Skip to main content

Wilkinson Power Divider

And now for a little applied physics!  The Wilkinson power divider shown to the left schematically (picture 1), is a cool little circuit that evenly divides a microwave signal at a specified design frequency and supplies it to two or more circuits downstream from itself.  In addition to evenly dividing the applied power from the source, the Wilkinson divider also protects each of the circuits it supplies from any reflected signals from the other supplied circuits.  The circuit design was first published in 1960 by Ernest Wilkinson[1].

A simplified diagram of the circuit is shown below.  It divides the input from the source down two conductors that are each cut to be exactly as long as one quarter of the wavelength of the microwave signal supplied by the source.  The power is automatically divided due to one of the properties that physicists love: symmetry.  Faced with no difference in the two paths it's presented with, the input microwave signal splits and half of its power travels down each path.  That's kind of cool, but if that's all that Wilkinson intended, he could have used any conductor length.



The quarter wavelength conductors provide an ingenious way of protecting each supplied circuit from the
other ones.  Under normal operation, there's no potential difference at the end of the divider where the resistor connects the two conductors, so no current flows through the resistor.  If one of the supplied circuits begins to force reflected power back into the divider, the resistor comes into play.  It immediately shunts part of the reflected power over to the other output.  That sounds bad, but wait for it.

The portion of the reflected signal, (step 1 in picture 3) that isn't shunted will travel back down the quarter wavelength conductor changing it's phase by 90 degrees, (a quarter wavelength), in the process, (step 2 in picture 3).  At the top of the divider it will travel the opposite direction down the other conductor and in so doing pick up another 90 degree phase shift.  At this point, it's picked up 180 degree phase shift and perfectly interferes with itself in the second conductor cancelling itself out! (step 3 in picture 3)



References:

1.  Original circuit design
Wilkinson E.J. (1960). An N-Way Hybrid Power Divider, IEEE Transactions on Microwave Theory and Techniques, 8 (1) 116-118. DOI:

http://ieeexplore.ieee.org/xpl/articleDetails.jsp?tp=&arnumber=1124668&contentType=Journals+%26+Magazines&sortType%3Dasc_p_Sequence%26filter%3DAND%28p_IS_Number%3A24846%29

Comments

Popular posts from this blog

More Cowbell! Record Production using Google Forms and Charts

First, the what : This article shows how to embed a new Google Form into any web page. To demonstrate ths, a chart and form that allow blog readers to control the recording levels of each instrument in Blue Oyster Cult's "(Don't Fear) The Reaper" is used. HTML code from the Google version of the form included on this page is shown and the parts that need to be modified are highlighted. Next, the why : Google recently released an e-mail form feature that allows users of Google Documents to create an e-mail a form that automatically places each user's input into an associated spreadsheet. As it turns out, with a little bit of work, the forms that are created by Google Docs can be embedded into any web page. Now, The Goods: Click on the instrument you want turned up, click the submit button and then refresh the page. Through the magic of Google Forms as soon as you click on submit and refresh this web page, the data chart will update immediately. Turn up the:

Cool Math Tricks: Deriving the Divergence, (Del or Nabla) into New (Cylindrical) Coordinate Systems

Now available as a Kindle ebook for 99 cents ! Get a spiffy ebook, and fund more physics The following is a pretty lengthy procedure, but converting the divergence, (nabla, del) operator between coordinate systems comes up pretty often. While there are tables for converting between common coordinate systems , there seem to be fewer explanations of the procedure for deriving the conversion, so here goes! What do we actually want? To convert the Cartesian nabla to the nabla for another coordinate system, say… cylindrical coordinates. What we’ll need: 1. The Cartesian Nabla: 2. A set of equations relating the Cartesian coordinates to cylindrical coordinates: 3. A set of equations relating the Cartesian basis vectors to the basis vectors of the new coordinate system: How to do it: Use the chain rule for differentiation to convert the derivatives with respect to the Cartesian variables to derivatives with respect to the cylindrical variables. The chain

The Valentine's Day Magnetic Monopole

There's an assymetry to the form of the two Maxwell's equations shown in picture 1.  While the divergence of the electric field is proportional to the electric charge density at a given point, the divergence of the magnetic field is equal to zero.  This is typically explained in the following way.  While we know that electrons, the fundamental electric charge carriers exist, evidence seems to indicate that magnetic monopoles, the particles that would carry magnetic 'charge', either don't exist, or, the energies required to create them are so high that they are exceedingly rare.  That doesn't stop us from looking for them though! Keeping with the theme of Fairbank[1] and his academic progeny over the semester break, today's post is about the discovery of a magnetic monopole candidate event by one of the Fairbank's graduate students, Blas Cabrera[2].  Cabrera was utilizing a loop type of magnetic monopole detector.  Its operation is in concept very sim