Dear Mr. Brown, You may indeed have missed some good articles in your quick scan of my site www.sigcon.com. Two articles are particularly relevant to the issue of differential coupling: "Differential Trace Impedance", and "Ribbon Cable Impedance" To find them, look under "archives" for the "key word index", and try the keyword "differential". The content of those articles generally agrees with the writeup you have provided below. Best regards, Dr. Howard Johnson, Signal Consulting Inc., tel +1 509-997-0505, howiej@xxxxxxxxxx http:\\sigcon.com -- High-Speed Digital Design articles, books, tools, and seminars -----Original Message----- From: si-list-bounce@xxxxxxxxxxxxx [mailto:si-list-bounce@xxxxxxxxxxxxx]On Behalf Of Mike Brown Sent: Friday, April 11, 2003 4:50 PM To: Jim G Roberts Cc: si-list@xxxxxxxxxxxxx Subject: [SI-LIST] Re: LVDS Termination Jim, "The two lines in parallel, . . ." is missing one word to be correct. That word is "isolated". When is 50 ohms in parallel with 50 ohms not equal to 25 ohms? When the 50 ohm impedances are half the differential impedance of a pair of coupled lines. The impedance depends on the excitation. Let's look into an ideal symmetrical line. o ---- Cm ---- o <-- line conductor | | Cg Cg | | gnd gnd If the lines are driven differentially, current flows in both the ground capacitance Cg and the line-to-line capicatance Cm, and both figure into the Zdiff calculation. If the lines are driven in parallel (common mode, CM, excitation), there's no CM current in Cm because both sides of Cm operate at the same potential (by definition of the CM drive stimulus). If there is no current flow through an element it may be removed from the circuit being analyzed. Less C => higher Z. If the lines are loosely coupled (Cm ~ 0) then your model is correct - the parallel impedance is practically 25 ohms, and the Rcm value is practically 0. If Cm is other than very small, then the CM impedance is greater than Zdiff/2. If asymmetry is introduced into the lines, common-mode excitation results in differential-mode noise, and vice versa. I'm not particularly concerned about high frequency Vcm spikes from a signalling viewpoint (within the spec Vcm range of the receiver), but I am concerned about the resultant differential noise. I also understand the EMI threat of CM noise. That's two reasons why CM termination is important. Dr. Johnson's HSDD book, and his web site articles (see Charles Grasso, below), seem to ignore the coupled line effects on the CM impedance (unless I missed the article in my admittedly quick scan of the site). This is possibly because the achievable coupling in a PWB is low, hence the practical CM impedance in a PWB differs little from Zdiff/2. That's not necessarily the case if the transmission medium is not a PWB. Whether or not there's an added Rcm in the ground return path, there must be at least an AC ground return path from the center of the differential termination in order to terminate CM noise. Regards Mike Jim G Roberts wrote: >Hi Mike, > I think I am missing something here. >The two lines in parallel, in accordance with your sketch, will have a >common-mode impedance of 25ohm [50/2]. >With Rcm at zero you will always terminate the common signals at the receiver >end however they are generated. >More often high frequency Vcm spikes, etc. are generated by unequal length of >lines. Of course crosstalk and power supply ripple can induce unwanted signals. >Can you explain why you would need a different impedance for the common-mode ac >signals. >-- >Regards, __________ James G Roberts > /___ ____ | jrobert@xxxxxxxxxxxxxxxxxxxxx > Jim __ / /___/ / jgroberts@xxxxxxxxxx > / /_/ /---| | Room: BE436, Hilversum > \____/ /_/ Tel: +31 35 687 4308 Fax: 5976 > >Mike Brown wrote: > > > >>Justin, >> >>Perhaps a sketch will help, just in case you are thinking about a >>different topology than I (differential sources omitted): >> (Rdiff) >> +---- Line + --- 50 ---+ >>Gnd --- Vcm ---+ +--- Rcm --- Cap --- Gnd >> +---- Line - --- 50 ---+ >> >>The cap charges to Vcm (average); the termination impedance of the >>common-mode driven lines for AC is Rdiff/2 + Rcm, where that sum is >>ideally the CM impedance. With no AC CM, no current flows in the CM >>termination. The requirement is that (25+Rcm)*Cap >> period of the >>common mode noise. The cap is thus a near short at the frequencies of >>concern. >> >>In widely-spaced lines, Rcm approaches zero, because the CM impedance >>approaches Zdiff/2. This is the typical center-tapped termination. If >>the lines are coupled, the mutual C, Cm, (too many CMs/Cm's in this >>discussion!) impacts the differential Z, but drops out of the >>calculation of Zcm. For common mode excitation, the voltage at each >>terminal of Cm is equal, hence no current flows in Cm. If there's no >>current flow through the component, the component can be excluded from >>the analysis. The result is that Zcm is greater than Zdiff/2, and the >>need for Rcm for ideal termination. >> >>HTH >> >>Mike >> >>Tabatchnick, Justin wrote: >> >> >> >>>Mike; >>> >>>I don't quite understand your approach , it seems to me that you will >>>still get large reflection because your load impedance is now complex >>>with the addition of the cap and the real part is still a large >>>impedance. Can you elaborate more ? >>> >>>Thanks >>> >>>Justin >>> >>>-----Original Message----- >>>From: Mike Brown [mailto:bmgman@xxxxxxxxxx]=20 >>>Sent: Thursday, April 10, 2003 8:08 PM >>>To: kenneth.w.siders@xxxxxxxx >>>Cc: 'si-list@xxxxxxxxxxxxx' >>>Subject: [SI-LIST] Re: LVDS Termination >>> >>>Think about driving the 2 lines in parallel, with only a high-Z path to >>> >>> >>ground at the receiver input (the condition without the cap). Without the >>capacitor, the CM reflection coefficient approaches 1. With the cap, it >>approaches zero. With an appropriate resistor in series with the cap at the >>CT of the 50 ohms, it can be made to be zero. >> >> >>>The obvious drawback is parts count and board real estate. >>> >>>Regards >>>Mike >>> >>>Siders, Kenneth W wrote: >>> >>> >>>>Hello Group, >>>>My question concerns terminating an LVDS receiver with two 50 ohm resistors >>>> >>>> >>in series with a center tap capacitor to ground across the inputs of the >>receiver to achieve better common mode noise rejection? What type of >>improvement if any will I see. Also, are there any draw back with this type >>of termination. >> >> >>>>Regards, >>>>Ken >>>> >>>>Ken Siders >>>>Sr. Design Engineer >>>>Lockheed Martin MFC >>>>5600 Sand Lake Rd. >>>>MP 916 >>>>Orlando, FL 32819-8907 >>>>Phone: (407) 356-4891 >>>>Pager: (888) 363-3411 >>>>Fax: (407) 356-8944 >>>> >>>> >>>>Email: kenneth.w.siders@xxxxxxxx >>>> >>>> > > > > ------------------------------------------------------------ ------ To unsubscribe from si-list: si-list-request@xxxxxxxxxxxxx with 'unsubscribe' in the Subject field or to administer your membership from a web page, go to: //www.freelists.org/webpage/si-list For help: si-list-request@xxxxxxxxxxxxx with 'help' in the Subject field List archives are viewable at: //www.freelists.org/archives/si-list or at our remote archives: http://groups.yahoo.com/group/si-list/messages Old (prior to June 6, 2001) list archives are viewable at: http://www.qsl.net/wb6tpu ------------------------------------------------------------------ To unsubscribe from si-list: si-list-request@xxxxxxxxxxxxx with 'unsubscribe' in the Subject field or to administer your membership from a web page, go to: //www.freelists.org/webpage/si-list For help: si-list-request@xxxxxxxxxxxxx with 'help' in the Subject field List archives are viewable at: //www.freelists.org/archives/si-list or at our remote archives: http://groups.yahoo.com/group/si-list/messages Old (prior to June 6, 2001) list archives are viewable at: http://www.qsl.net/wb6tpu