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Published byHerbert Heath Modified over 9 years ago
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Power and power-gains are two main considerations in the design of a microwave transistor amplifier. To derive power and power-gains using traveling waves concept, we need to determine the reflection coefficients in the form of traveling waves and S parameters.
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the source and the load reflection coefficient in a Z 0 system are For the transistor, the input and output traveling waves measured in a Z 0 system are related by
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The concepts of a reflection coefficient and traveling waves can be used even if there are no transmission lines at port 1 and port 2. We can show that the input reflection coefficient
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For the output reflection coefficient:
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and can be shown in terms of S parameters as and where
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The power available from the source is equal to the input power when IN = S * and can be expressed as We can also express P IN in the form or P IN = P AVS M S
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where M S is the source mismatch factor which is equal to
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The power delivered to the load Z L is and can be shown in terms of S parameters as and where
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The power available from the network P AVN is equal to the power delivered to the load when L = OUT * and can be expressed as We can also express P L in the form or P L = P AVN M L
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where M L is the load mismatch factor which is equal to
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The power gain G P is given by The transducer power gain G T is given by
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Manipulating the denominator, G T can be also written in the form The unilateral power gain G TU is an often employed approximation for the transducer power gain. G TU which neglects the feedback effect of the amplifier (S 12 = 0) can be expressed as
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The available power gain G A can be expressed in the form
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,the input side of the amplifier is connected to a voltage source with E 1 = 10 V and source impedance Z S = 50 . The output is connected to a load which also has an impedance Z L = 50 , given find the following quantities: a) transducer power gain G T, unilateral transducer gain G TU, available power gain G A, and operating power gain G P. b) power delivered to the load P L, power available from the source P AVS, and input power P IN.
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In a two-port network, oscillations are possible when either input or output port represents a negative resistance. This occurs when or For a unilateral device (S 12 = 0), the oscillations occur when or.
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The two-port network is unconditionally stable if the real parts of Z IN and Z OUT are greater than zero for all passive load and source impedances. (1) (2) (3) (4) Note: all coefficients are normalized to the same characteristic impedance Z 0.
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This happens when some passive source and load terminations (some but not all values of S and L ) produce input and output impedances having a negative real part.
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The graphical analysis is useful in the analysis of potentially unstable transistors. First, the regions where values of S and L produce and are determined, respectively. The solutions for S and L lie on circles (called stability circles) whose equations are given by and
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The radii and centers of the circles where and in the L plane and S plane, respectively, are obtained, namely L values for (Output Stability Circle): radius center
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S values for (Input Stability Circle): radius center where = S 11 S 22 -S 12 S 21.
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(a) L plane (b) S plane
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The region where values of L (where ) produce are the stable regions.
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The region where values of S (where ) produce are the stable regions.
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K > 1 where and. or K > 1 and
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From practical point of view, most microwave transistors produced by manufacturers are either unconditionally stable or potentially unstable with 0< K < 1 and. Conditions for unconditionally stability for L plane and s plane.
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Determine the stability. If the transistor is potentially unstable at a given frequency, draw the input and output stability circles. f (GHz)S 11 S 12 S 21 S 22 0.5 1 2 4
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Even when the selection of S and L produces or, the circuit can be made stable if Re(Z S +Z IN ) > 0 and Re(Z L +Z OUT ) > 0 A potentially unstable transistor can be made unconditionally stable by either resistively loading the transistor or by adding negative feedback. These techniques are not recommended in narrowband amplifiers.
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