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Scattering Parameters for Two-port Circuit

Scattering Parameters for Two-port Circuit

Presentation in Experiments and Practice of Electrical and Electronics Engineering for fourth-year technical college students.

Avatar for Kazuaki Ohyama

Kazuaki Ohyama

March 27, 2024

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  1. 2026/4/20 Introduction: Background 1 Wireless Power Transmission Wireless IoT https://newswitch.jp/p/31332

    https://mitssolutions.asia/products/bea nair/sensors/wireless-iot-accelerometer- sensors/beandevice-wifi-wilow-ax-3d/
  2. 2026/4/20 • Conductor wire – For kHz order • Coaxial

    cable – For MHz, GHz order Introduction: Transmission Devices 2 https://www.kawai-cable.co.jp/products/vct-sb.html https://eshop.aisan.co.jp/?p=13748
  3. 2026/4/20 Distributed Line: Wavelength in a Circuit • Wavelength 𝜆

    = ! " 3 <latexit sha1_base64="WxRC5H9J/NGzm7Fn2SzeVE0B7dU=">AAAB63icbVDLSgNBEOyNrxhfUY9eFoPgKeyKr2PQi8cI5gHJEmYnnWTIzOw6MyuEJb/gxYMiXv0hb/6Ns8keNLGgoajqprsrjDnTxvO+ncLK6tr6RnGztLW9s7tX3j9o6ihRFBs04pFqh0QjZxIbhhmO7VghESHHVji+zfzWEyrNIvlgJjEGggwlGzBKTCZ1JT72yhWv6s3gLhM/JxXIUe+Vv7r9iCYCpaGcaN3xvdgEKVGGUY7TUjfRGBM6JkPsWCqJQB2ks1un7olV+u4gUrakcWfq74mUCK0nIrSdgpiRXvQy8T+vk5jBdZAyGScGJZ0vGiTcNZGbPe72mUJq+MQSQhWzt7p0RBShxsZTsiH4iy8vk+ZZ1b+sXtyfV2o3eRxFOIJjOAUfrqAGd1CHBlAYwTO8wpsjnBfn3fmYtxacfOYQ/sD5/AEbTY5M</latexit> 6= >
  4. 2026/4/20 Introduction: Purposes • The impedance matching at the distributed

    line • The definition of the scattering parameters for a two-port circuit 1. Solve the telegram equations 2. Connect two distributed lines as a two-port circuit 3. Suppose a special situation 4
  5. 2026/4/20 Distributed Line: Coaxial Cable Model (1) 5 <latexit sha1_base64="ES8A0ODLLfNd3GnERolM0ETqeus=">AAACGHicbVDLSsNAFJ34rPEVdekmWAQXUhOR6rLoxoVgRfugSQiT6aQdOpOEmYlQQj/Djb/ixoUibrvzb5y0WWjbAxcO59zLvfcECSVCWtaPtrS8srq2XtrQN7e2d3aNvf2miFOOcAPFNObtAApMSYQbkkiK2wnHkAUUt4LBTe63njEXJI6e5DDBHoO9iIQEQakk3zjr+I/uqeMyKPucZe49wz048lxX7/h3CwzfKFsVawJzntgFKYMCdd8Yu90YpQxHElEohGNbifQyyCVBFI90NxU4gWgAe9hRNIIMCy+bPDYyj5XSNcOYq4qkOVH/TmSQCTFkgerM7xSzXi4u8pxUhldeRqIklThC00VhSk0Zm3lKZpdwjCQdKgIRJ+pWE/Uhh0iqLHUVgj378jxpnlfsaqX6cFGuXRdxlMAhOAInwAaXoAZuQR00AAIv4A18gE/tVXvXvrTvaeuSVswcgH/Qxr+RNKAj</latexit>

    ZS [⌦] ZL [⌦] : Internal impedance of 𝑣! 𝑡 <latexit sha1_base64="ES8A0ODLLfNd3GnERolM0ETqeus=">AAACGHicbVDLSsNAFJ34rPEVdekmWAQXUhOR6rLoxoVgRfugSQiT6aQdOpOEmYlQQj/Djb/ixoUibrvzb5y0WWjbAxcO59zLvfcECSVCWtaPtrS8srq2XtrQN7e2d3aNvf2miFOOcAPFNObtAApMSYQbkkiK2wnHkAUUt4LBTe63njEXJI6e5DDBHoO9iIQEQakk3zjr+I/uqeMyKPucZe49wz048lxX7/h3CwzfKFsVawJzntgFKYMCdd8Yu90YpQxHElEohGNbifQyyCVBFI90NxU4gWgAe9hRNIIMCy+bPDYyj5XSNcOYq4qkOVH/TmSQCTFkgerM7xSzXi4u8pxUhldeRqIklThC00VhSk0Zm3lKZpdwjCQdKgIRJ+pWE/Uhh0iqLHUVgj378jxpnlfsaqX6cFGuXRdxlMAhOAInwAaXoAZuQR00AAIv4A18gE/tVXvXvrTvaeuSVswcgH/Qxr+RNKAj</latexit> ZS [⌦] ZL [⌦] : Load impedance <latexit sha1_base64="PkJDcbKOaYFq9n50M5dHlgBLMIA=">AAAB+HicbVDLSsNAFL3xWeujUZduBovgQkoiUl0W3bisYB/QhDKZTtqhM0mYmYg19EvcuFDErZ/izr9x0mahrQcGDufcyz1zgoQzpR3n21pZXVvf2Cxtlbd3dvcq9v5BW8WpJLRFYh7LboAV5SyiLc00p91EUiwCTjvB+Cb3Ow9UKhZH93qSUF/gYcRCRrA2Ut+uPHpnPU9gPZIiE1O/b1edmjMDWiZuQapQoNm3v7xBTFJBI004VqrnOon2Myw1I5xOy16qaILJGA9pz9AIC6r8bBZ8ik6MMkBhLM2LNJqpvzcyLJSaiMBM5hHVopeL/3m9VIdXfsaiJNU0IvNDYcqRjlHeAhowSYnmE0MwkcxkRWSEJSbadFU2JbiLX14m7fOaW6/V7y6qjeuijhIcwTGcgguX0IBbaEILCKTwDK/wZj1ZL9a79TEfXbGKnUP4A+vzB/R3k04=</latexit> x [m] : Distance Coaxial Cable
  6. 2026/4/20 Distributed Line: Telegram Equations (2) 9 Incident wave Reflected

    wave <latexit sha1_base64="Wx04HTQsNtITvt0QVKpAhpKvLzs=">AAACHnicbVDJSgNBEO1xjXGLevTSGBRFDTPidhGCXjwqmFHIRk+nkjTpnhm6a8Qw5Eu8+CtePCgieNK/sRODuD1oeP1eFVX1glgKg6777oyMjo1PTGamstMzs3PzuYVF30SJ5lDikYz0VcAMSBFCCQVKuIo1MBVIuAw6J33/8hq0EVF4gd0Yqoq1QtEUnKGV6rm9CrZBQzPSQP31my2KG2tHfm0Taul2pcWUYvSmt+nXtq3w9S/Uc3m34A5A/xJvSPJkiLN67rXSiHiiIEQumTFlz42xmjKNgkvoZSuJgZjxDmtB2dKQKTDVdHBej65apUHtivaFSAfq946UKWO6KrCVimHb/Pb64n9eOcHmYTUVYZwghPxzUDORFCPaz4o2hAaOsmsJ41rYXSlvM8042kSzNgTv98l/ib9T8PYL++e7+eLxMI4MWSYrZJ145IAUySk5IyXCyS25J4/kyblzHpxn5+WzdMQZ9iyRH3DePgCbrqD0</latexit> ) V (x, t) = V +e x + V e x. Propagation constant <latexit sha1_base64="rMSUXxeH5TXsUZxTE8CiAJUm05k=">AAACEnicbVDLSgMxFM3UV62vUZdugkXoINQZkepGKHahCxdV7AM7w5BJ0zY28zDJCGXoN7jxV9y4UMStK3f+jWk7iFYPXDg5515y7/EiRoU0zU8tMzM7N7+QXcwtLa+srunrG3URxhyTGg5ZyJseEoTRgNQklYw0I06Q7zHS8PqVkd+4I1zQMLiSg4g4PuoGtEMxkkpydePaNeExtMUtl0nhcvfGDn3SRfDc2Cucfr8qhjF09bxZNMeAf4mVkjxIUXX1D7sd4tgngcQMCdGyzEg6CeKSYkaGOTsWJEK4j7qkpWiAfCKcZHzSEO4opQ07IVcVSDhWf04kyBdi4Huq00eyJ6a9kfif14pl58hJaBDFkgR48lEnZlCGcJQPbFNOsGQDRRDmVO0KcQ9xhKVKMadCsKZP/kvq+0WrVCxdHOTLJ2kcWbAFtkEBWOAQlMEZqIIawOAePIJn8KI9aE/aq/Y2ac1o6cwm+AXt/Qv4HZsq</latexit> Z0 = p (R + j!L)/(G + j!C)) Characteristic impedance <latexit sha1_base64="DZjWAi5IjOLOG9ohr0X4z6vnKYk=">AAACFHicbVDLSgMxFM3UV62vqks3wSK0FMqMSHUjFLvQhYsqVgudUu6kaRubzIxJRihDP8KNv+LGhSJuXbjzb0wfiLYeuHByzr3k3uOFnClt219WYm5+YXEpuZxaWV1b30hvbl2rIJKEVknAA1nzQFHOfFrVTHNaCyUF4XF64/XKQ//mnkrFAv9K90PaENDxWZsR0EZqpvNuB4QAfIxddSd1nL3M37qBoB3A57ns6c+jnMsNmumMXbBHwLPEmZAMmqDSTH+6rYBEgvqacFCq7tihbsQgNSOcDlJupGgIpAcdWjfUB0FVIx4dNcB7RmnhdiBN+RqP1N8TMQil+sIznQJ0V017Q/E/rx7p9lEjZn4YaeqT8UftiGMd4GFCuMUkJZr3DQEimdkVky5IINrkmDIhONMnz5Lr/YJTLBQvDjKlk0kcSbSDdlEWOegQldAZqqAqIugBPaEX9Go9Ws/Wm/U+bk1Yk5lt9AfWxzdiipyF</latexit> = p (R + j!L)(G + j!C))
  7. 2026/4/20 Distributed Line: Reflection Coefficient 𝛤 (2) • 𝛤 ≡

    #! #" • 𝛤 = 0 Ø 𝑉" = 0: No reflected wave Ø Impedance matched 12 Distributed Line
  8. 2026/4/20 Scattering Parameters: Case of Port Matched 17 <latexit sha1_base64="b0+soynN/3WUZWtCmtw8JDYK1yA=">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</latexit>

    ✓ b1 b2 ◆ = ✓ S11 S12 S21 S22 ◆ ✓ a1 a2 ◆ <latexit sha1_base64="iO9ARtNA4baLlv+TuCX31GtAor0=">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</latexit> ) S11 = b1 a1 a2=0 ) S21 = b2 a1 a2=0
  9. 2026/4/20 • 𝛤 = #! #" • 𝑆$$ = '

    %# &# &$'( Reflection Coefficient and Scattering Parameter 18 Distributed Line
  10. 2026/4/20 • 𝛤 = #! #" • 𝑆$$ = '

    %# &# &$'( Reflection Coefficient and Scattering Parameter 19 Distributed Line <latexit sha1_base64="J86CAl0qOR4xeGu7adgzFIM05gs=">AAACCHicbVBNS8NAEN34WetX1KMHF4vgqSQi6kUQPeixotVCE8pmO7WLu0nYnQgl5OjFv+LFgyJe/Qne/Dduaw5afTDweG+GmXlRKoVBz/t0JianpmdmK3PV+YXFpWV3ZfXKJJnm0OSJTHQrYgakiKGJAiW0Ug1MRRKuo9uToX99B9qIJL7EQQqhYjex6AnO0EoddyPAPmjoJRpoHgjMg1OmFCuKw4tO7vtFx615dW8E+pf4JamREo2O+xF0E54piJFLZkzb91IMc6ZRcAlFNcgMpIzfshtoWxozBSbMR48UdMsqXWqPsRUjHak/J3KmjBmoyHYqhn0z7g3F/7x2hr2DMBdxmiHE/HtRL5MUEzpMhXaFBo5yYAnjWthbKe8zzTja7Ko2BH/85b/kaqfu79X3zndrR8dlHBWyTjbJNvHJPjkiZ6RBmoSTe/JInsmL8+A8Oa/O23frhFPOrJFfcN6/ANY9md0=</latexit> ) = S11
  11. 2026/4/20 Conclusion • Two analog filters were measured by 1.

    The time-domain response 2. The frequency-domain response • Impedance matching can be done by – The reflection coefficient 𝛤 – Scattering parameters • The reflection coefficient 𝛤 is equal to 𝑆$$ 20