EE431/531 Microwave Circuit Design I: Lab 3
© B. Pejcinovic, P. Wong, O. Woywode

Introduction

This lab delves into the principles of amplifier design under the constraints of either maximum transducer gain or a specific operating power gain. In addition, the relationship between constant gain circles and the frequency is explored. You will also learn how to create a circuit layout in MDS.

Design Specifications

Single stage BJT amplifier

Figure 1: Block diagram of a single stage BJT amplifier

You are to design two different single-stage transistor amplifier circuits. For the first circuit, the design constraint is to achieve maximum transducer gain GT,max. In the second circuit, the amplifier must obtain a specified operating power gain Gp. The design frequency is f = 1 GHz.

The input matching network (IMN) and output matching network (OMN) are to be constructed from microstrip. The substrate is Duroid (relative permittivity = 2.23 and height H = 0.7874 mm). The matching networks should use balanced stubs (either open-circuited or short-circuited) and a series transmission line.

The core of the amplifier is a bipolar junction transistor (BJT) in common-emitter configuration. For this lab, the transistor is a Siemens BJT (MDS Part# "siemens_10bfq196_s"). This particular device is parameterized at a fixed bias of VCE = 5 V and IC = 70 mA.

Technically, the parameterized BJT does not need external biasing for simple S-parameter and gain measurements. However, you are required to design base and collector biasing circuits (including DC voltage sources) and add them to your amplifier. You may use high-impedance microstrip, inductors, and capacitors. Although the bias circuits do not actually power the parameterized BJT, they may still have an impact on the amplifier due to non-ideal component effects.

The input port of the BJT needs to be matched to a 50 ohm source, while the BJT's output port is to be matched to a 50 ohm load. In the actual circuit, the source and load impedances are represented by S-ports. Coupling capacitors should be placed between the source and the IMN, and also between the OMN and the load.

For a good example of what your completed amplifier circuit design might look like, refer to page 167 of the Gonzalez textbook (2nd edition).

Circuit Layout

If a circuit design is to be manufactured, then you need to create a layout for the circuit. The layout procedure converts a schematic drawing to a set of detailed instructions that tell how to arrange the circuit for actual fabrication. MDS has layout models for many circuit components, which are used to define and constrain the physical layout of the components. For devices with no built-in models, you can create your own definitions that describe how to perform the component layout.

In MDS, the layout procedure can be performed automatically or interactively. In auto-layout mode, MDS examines the schematic, applies the appropriate models, and then generates the circuit layout. This is convenient for the engineer, but the resulting layout might not conform to certain design guidelines (especially if the models are incomplete). In this case, interactive mode is appropriate. With the MDS layout editor, you can edit a layout to fix minor problems or even create new layouts from scratch.

When a circuit layout is produced, MDS creates a layout icon in the workbench. Double-clicking this icon opens its associated layout page. What you see on the layout page is a proportionally scaled view of how the circuit will be constructed.

When the layout is finished, it can be saved as a UNIX file and imported into special software that validates the layout. Once verified, the layout can be used as a guide to make PC boards or IC masks that implement the original circuit design.

Layout problems with the Siemens BJT

The Siemens 10bfq196_s BJT does not have a built-in layout model. If you attempt to perform an auto-layout of a schematic that contains the Siemens BJT, MDS will use a default component layout that makes no sense. To get around this problem, you will define a new layout model for the BJT.

If package specifications for the Siemens BJT were available, you could create a realistic layout that takes into account the actual dimensions of the device. Since we do not have that information, you will create a simplified BJT layout instead, which consists of a 70 mil diameter circle with four terminals in the proper orientation.

Creating a new BJT layout

Here is the procedure for creating the simplified BJT layout:

Layout procedure for the Siemens BJT

Figure 2: Step-by-step layout procedure for the Siemens BJT

Accessing the new BJT layout

You have to make a few changes to your circuit schematic in order to access the simplified layout. Essentially, you insert transistor attribute statements onto the circuit page which explicitly tell MDS to use the new 70mil layout instead of the default component layout. The procedure for doing this is outlined in the next section.


BJT Characteristics


Assignment

As the first step in the amplifier design, you will determine the characteristics of the Siemens BJT. From the resulting S-parameter data, you can instruct MDS to find the reflection coefficients for a bilateral simultaneous conjugate match and compute the corresponding maximum transducer gain. The test circuit consists of the BJT, two S-ports, and no matching or bias networks.

Circuit construction

BJT characterization test circuit

Figure 3: BJT characterization test circuit

Circuit layout

Simulation and output

Items to turn in

Questions

  1. Is the Siemens 10bfq196_s BJT unconditionally stable at the design frequency of 1 GHz? From the simulation results, explain why the transistor does not fulfill the unilateral criterion.
  2. Discuss the significance of the gains versus frequency plot.
  3. Determine the frequency at which the transistor becomes potentially unstable.
  4. Determine fbeta, fT, and fs. Explain why you are not asked to find fmax. (Refer to Fig. 1.11.10 in the textbook for definitions of these frequencies.)
  5. What is the maximum transducer gain at the design frequency? How does GT,max vary with frequency?

Amplifier Circuit 1: Designing for GT,max


Assignment

Using the Gamma_Ms and Gamma_ML values that were computed in the previous section, design the microstrip input and output matching networks of the amplifier to achieve maximum transducer gain (GT,max) at the 1 GHz design frequency.

Circuit construction

GTmax amplifier circuit

Figure 4: GT,max amplifier circuit

Here are some general hints that may be useful:

Circuit optimization

Before attaching the IMN and OMN subcircuits to the main amplifier circuit, test them individually first. Verify that the IMN transforms Gamma_Ms to the 50 ohm source and that the OMN transforms Gamma_ML to the 50 ohm load.

Use the MDS optimization feature to tune the matching networks at the design frequency. When you are done, the output port of the IMN should not deviate more than a few percent from the required Gamma_Ms value. Likewise, the input port of the OMN should be as close as possible to the required Gamma_ML value.

Tuning the IMN

IMN test circuit

Figure 5: IMN test circuit

IMPORTANT: After you have finished optimizing the IMN, you need to collect some S-parameter versus frequency data that will be used later in the lab. Follow this procedure:

Tuning the OMN

OMN test circuit

Figure 6: OMN test circuit

IMPORTANT: After you have finished optimizing the OMN, you need to collect some S-parameter versus frequency data that will be used later in the lab. Follow this procedure:

Circuit layout

Items to turn in


Amplifier Circuit 1: Using MDS to find GT vs. freq


Assignment

For the GT,max amplifier circuit, determine the transducer gain GT as a function of frequency. Compare GT and GT,max at the 1 GHz design frequency.

GT computation issues

At first glance, calculating the transducer gain using the equations in the textbook seems like a simple task. However, on closer examination, there are several subtle points that complicate the situation.

S-param & reflect. coeff. definitions for general amplifier

Figure 7: S-parameter and reflection coefficient definitions for a general amplifier

Figure 7 shows the reference positions for specific reflection coefficients as defined in the textbook. Notice that S11, S12, S21, and S22 are the S-parameters for the BJT. The transducer gain formula is

Equation (1)

Hence, to compute GT , all you need to do is plug in the correct S-parameters and values.

So what is the problem? Well, there are actually two potential difficulties:

  1. The transducer gain equation is implicitly dependent on the frequency. For each frequency at which you want to compute GT , you must re-measure the BJT S-parameters and the reflection coefficients and then plug those new values into the gain equation.
  2. In MDS, S-ports cannot be inserted between circuit blocks. They can only be placed on the input and output ports of the overall circuit. Figure 8 illustrates this situation. Notice that in the prime reference system, the S-parameters are for the overall circuit and not for the BJT alone.

How MDS calculates S-params and reflection coefficients

Figure 8: How MDS calculates S-parameters and Gamma values.

In the prime reference system, the transducer gain equation is now

Equation (2)

In a 50 ohm system, Gamma_s' = 0 and Gamma_L' = 0. Equation (2) then reduces to GT' = |S21'|2. Surprisingly, GT' is equal to GT (refer to your lecture notes for an explanation of why this is so). In this section, you will examine the transducer gain versus frequency relationship using both equation (1) and (2).

Computing GT using equation (1)

In this approach, the overall amplifier circuit is broken down into three separate test circuits - IMN, BJT, and OMN. S-parameters and reflection coefficients are computed as a function of frequency for each test circuit separately, and the resulting values are used in equation (1) to find GT.

EQ1: How to find Gamma_s vs frequency

EQ1: How to find the BJT S-parameters vs frequency

EQ1: How to find Gamma_L vs frequency

EQ1: How to find GT vs frequency

Now that you have all the necessary data, how do you extract the required values to compute GT using equation (1)? In addition to evaluating equations on a circuit page, MDS also has the capability of defining equations on a display page (i.e., a presentation page). You can create new variables from scratch, or you can access data (such as S-parameters) that are stored in different simulation datasets. Of course, you can also perform standard mathematical operations on the variables.

s11x=DS_BJT.sim1.SP.S[1,1]
s12x=DS_BJT.sim1.SP.S[1,2]
s21x=DS_BJT.sim1.SP.S[2,1]
s22x=DS_BJT.sim1.SP.S[2,2]

Gamma_S=DS_IMN.sim1.SP.S[2,2]
Gamma_L=DS_OMN.sim1.SP.S[1,1]
Gamma_IN=s11x+((s12x*s21x*Gamma_L)/(1-s22x*Gamma_L))

G1=(1-(mag(Gamma_S))^2)/(mag(1-Gamma_IN*Gamma_S))^2
G2=(mag(s21x))^2
G3=(1-(mag(Gamma_L))^2)/(mag(1-s22x*Gamma_L))^2

GT=G1*G2*G3
GT_dB=10*log(GT)

Figure 9: Equations for calculating GT

Figure 9 shows the equations that you need to enter on the presentation page. The variable names s11, s12, s21, and s22 are reserved in MDS, so you have to use slightly different names. Unlike equations on a circuit page, there is no special EQUATION statement that precedes equations on a presentation page.

Notice the syntax for assigning data from a dataset to a variable name. For example, the variable s11x accesses a data array (S[1,1]) of type S-parameter (SP) from simulation 1 (sim1) within an external dataset (DS_BJT). It is important to realize that the defined variables do not contain just a single value, but an entire array of values (one value for each frequency tested). MDS performs mathematical operations on variables on an element-by-element basis. Therefore, the variable GT_dB is an array that contains the computed transducer gain at each tested frequency.

To add the equations in Figure 9 to a presentation page, follow this procedure:

EQ1: Items to turn in

EQ1: Questions

  1. What is the transducer gain GT at the design frequency? How does GT vary with frequency?
  2. Does the computed value for GT equal GT,max (to within a few percent) at 1 GHz?

Computing GT' using equation (2)

For this approach, you use the S-parameter values of the overall circuit in conjunction with equation (2) to compute . As a reminder, GT' = |S21'|2.

EQ2: How to find G'T vs frequency

EQ2: Items to turn in

EQ2: Questions

  1. What is the value of GT' at the design frequency?
  2. Does the computed value for GT' equal GT,max (to within a few percent) at 1 GHz?
  3. From your simulations, does the value of GT' (computed from eqn (2)) equal the value of GT (computed from eqn (1)) at each frequency?

Amplifier Circuit 2: Designing for Gp


Assignment

In this part of the lab, you need to re-design your microstrip matching networks to obtain a specific operating power gain (Gp) at the design frequency. The requirements are a) Gp = 16 dB, b) magnitude of Gamma_L is minimized, and c) GT = Gp.

Circuit construction

Circuit layout

Items to turn in


Amplifier Circuit 2: Using MDS to verify GT = Gp


Finding GT

Items to turn in

How to find Gp at the design frequency

Gp test circuit

Figure 10: Gp test circuit

Figure 10 is the schematic used to determine Gp. Notice that the IMN circuit is not included in the overall circuit. The equation for the operating power gain is:

Equation (3)

In a 50 ohm system, Gamma_L' = 0. This means equation (3) reduces to the simpler expression:

Equation (4)

Using an argument similar to the one that proves GT = GT', it also turns out that Gp = Gp'.

Items to turn in

Questions

  1. At a frequency of 1 GHz, does the computed value for Gp meet the design requirement of 16 dB (to within 1%)?
  2. Does GT = Gp at the design frequency? Compare the values of GT and GP as the frequency moves away from the design value. What is the reason for this behavior?
  3. How do the input SWR (defined as (1+|S11'|)/(1-|S11'|)) and the output SWR (defined as (1+|S22'|)/(1-|S22'|)) of the overall Amp_Gp circuit vary with frequency?

Constant Gain Circles


Assignment

You will examine the effect of frequency on constant gain circles. The test circuit consists of the BJT, two S-ports, and no matching or bias networks.

Circuit construction

Constant gain circle test circuit

Figure 11: Constant gain circle test circuit

Circuit layout

Simulation

Output

Items to turn in

Questions

  1. What is the behavior of the gain circles as the frequency increases?
  2. The G=Gcircle(S, 15, 0, 1) equation called for a 15 dB gain circle. What happens to the gain circles on the Z-Smith chart if you try 16 dB? What is the reason for this effect?