the 𝑍in domain, one can map this circle to the Ξ“in domain using the bilinear transformation𝑍in=π‘π‘œΞ“in+π‘π‘œβˆ’Ξ“in.+1(6) For a circle having a centre (𝐢in) and radius (𝑅in) in the 𝑍in domain, the mapped circle in the Ξ“in domain will have a center (𝐢Γ) and radius (𝑅Γ) given by𝐢Γ=||𝐢in||2βˆ’π‘…2inβˆ’π‘2π‘œ+𝑗2π‘π‘œξ€·πΆIminξ€Έ||𝐢in||2βˆ’π‘…2in+𝑍2π‘œ+2π‘π‘œξ€·πΆReinξ€Έ,𝑅Γ=2𝑅inπ‘π‘œ||𝐢in||2βˆ’π‘…2in+𝑍2π‘œ+2π‘π‘œξ€·πΆReinξ€Έ.(7) Since the interior of the circle in the 𝑍in domain is mapped to the interior of the circle in the Ξ“in domain, (1) can be rewritten as||𝐢Γ||+𝑅Γ<1.(8) To check this condition, define𝐢in=π‘Ž+𝑗𝑏.(9) From (5), one can writeπ‘Ž2=𝑅2in+𝛿2,(10) where 𝛿2>0 is a parameter that can indicate higher stability. Substituting with (10) in (7), one can write||𝐢Γ||+𝑅Γ=𝑏2+𝛿2+𝑍2π‘œξ€Έ2βˆ’ξ€·2π›Ώπ‘π‘œξ€Έ2+2𝑅inπ‘π‘œξ€·π‘2+𝛿2+𝑍2π‘œξ€Έ+2π‘Žπ‘π‘œ.(11) In this case, the ΞΌ-test is simply the inverse of the previous expression. Thus, based on (2),1πœ‡=||𝐢Γ||+𝑅Γ=𝑏2+𝛿2+𝑍2π‘œξ€Έ+2π‘Žπ‘π‘œξ”ξ€·π‘2+𝛿2+𝑍2π‘œξ€Έ2βˆ’ξ€·2π›Ώπ‘π‘œξ€Έ2+2𝑅inπ‘π‘œ.(12) The value of the previous expression is always greater than 1 given that (5) is satisfied irrespective of the value of π‘π‘œ. That is because the first term in the numerator is greater than the first term in the denominator, and the same is true for the second term in the numerator and denominator. Also, at the stability edge in the 𝑍in domain where 𝛿→0, the value of ΞΌ will approach 1. It should be noted that the value of ΞΌ will also approach 1 in the limiting case as π‘π‘œ approaches zero or infinity. The previous steps of the proof are summarized in Figure 3.

3. Verification of Theory Using Two Examples

Two examples are given to validate the previous results. The first example is for an unconditionally stable amplifier and the second one is for a conditionally stable amplifier. First, consider the parameters of an amplifier circuit in the 𝑍-domain at certain frequency (π‘“π‘œ) as𝑍amp=⎑⎒⎒⎣⎀βŽ₯βŽ₯⎦,36βˆ’π‘—241.5βˆ’π‘—4βˆ’15βˆ’π‘—58520βˆ’π‘—28(13) which corresponds to the following 𝑆-parameters (in a 50-Ohms system):𝑆amp=⎑⎒⎒⎣0.1βˆ βˆ’10.5∘0.05βˆ βˆ’46.5∘7βˆ βˆ’68.5∘0.15βˆ βˆ’112.7∘⎀βŽ₯βŽ₯⎦.(14) For this amplifier, the ΞΌ-test, given by (15), is calculated for different values of π‘π‘œ and the result is shown in Figure 4(a),||π‘†πœ‡=1βˆ’11||2|||𝑆22βˆ’Ξ”π‘†π‘†11|||+||𝑆12𝑆21||,(15) where Δ𝑆 is determinant of the 𝑆-parameters matrix, and the upper bar indicates conjugation. It is clear from Figure 4(a) that the value of ΞΌ is always greater than 1 and it approaches 1 as π‘π‘œ tends to zero or infinity. The same conclusion can be obtained by observing the mapped circles of the region (Re(𝑍𝐿)>0) in the Ξ“in domain as a function of π‘π‘œ (Figure 5(a)), where all the mapped circles are located inside the unity circle (|Ξ“in|=1). Now consider a second case where the amplifier 𝑍-parameters are changed to𝑍amp=⎑⎒⎒⎣⎀βŽ₯βŽ₯⎦1.8βˆ’π‘—310.87βˆ’π‘—8.4βˆ’115.6βˆ’π‘—373.3βˆ’9.4βˆ’π‘—30.6(16) which corresponds to the following 𝑆-parameters (in a 50-Ohms system):𝑆amp=⎑⎒⎒⎣0.1βˆ βˆ’11.3∘0.15βˆ βˆ’45.9∘7βˆ βˆ’68.8∘0.15βˆ βˆ’114.7∘⎀βŽ₯βŽ₯⎦.(17) The ΞΌ-test as a function of π‘π‘œ is shown in Figure 4(b). As the figure indicates, the value of ΞΌ is less than 1, irrespective of π‘π‘œ. Also, Figure 5(b) shows that the mapped circles of the region (Re(𝑍𝐿)>0) in the Ξ“in domain intersect with the unity circle at all values of π‘π‘œ. The previous two examples illustrate the application of the theory.

fig4
Figure 4: ΞΌ-test as a function of π‘π‘œ for (a) unconditionally stable amplifier and (b) conditionally stable amplifier.
fig5
Figure 5: Mapped circles in the Ξ“in domain for (a) unconditionally stable amplifier and (b) conditionally stable amplifier.

4. Conclusion

One of the most popular tests for stability is the ΞΌ-test due to its simplicity (one parameter, instead of two) and its ability to indicate relative stability. This paper proves that the conclusions reached through the ΞΌ-test are invariant with characteristic impedance π‘π‘œ choices. This proof is necessary for using the ΞΌ-test with confidence. A stability test which does not meet this condition may lead to inaccurate conclusions. Two examples illustrating the application of the theory were provided.

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