ECE 5317-6351 Microwave Engineering Fall 2011 Prof. David R. Jackson Dept. of ECE Notes 16 S-Parameter Measurements 1 S-Parameter Measurements S-parameters are typically measured, at microwave frequencies, with a network analyzer (NA). These instruments have found wide, almost universal, application since the mid to late 1970’s. Vector network analyzer: Magnitudes and phases of the S parameters are measured. Scalar network analyzer: Only the magnitudes of the Sparameters is measured. 2 Vector Network Analyzer (VNA) Port 1 a1 b1 DUT Hewlett-Packard 8510 DUT b2 a2 3 Network Analysis of VNA Measurement Port 1 Vector Network Analyzer Measurement plane 1 a1 Measurement Port 2 plane 2 a2 b1 b2 Device under test (DUT) Test cables 4 S-Parameter Measurements We want to measure [S] for DUT m a Port 1 1 b1m Error Box A Meas. plane 1 Error Box B DUT Ref. plane Ref. plane a2m m 2 Port 2 b Meas. plane 2 Error boxes contain effects of test cables, connectors, couplers,… 5 S-Parameter Measurements (cont.) Error Box A m 1 a A S21 S11A S12A S21 1 1 S12 S12B 1 1 1 b2m S11B B S22 S22 S11 A S22 b1m Error Box B DUT B S21 a2m Assume error boxes are reciprocal A B S21 S12A and S21 S12B A B W e n e e d to " ca lib ra te " to fin d S a n d S . A B If S a n d S a re k n o w n w e ca n e xtra ct S fro m m e a su re m e n ts . This is called “de-embedding.” 6 Calibration “Short, open, match” calibration procedure S21 1 a1m 1 S22 S11 SC -1 Connect OC +1 Z0 0 b1m S12 1 short 1 open A,B Calibration loads S S m 11 SC S 11 S S m 11 m atch S 11 S 11 2 Recall from Notes 15: 21 1 S 22 S m 11 O C match 2 21 1 S 22 3 m e a s u re m e n ts : m m ( S 11 , S 11 SC m OC , S 11 ) m atch in S 11 S 21 S 12 L 1 L S 22 3 u n k n o w n s fo r e a c h p o rt : S , S 21 , S 22 11 7 Calibration (cont.) “ Thru-Reflect-Line (TRL)” calibration procedure This is an improved calibration method that involves three types of connections: 1) The “thru” connection, in which port 1 is directly connected to port 2. 2) The “reflect” connection, in which a load with an (ideally) large (but not necessarily precisely known) reflection coefficient is connected. 3) The “line” connection, in which a length of matched transmission line (with an unknown length) is connected between ports 1 and 2. The advantage of the TRL calibration is that is does not requires precise short, open, and matched loads. This method is discussed in the Pozar book (pp. 193-196). 8 Z-Parameter Extraction Assume a reciprocal and symmetrical waveguide or transmission-line discontinuity. T Examples g T Microstrip gap Waveguide post Discontinuity model T We want to find Z1 and Z2 to model the discontinuity. T Z1 Z1 Z0 Z2 Z0 9 Z-Parameter Extraction (cont.) T T Z1 Z1 Z0 Z2 Plane of symmetry (POS) Z0 POS T T Z1 Z0 Z1 2Z 2 2Z 2 Z0 10 Z-Parameter Extraction (cont.) Assume that we place a short or an open along the plane of symmetry. T T POS Z1 Z0 Z1 2Z 2 2Z 2 SC Z0 ZL Z0 ZL Z1 Z LSC POS Z1 Z1 OC 2Z 2 Z0 2Z 2 Z1 2 Z 2 Z LOC Z1 Z L SC Z2 1 2 Z SC L ZL OC 11 Z-Parameter Extraction (cont.) The short or open can be realized by using odd- or even-mode excitation. T Incident voltage waves + - Odd mode excitation + + Even mode excitation The even/odd-mode analysis is very useful in analyzing devices (e.g., using HFSS). 12 De-embeding of a Line Length We wish the know the reflection coefficient of a device under test (DUT), but the DUT is not assessable directly – it has an extra length of transmission line connected to it. S11m S11 L L m , DUT S 11 S 11 DUT e Z0 , j2 L Z L Z0 Z L Z0 ZL DUT Ref. plane Meas. plane R e p la ce D U T Z L w ith short circuit S 11 m , SC e S SC 11 1 j2 L L S DUT 11 S m ,D U T 11 1 m , SC S 11 13