I have read through your problem and the other various answers the solution however is simpler than you would imagine. I am going to assume that L C and R are in series if not its dosnt really matter the principle is the same. You need to add a spoiler to the circuit block which will widden the bandwidth because Qseries= SQRT((X/R)-1) in other words increasing R in series reduces the Q. Or in parrallel Qpar= SQRT((R/X)-1) which in this case add R in parrallel with the existing parallel R to reduce the R. Jobs a good one. I have had to make some assumptions about exctly what it is your CCT does, however the principle is one that is used all the time I hope this can be used in your case. Then just match to the new vaue of the real parts of the source and the load and then resonate out any reactance if you desire to do that. Remember the ultimate Q you can achieve is limited by the real parts of the source and load therefore if you find the remaining real parts still presents too high a Q then match with several cascaded L sections to increase the bandwidth. The more you cascade L section the more the match approaches that of a wide band transmission line. Hope the above is of use.
I have a circuit block ---R---C---L---, where R (5 ohm) is small, L is large, and C is small. The total impedance Z = R at 915 MHz (L and C resonate). Since the imaginary part can be very large, how can I design a broadband matching network? I have to point out that we can't do anything to the block itself.
Dear AmirMohammad,
Thank you for your introduction about a book named "solid state microwave amplifier design" written by T.T.Ha, although I cannot find this book.
Can you send an ebook of that one? My email:bg_islang@sohu.com.
Thanks again!
Lu