Notes 17 ECE Microwave Engineering Multistage Transformers

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Notes 18 ECE Microwave Engineering Multistage Transformers
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Notes 17 ECE 5317-6351 Microwave Engineering Multistage Transformers Fall 2015 Prof. David R. Jackson Dept. of ECE Notes 17 Multistage Transformers

Single-stage Transformer The transformer length is arbitrary in this analysis.

Single-stage Transformer (cont.) After some algebra (omitted), we can write Assume small reflections:

Single-stage Transformer (cont.) Approximation for small reflections:

Single-stage Transformer (cont.) Physical interpretation:

Multistage Transformer Assuming small reflections: where Note that this is a polynomial in powers of z = exp(-j2).

Multistage Transformer (cont.) (N+1 terms) If we assume symmetric reflections of the sections about the center of the structure (not a symmetric layout of line impedances), we have: or Last term

Multistage Transformer (cont.) Hence, for symmetric reflections we can also write: Note that this is a finite Fourier cosine series.

Multistage Transformer (cont.) Design philosophy: If we choose a response for ( ) that is in the form of either a polynomial (in powers of z = exp (-j2 )) or a Fourier cosine series, we can obtain the needed values of n and hence complete the design. (does not assume symmetric reflections) or (assumes symmetric reflections)

Binomial (Butterworth*) Multistage Transformer Choose: (A is real, could be positive or negative) (alternative form) *The name comes from the British physicist/engineer Stephen Butterworth, who described the design of filters using the binomial principle in 1930.

Binomial Multistage Transformer (cont.) Maximally flat property: Use: Choose all lines to be a quarter wavelength at the center frequency so that (We have a perfect match at the center frequency.) The reflection coefficient stay small for as wide a frequency as possible.

Binomial Multistage Transformer (cont.) Using the binomial expansion, we can express the Butterworth response in terms of a polynomial series: A binomial type of response is obtained if we thus choose We want to use a multistage transformer to realize this type of response. Set equal (Both are now in the form of polynomials.)

Binomial Multistage Transformer (cont.) Solving for A: Use: Hence Also (A zero-length set of lines has no effect.) Equating these two results, we have Note: A could be positive or negative.

Binomial Multistage Transformer (cont.) Solving for n: Set equal Equating responses for each term in the polynomial series gives us: Hence or This gives us a solution for the line impedances (recursive formula).

Binomial Multistage Transformer (cont.) Note on reflection coefficients Note that: Hence Although we did not assume that the reflection coefficients were symmetric in the design process, they actually come out that way.

Binomial Multistage Transformer (cont.) Note: The table only shows data for ZL > Z0 since the design can be reversed (Ioad and source switched) for ZL < Z0 .

Binomial Multistage Transformer (cont.) Example showing a microstrip line A three-stage transformer is shown.

Binomial Multistage Transformer (cont.) Note: Increasing the number of lines increases the bandwidth.

Binomial Multistage Transformer (cont.) Approximate formula for line impedances Recall Use a series approximation for the ln function on both sides: Hence Recursive formula

Binomial Multistage Transformer (cont.) Bandwidth Maximum acceptable reflection The bandwidth is then: Hence

Binomial Multistage Transformer (cont.) Summary of Design Formulas Reflection coefficient response A coefficient or Design of line impedances Bandwidth

Recall: A single quarter-wave transformer had a bandwidth of about 6%. Example Three-stage binomial transformer Given: Recall: A single quarter-wave transformer had a bandwidth of about 6%.

Example (cont.)

Example (cont.) Using the table in Pozar we have: (The above normalized load impedance is the reciprocal of what we actually have.) Hence, switching the load and the source ends, we have Therefore

Example (cont.)  Microstrip Response from Ansys Designer

Chebyshev Multistage Matching Transformer Chebyshev polynomials of the first kind: We choose the response to be in the form of a Chebyshev polynomial. (This will lead to a finite Fourier cosine series in .)

Chebyshev Transformer (cont.)

Chebyshev Transformer (cont.) A Chebyshev response will have equal ripple within the bandwidth. Choose: This can be put into a form involving the terms cos (n ) (i.e., a finite Fourier cosine series). Note: As frequency decreases, x increases.

Chebyshev Transformer (cont.) We have that, after some algebra, Hence, the term TN (secm, cos) can be cast into a finite cosine Fourier series expansion.

Chebyshev Transformer (cont.) Transformer design From the above formula we can extract the coefficients n (no general formula is given here). Solve for A:

Chebyshev Transformer (cont.) Alternative formula for A: Which sign is correct? Hence

Chebyshev Transformer (cont.) Bandwidth What is m ? Also, we have Hence, we have

Chebyshev Transformer (cont.) Bandwidth (cont.) Use: Hence We then have

Chebyshev Transformer (cont.) Summary of Design Formulas Reflection coefficient response m term A coefficient No formula given for the line impedances. Use the Table from Pozar or generate (“by hand”) the solution by expanding ( ) into a polynomial with terms cos (n ). Design of line impedances Bandwidth

Chebyshev Transformer (cont.) Note: The table only shows data for ZL > Z0 since the design can be reversed (Ioad and source switched) for ZL < Z0 .

Chebyshev Transformer (cont.)

Example Example: three-stage Chebyshev transformer Hence Given Equate (finite Fourier cosine series form) Equate

Example (cont.) Equating coefficients from the previous equation on the last slide, we have:

(It should be 100 []; there is some round-off error here). Example (cont.) (It should be 100 []; there is some round-off error here).

Example (cont.) Alternative method:

Example (cont.)

Example (cont.)  Response from Ansys Designer

Example (cont.) Comparison of Binomial (Butterworth) and Chebyshev The Chebyshev design has a higher bandwidth (100% vs. 69%). The increased bandwidth comes with a price: ripple in the passband. Note: It can be shown that the Chebyshev design gives the highest possible bandwidth for a given N and m.

Tapered Transformer The Pozar book also talks about using continuously tapered lines to match between an input line Z0 and an output load ZL. (pp. 255-261). Please read this. The “Klopfenstein taper” gives the Z(z) that is best (lowest reflection coefficient) for a given length L.