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From: "nanchez" on Fri 3 Jun 2005 14:59
I'm doing some RF experimentation and I need to know the "relation" between dBm specificatons and voltage level for a signal. I have a RF mixer with a specification that says: LO drive level (50 ohm) = -16 dBm And I have a LO source that give me an output of 2.5Vpp to a capacitive load of 5pF at 40MHz. How can I relate both items and design a circuit to connect LO source to RF mixer ? A basic definition that is industry-wide, government-wide, has "dbm" as decibels of "0 dbm" related to a power level of 1.0 milliWatts in a "50 Ohm system." That has become so widespread that specification writers don't always include those words. It is implicit when referring to RF components. The RMS voltage can be quickly calculated from some identities on the basic formula for Watts: P = E x I. Knowing R (50 Ohms) one can substitute Ohm's Law of Resistance of I = E / R into that to get E = SquareRoot (P x R). For 1.0 mW in a 50 Ohm system, P x R = 0.050 and the square root of that is 0.2236 so 0 dbm has an RMS voltage of 223.6 milliVolts. In your mixer specification, -16 dbm is equal to 35.44 mV RMS across a resistance of 50 Ohms. You can't DIRECTLY use your 40 MHz source value of 2.5 V peak-peak across a 5.0 pFd capacitance because it does not include the characteristic RESISTIVE impedance of 50 Ohms. Power in Watts must be related to the impedance of a load in order to perform "work." [a basic definition of power in Watts is "a unit of work"] Capacitance across a load will vary its impedance depending on the frequency. For that reason the electronics industry has long relied on a basic resistive impedance to measure and characterize RF components. The result is the very common "dbm" referred to 1.0 mW across a resistive 50 Ohm load...or the characteristic impedance of the measurement system, both source and load impedance. To relate your mixer specification to your RF source, you will have to put a 50 Ohm load across the source and measure that. If you have some stray capacitance across that load (inevitable) and know approximately what that is, you can calculate its effect across a resistance. At 40 MHz a 5.0 pFd capacitance has a reactance of 796 Ohms. That is not much but it changes the magnitude of the parallel R-C from 50.0 Ohms resistive to 47.0 Ohms slightly capacitive. That's a small change and can generally be neglected for experimental bench work. If you have some web source to study about this items, I'll be glad to hear about it. It's in practically every textbook on the subject of RF electronics. What can confuse newcomers to RF is the implicit "standard" which is not always included in specification sheets. The definition of "dbm" is arbitrary and probably picked (way back in time) for sake of convenience in measurement by all concerned. The reason for picking "50 Ohms" in a "system" is more obscure and ties into the physics of power transfer in coaxial cables. That's a curiosity that some can look up if they are interested but does not apply to how to USE the "dbm" specifications. To use "dbm" one only needs to remember the definition and apply simple forumulas for Power and Ohm's Law of Resistance. I hope that was of some help to you. |
#12
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From: "nanchez" on Fri 3 Jun 2005 14:59
I'm doing some RF experimentation and I need to know the "relation" between dBm specificatons and voltage level for a signal. I have a RF mixer with a specification that says: LO drive level (50 ohm) = -16 dBm And I have a LO source that give me an output of 2.5Vpp to a capacitive load of 5pF at 40MHz. How can I relate both items and design a circuit to connect LO source to RF mixer ? A basic definition that is industry-wide, government-wide, has "dbm" as decibels at "0 dbm" related to a power level of 1.0 milliWatts in a "50 Ohm system." That has become so widespread that specification writers don't always include those words. It is implicit when referring to RF components. The RMS voltage can be quickly calculated from some identities on the basic formula for Watts: P = E x I. Knowing R (50 Ohms) one can substitute Ohm's Law of Resistance of I = E / R into that to get E = SquareRoot (P x R). For 1.0 mW in a 50 Ohm system, P x R = 0.050 and the square root of that is 0.2236 so 0 dbm has an RMS voltage of 223.6 milliVolts. In your mixer specification, -16 dbm is equal to 35.44 mV RMS across a resistance of 50 Ohms. You can't DIRECTLY use your 40 MHz source value of 2.5 V peak-peak across a 5.0 pFd capacitance because it does not include the characteristic RESISTIVE impedance of 50 Ohms. Power in Watts must be related to the impedance of a load in order to perform "work." [a basic definition of power in Watts is "a unit of work"] Capacitance across a load will vary its impedance depending on the frequency. For that reason the electronics industry has long relied on a basic resistive impedance to measure and characterize RF components. The result is the very common "dbm" referred to 1.0 mW across a resistive 50 Ohm load...or the characteristic impedance of the measurement system, both source and load impedance. To relate your mixer specification to your RF source, you will have to put a 50 Ohm load across the source and measure that. If you have some stray capacitance across that load (inevitable) and know approximately what that is, you can calculate its effect across a resistance. At 40 MHz a 5.0 pFd capacitance has a reactance of 796 Ohms. That is not much but it changes the magnitude of the parallel R-C from 50.0 Ohms resistive to 47.0 Ohms slightly capacitive. That's a small change and can generally be neglected for experimental bench work. If you have some web source to study about this items, I'll be glad to hear about it. It's in practically every textbook on the subject of RF electronics. What can confuse newcomers to RF is the implicit "standard" which is not always included in specification sheets. The definition of "dbm" is arbitrary and probably picked (way back in time) for sake of convenience in measurement by all concerned. The reason for picking "50 Ohms" in a "system" is more obscure and ties into the physics of power transfer in coaxial cables. That's a curiosity that some can look up if they are interested but does not apply to how to USE the "dbm" specifications. To use "dbm" one only needs to remember the definition and apply simple forumulas for Power and Ohm's Law of Resistance. I hope that was of some help to you. |
#13
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#14
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![]() "Wes Stewart" wrote in message ... On Sat, 4 Jun 2005 14:53:43 +0100, "john jardine" wrote: "nanchez" wrote in message oups.com... Hi. I'm doing some RF experimentation and I need to know the "relation" between dBm specificatons and voltage level for a signal. I have a RF mixer with a specification that says: LO drive level (50 ohm) = -16 dBm And I have a LO source that give me an output of 2.5Vpp to a capacitive load of 5pF at 40MHz. How can I relate both items and design a circuit to connect LO source to RF mixer ? If you have some web source to study about this items, I'll be glad to hear about it. Thanks Hernán Sánchez To rejoin the real world, take the "16" figure and divide it by 20. get "0.8" Then find the antilog of that 0.8 [use normal 'base10' logs] get "6.31" This number is a multiply or divide factor that is applied to a 50 ohm 0dBm reference voltage. So what is this god like reference voltage?. The 50ohm 0dBm reference voltage is in actual fact 0.223Vac. The original number was "-"16 dBm. Just read the minus sign as meaning a voltage less than the 0dBm reference voltage. So that 0.223Vac reference value is divided by your 6.31 factor. get "0.035" Vac. So "-16dBm" is really 35mVac. This means you have more than enough drive voltage available from your 2.5Vpp (900mVac) local oscillator signal. Except neither you or Hernan can be sure of this. His source is not specified to work into a 50 ohm load or present a 50 ohm source impedance to the mixer (what is really needed). Who knows what the delivered voltage will be when driving the mixer port? A measurement is in order. Terminate the source in 50 ohm and measure the power and/or voltage. If it exceeds -16 dBm, attenuate accordingly. I imagine we would both have read Hernans post the same way. I.e that he has some logic running at 40MHz and is seeing a rough 2.5Vpp sinewave on his 50-100MHz oscilloscope via a 10:1 probe. From this I'd also assume we both knew that the logic drive impedance would be a couple hundred ohms at the most and that serious mis-matching was not going to be a problem. I'd though, suggest he just connects the parts together and see what happens. He's experimenting. Monitoring the results (good or bad) is just part of the due process. Doesn't look like he's got a spectrum analyser, so how can he validate a 50ohm test measurement as exceeding -16dBm?. His sticking point was specifically about the link between Dbs and Volts. A common, basic electronics question yet surprisingly badly answered by the original suggested link, which started off with the concept of a "dimensionless gain" and went downhill from there using 3 pages of sums. How many radio hams talk to each other about their TX powers in terms of (ISO standard) units of dBs wrt one watt?. Why do the filter tables tell me a Cheb' filter ripple is in dBs when all I want is percent values. Why do my function generators handbooks tell me the sine THD is 0.2% upto 200kHz but beyond that the distortion suddenly becomes an obscure "-30db wrt the fundamental". A recent EW magazine article for a AC mV meter said the response was flat within 0.0024dB. How flat is that?. Be very wary whenever you come across dBm figures. There is a minefield of disinformation out there. In many cases they are intended purely to obfscutate the reader and prevent them clearly seeing that the described circuit is junk. Spoken like a real expert on bafflegab. Indeed, the word was intended that way (UK English). regards john |
#15
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From: Roy Lewallen on Sat, 04 Jun 2005 14:06:41 -0700
wrote: A basic definition that is industry-wide, government-wide, has "dbm" as decibels of "0 dbm" related to a power level of 1.0 milliWatts in a "50 Ohm system." That has become so widespread that specification writers don't always include those words. It is implicit when referring to RF components. . . . That's common in the RF industry, but many others also use dBm -- for example, it's often used in video systems where the standard impedance is 75 ohms, and others where the standard is 600 ohms. In all those applications, dBm is universally defined and understood to mean dB relative to 1 mW, regardless of the impedance. Quite true, Roy. :-) I restricted myself to "50 Ohms" for a couple of reasons: As far as "pure" RF components go, 50 Ohms is the Z characteristic; I didn't want to complicate my explanation. The TV Cable industry is HUGE and they use 75 Ohms. However, so many radio amateurs run around snarking on "TV" that it could have raised a lot of unneccessary babbling in here. :-) TV cable is digital in some locations (ours is in the SF Valley of L.A.) and has more TV channels crammed into the same VHF-UHF space than old analog TV. Don't know the modulation of my digital TV cable signals, whether it is wider or narrower than analog channels...but my TV service crams over 400 channels into the same bandwidth. TV sure isn't the narrow-band stuff that many hams are used to. "dbv" (sometimes "dbu" but rarely) refers "0" as 1.0 microVolt, almost any characteristic. Not seen much in specifications, though. The "VU" (for Volume Unit) is an old, old one in the audio and telephone industry with "0 VU" being 1.0 mW into 600 Ohms impedance. Not only that, the "VU" industry standard used to call out the indicating meter's ballistic (needle or meter motor) characteristics! :-) "dbc" is an often-used term on component specifications but is still a relative term of db in regards to the Carrier of a signal where the noise is called out. ["C" for Carrier] "dba" is a legal term in the USA standing for "Doing Business As" in local governments that require business licenses. :-) My apologies if some ISPs show two more postings of my message. When I posted via Google on Saturday early afternoon, Google was interrupting itself with lots of users (?) or something that kept prompting "server error." I've since removed redundant posts on Google, but some other ISPs may be storing the multiples. Stuff happens. |
#16
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#17
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#18
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I've never seen "dBv" refer to 1uv either. Always 1V.
Joe W3JDR "Roy Lewallen" wrote in message ... wrote: . . . "dbv" (sometimes "dbu" but rarely) refers "0" as 1.0 microVolt, almost any characteristic. Not seen much in specifications, though. . . . Interesting. I've many times seen dB relative to one volt as dBV, and dB relative to one microvolt as dBuV, but never dBv meaning dB relative to one microvolt, or dBu at all. Do you have any references that show these unusual usages? Roy Lewallen, W7EL |
#19
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#20
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This page: http://decibel.biography.ms/ mentions both dBv and dBu.
Says in "electrical voltage" (probably with reference to audio industry), dBu and dBv both mean dB relative to 0.775V -- generally 0.775Vrms, but dB taken as 20 log(V/0.775), without reference to a particular impedance. But the same page says dBu or dB(lower-case Greek mu: "micro") as radio power is dB relative to one microvolt per square meter. Go figure. It all points out the need to be careful to define your terms if there's any chance of ambiguity. If you're not careful, your reader may think dBu refers to Dallas Baptist University, or Deutsche Billiard Union, or Duluth Business University... though the capitalization would be wrong for those. Cheers, Tom |
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