Wilkinson power divider

Power divider in microstrip technology

In the field of microwave engineering and circuit design, the Wilkinson Power Divider is a specific class of power divider circuit that can achieve isolation between the output ports while maintaining a matched condition on all ports. The Wilkinson design can also be used as a power combiner because it is made up of passive components and hence reciprocal. First published by Ernest J. Wilkinson in 1960,^[1] this circuit finds wide use in radio frequency communication systems utilizing multiple channels since the high degree of isolation between the output ports prevents crosstalk between the individual channels.

It uses quarter wave transformers, which can be easily fabricated as quarter wave lines on printed circuit boards. It is also possible to use other forms of transmission line (e.g. coaxial cable) or lumped circuit elements (inductors and capacitors).^[2]

Theory

Picture shows a typical output expected from a Wilkinson power divider. The

S_{{21}},S_{{31}}

are almost -3 dB, and the

S_{{11}}

is low near the design frequency.

Picture demonstrates a very high isolation between output ports (port 2 & 3) of a Wilkinson power divider

The scattering parameters for the common case of a 2-way equal-split Wilkinson power divider at the design frequency is given by^[3]

[S]={\frac {-j}{{\sqrt {2}}}}{\begin{bmatrix}0&1&1\\1&0&0\\1&0&0\\\end{bmatrix}}

Inspection of the S matrix reveals that the network is reciprocal ( $S_{{ij}}=S_{{ji}}$ ), that the terminals are matched ( $S_{{11}},S_{{22}},S_{{33}}=0$ ), that the output terminals are isolated ( $S_{{23}},S_{{32}}$ =0), and that equal power division is achieved ( $S_{{21}}=S_{{31}}$ ). The non-unitary matrix results from the fact that the network is lossy. An ideal Wilkinson divider would yield $S_{{21}}=S_{{31}}=-3\,{\text{dB}}=10\log _{{10}}({\frac {1}{2}})$ .

Network theorem governs that a divider cannot satisfy all three conditions (being matched, reciprocal and loss-less) at the same time. Wilkinson divider satisfies the first two (matched and reciprocal), and cannot satisfy the last one (being loss-less). Hence, there is some loss occurring in the network.

No loss occurs when the signals at ports 2 and 3 are in phase and have equal magnitude.

However, some modification can be done to achieve unequal power division at the output ports. By cascading, the input power might be divided to any $n$ -number of outputs.

References

↑ E.J. Wilkinson, "An N-way Power Divider", IRE Trans. on Microwave Theory and Techniques, vol. 8, p. 116-118, Jan. 1960, doi: 10.1109/TMTT.1960.1124668
↑ "Overview and essentials of the Wilkinson divider splitter combiner". Radio-electronics.com. Retrieved 6 February 2013.
↑ D.M. Pozar, Microwave Engineering, Third Edition, John Wiley & Sons: New York, 2005

External links

Online Wilkinson Power Split Calculator
Online Resistive Power Split Calculator
Online Coaxial Power Split Calculator
Wilkinson power divider tutorial with other power divider / combiner pages

This article is issued from Wikipedia - version of the 4/22/2014. The text is available under the Creative Commons Attribution/Share Alike but additional terms may apply for the media files.

Wilkinson power divider

Theory

See also

References

External links