Examination of SMA connector parameters

Palecek, Juraj; Vestenický, Martin; Vestenický, Peter; Spalek, Juraj

doi:10.1109/ines.2012.6249841

Cited by 13 publications

(8 citation statements)

References 3 publications

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“…If we still set the electrical length of each transmission line as a quarter‐guided wavelength at the centre frequency, the power dividing ratio is defined as

P_{1} : P_{2} : P_{3} = k_{1}^{2} : k_{2}^{2} : k_{3}^{2}

Then, the impedance of distributing networks is

Z_{0 n} = \sqrt{(k_{1}^{2} + k_{2}^{2} + k_{3}^{2}) R_{x 0} R_{x n} / k_{n}^{2}}, n = 1, 2, 3

where R x 0 and R xn are the characteristic impedances of the common port and distributing ports, respectively. Following the derivation process in [31], the relationships between voltages and currents in the distributing network are

({, \begin{aligned} U_{0} = - j \frac{U_{1} R_{x 0}}{Z_{01}} \\ I_{1 c} = I_{1 c 2} + I_{1 c 3} = U_{1} ()(, \frac{1}{R_{x 1}} - \frac{R_{x 0}}{Z_{01}^{2}}) \\ I_{2 c} = I_{2 c 1} - I_{2 c 3} = \frac{U_{1} R_{x 0}}{Z_{01} Z_{02}} \\ I_{3 c} = I_{3 c 1} + I_{3 c 2} = \frac{U_{1} R_{x 0}}{Z_{01} Z_{03}} \end{aligned}),

…”

Section: Design Equation Derivationmentioning

confidence: 99%

“…Generally, the port impedances of common port R x0 and distributing ports R xn are unified to Z 0 for circuit simplification and realisation convenience. Thus, (9) can be expressed as

({, \begin{aligned} Z_{n m} = p_{m n} Z_{m n}, R_{n m} = q_{m n} R_{m n} \\ Z_{0 m} = \frac{Z_{0}}{K_{m}} \sqrt{false(K_{1}^{2} + K_{2}^{2} + K_{3}^{2} false)} \\ Z_{m n m} = \sqrt{\frac{(K_{1}^{2} + K_{2}^{2} + K_{3}^{2}) Z_{0}}{K_{n}^{2}} ∙ \frac{q_{m n} R_{m n}}{p_{m n}^{2} + q_{m n}}} \\ Z_{m n n} = \sqrt{\frac{(K_{1}^{2} + K_{2}^{2} + K_{3}^{2}) Z_{0}}{K_{m}^{2}} ∙ \frac{q_{m n} R_{m n} p_{m n}^{2}}{p_{m n}^{2} + q_{m n}}} \\ m = 1, 2, 3 \\ n = 1, 2, 3, m < n \end{aligned})

In (10), R mn , p mn , q mn , Z mn and Z 0 can be arbitrarily positive values, which may affect the frequency bandwidth, as discussed in [31]. In this paper, to investigate the effect of the operating frequency bandwidth, the model of the three‐way Gysel power divider is built and shown in Fig.…”

Section: Numerical Verification and Frequency Bandwidth Investigationmentioning

confidence: 99%

“…Afterwards, a back‐to‐back microstrip structure was used to realise an N‐ way Gysel combiner in [30]. Based on the existing designs, we proposed an N ‐way Gysel power divider on the arbitrary terminated impedance with closed‐form equations of arbitrary power dividing ratio, which were derived by using the node voltage and current method in [31].…”

Section: Introductionmentioning

confidence: 99%

“…The traditional N ‐way Gysel power dividers presented in 1975 [28] and in [29–31] have identical structures as shown in Fig. 1, which have the obvious characteristic of a common node in the centre of the divider.…”

Section: Introductionmentioning

confidence: 99%

See 3 more Smart Citations

Compact three‐way Gysel power divider with arbitrary power dividing ratio

Chen

Xue

et al. 2020

IET Microwaves, Antennas & Propagation

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“…If we still set the electrical length of each transmission line as a quarter‐guided wavelength at the centre frequency, the power dividing ratio is defined as

P_{1} : P_{2} : P_{3} = k_{1}^{2} : k_{2}^{2} : k_{3}^{2}

Then, the impedance of distributing networks is

Z_{0 n} = \sqrt{(k_{1}^{2} + k_{2}^{2} + k_{3}^{2}) R_{x 0} R_{x n} / k_{n}^{2}}, n = 1, 2, 3

({, \begin{aligned} U_{0} = - j \frac{U_{1} R_{x 0}}{Z_{01}} \\ I_{1 c} = I_{1 c 2} + I_{1 c 3} = U_{1} ()(, \frac{1}{R_{x 1}} - \frac{R_{x 0}}{Z_{01}^{2}}) \\ I_{2 c} = I_{2 c 1} - I_{2 c 3} = \frac{U_{1} R_{x 0}}{Z_{01} Z_{02}} \\ I_{3 c} = I_{3 c 1} + I_{3 c 2} = \frac{U_{1} R_{x 0}}{Z_{01} Z_{03}} \end{aligned}),

…”

Section: Design Equation Derivationmentioning

confidence: 99%

“…Generally, the port impedances of common port R x0 and distributing ports R xn are unified to Z 0 for circuit simplification and realisation convenience. Thus, (9) can be expressed as

({, \begin{aligned} Z_{n m} = p_{m n} Z_{m n}, R_{n m} = q_{m n} R_{m n} \\ Z_{0 m} = \frac{Z_{0}}{K_{m}} \sqrt{false(K_{1}^{2} + K_{2}^{2} + K_{3}^{2} false)} \\ Z_{m n m} = \sqrt{\frac{(K_{1}^{2} + K_{2}^{2} + K_{3}^{2}) Z_{0}}{K_{n}^{2}} ∙ \frac{q_{m n} R_{m n}}{p_{m n}^{2} + q_{m n}}} \\ Z_{m n n} = \sqrt{\frac{(K_{1}^{2} + K_{2}^{2} + K_{3}^{2}) Z_{0}}{K_{m}^{2}} ∙ \frac{q_{m n} R_{m n} p_{m n}^{2}}{p_{m n}^{2} + q_{m n}}} \\ m = 1, 2, 3 \\ n = 1, 2, 3, m < n \end{aligned})

Section: Numerical Verification and Frequency Bandwidth Investigationmentioning

confidence: 99%

Section: Introductionmentioning

confidence: 99%

Section: Introductionmentioning

confidence: 99%

See 2 more Smart Citations

Compact three‐way Gysel power divider with arbitrary power dividing ratio

Chen

Xue

et al. 2020

IET Microwaves, Antennas & Propagation

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“…Connectors are necessary to connect cables in such systems. The modeling of SMA connectors is either neglected in the simulation of microwave components or approximated by an inaccurate model to model its characteristics . In this study, modeling of the SMA connector is investigated and an accurate simulation modeling is studied and discussed.…”

Section: Introductionmentioning

confidence: 99%

Influence of the SMA connector and its modeling on electromagnetic simulation

Hirano

Hirokawa

Ando

2015

Micro & Optical Tech Letters

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The modeling of subminiature version A (SMA) connectors is occasionally neglected when simulating microwave components or when an approximated model is used to represent its characteristics. In this article, SMA connector modeling is investigated and an appropriate simulation modeling is discussed. It was observed that modeling the inner part of the SMA connector using the coaxial cable model is adequate when no electromagnetic field exist outside of the SMA connector. However, modeling the exterior structure including a receptacle, if it exists, is required when an electromagnetic field exist outside the connector. © 2015 Wiley Periodicals, Inc. Microwave Opt Technol Lett 57:2168–2171, 2015

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RF modeling and optimization of end-launch SMA to trace transition

Zha

Wang

et al. 2015

2015 IEEE 17th Electronics Packaging and Technology Conference (EPTC)

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Examination of SMA connector parameters

Cited by 13 publications

References 3 publications

Compact three‐way Gysel power divider with arbitrary power dividing ratio

Compact three‐way Gysel power divider with arbitrary power dividing ratio

Influence of the SMA connector and its modeling on electromagnetic simulation

RF modeling and optimization of end-launch SMA to trace transition

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