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- Date: Wed, 30 Mar 94 04:30:05 PST
- From: Info-Hams Mailing List and Newsgroup <info-hams@ucsd.edu>
- Errors-To: Info-Hams-Errors@UCSD.Edu
- Reply-To: Info-Hams@UCSD.Edu
- Precedence: Bulk
- Subject: Info-Hams Digest V94 #345
- To: Info-Hams
-
-
- Info-Hams Digest Wed, 30 Mar 94 Volume 94 : Issue 345
-
- Today's Topics:
- 10M indoor problem.
- CB Power meter
- FT-530 MOTD (Measurement of the Day -- Intermod!
- RF and AF speech processors. Was: FT-990 vs TS-850
-
- Send Replies or notes for publication to: <Info-Hams@UCSD.Edu>
- Send subscription requests to: <Info-Hams-REQUEST@UCSD.Edu>
- Problems you can't solve otherwise to brian@ucsd.edu.
-
- Archives of past issues of the Info-Hams Digest are available
- (by FTP only) from UCSD.Edu in directory "mailarchives/info-hams".
-
- We trust that readers are intelligent enough to realize that all text
- herein consists of personal comments and does not represent the official
- policies or positions of any party. Your mileage may vary. So there.
- ----------------------------------------------------------------------
-
- Date: 29 Mar 94 03:58:59 GMT
- From: ihnp4.ucsd.edu!agate!howland.reston.ans.net!news.moneng.mei.com!uwm.edu!reuter.cse.ogi.edu!netnews.nwnet.net!bach.seattleu.edu!quick!ole!rwing!eskimo!wrt@network.ucsd.edu
- Subject: 10M indoor problem.
- To: info-hams@ucsd.edu
-
- In article <CnDL5M.sC@gdss.grumman.com>, <higniro@gdss.grumman.com>
- wrote:
- >In article <1994Mar27.181416.165@news.unr.edu> destree@unr.edu (Louis
- Destree) writes:
- >> I recently bought a HTX-100 (no equipment flames please...buying
- >>the FT-990 would keep me from continuing school), and have set it up
- with
- >>a "V" type 1/2 wave indoor antenna. I have not been able to talk to
- >>anyone from my apartment yet. However, I have had good results (when
- the
- >>band is in) from a measly 1/4 wave mag mount on my car.
- >>
- >> The building I live in is made of stucco, with (I'm reasonably
- >>sure) chicken wire in the walls. Most stucco buildings I've seen have
-
- >>this wire in the walls. I am curious if the wire is acting as an
- >>attenuator. If anyone has had a similar experience, let me know.
- >>
- >> Yes, it is possible for me to put the antenna outside. However,
- >>rather than having people lining up at my door complaining of TVI, I
- >>wanted to keep everything indoors.
- >> Thanks!
- >> Louis
- >>
- >>--
- >>Louis A. Destree University of
- Nevada, Reno
- >>destree@equinox.unr.edu <> destree@equinox.bitnet Electrical
- Engineering
- >>Amateur Radio: N7XNX (General Class) Bike: 1980 Honda
- CB750C
- >> "When things go from bad to worse, the cycle will repeat itself!"
- >
- >
- >The trick to TVI complaints from neighbors is to put up the external
- >antenna and not operate for 30 days or so. This will weed out the true
- >TVI problems and problem neighbors......
- >
- >Rod - KB3MK
-
-
- Chicken wire is a RF killer for sure. KB3MK's suggestion is a good one,
- but second best is an attic antenna (above the chicken wire!). A 10
- meter dipole will fit easily and work like a charm. Just keep it away
- from anything metal and if there are phone wires, etc, try to run it ant
- a 90 degree angle to them if possible. I worked DXCC with 100 watts and
- an attic antenna. Have fun!
-
- 73 es gl
-
- Bill, W7LZP
-
-
- ------------------------------
-
- Date: 30 Mar 94 07:30:07 GMT
- From: dog.ee.lbl.gov!agate!howland.reston.ans.net!usc!crash!mauricio@ucbvax.berkeley.edu
- Subject: CB Power meter
- To: info-hams@ucsd.edu
-
- Hello everyone, I have a question concernong measuring power output from
- a ramsy FM-10, I have a RADIO SHACK CB Power meter 3 - 30 mhz(its what it
- said on the box), and i just want to know if hooking this up to my fm-10
- will give me an accurate power reading or not, if not how can i convert
- this reading to that of what i want? The meter goes between the Xmiter
- and the antenna. Any help would be appreciated.
-
- thanx
- mauricio@crash.cts.com
-
- ------------------------------
-
- Date: 29 Mar 94 02:58:46 GMT
- From: dog.ee.lbl.gov!agate!kabuki.EECS.Berkeley.EDU!kennish@ucbvax.berkeley.edu
- Subject: FT-530 MOTD (Measurement of the Day -- Intermod!
- To: info-hams@ucsd.edu
-
- OK, UHF measurements for sensitivity and intermod....
-
- Raw F3E sensitivity (opens squelch set at threshold):
-
- UHF receiver (right side):
-
- Freq (MHz) Pin (dBm)
-
- 300 -83
- 315 -96
- 330 -105
- 345 -111
- 360 -117
- 375 -122
- 390 -122
- 405 -121
- 430 -122
- 445 -122
- 460 -120
- 475 -119
- 490 -115
- 500 -114
-
- VHF receiver (left side):
-
- PLL does not lock for 300 MHz:
-
- Freq (MHz) Pin (dBm)
-
- 300 x
- 315 -74
- 330 -74
- 345 -77
- 360 -71
- 375 -84
- 390 -100
- 405 -100
- 430 -118
- 445 -122
- 460 -115
- 475 -105
- 490 -104
- 500 -104
-
- TTID (Twin Tone Intermod)
-
- f1 = 445 MHz, f2 = 446 MHz, tune 447 MHz for 3rd IM:
-
- breaks squelch at -66 dBm on UHF side, -69 dBm on VHF
- side.
-
- f1 = 475 MHz, f2 = 460 MHz, tune 445 MHz for 3rd IM:
-
- breaks squelch at -59 dBm. NO VHF side measurement (sorry).
-
-
- What this means: For best IM rejection, listen to UHF on
- the VHF side! As advertised in the manual, cross band RX
- has a narrower range, and hence better out of ham band IM
- rejection. Didn't test this on the bench, sorry, but
- remember that 1 dB of RF attenuation drops the 3rd IM
- products by 3dB......
-
-
- More numbers when I have time, next will be VHF sensitivity
- and IM rejection, followed by UHF+ (800 MHz) measurements.
-
- People that are dying for a particular measurement can
- mail me and I will try to set it up.
-
-
- -Ken
-
- p.s for those that must know, my FT-530 has the Jumper
- 13 mods done, and the serial number begins with 3D131...
-
- ------------------------------
-
- Date: Tue, 29 Mar 1994 14:34:44 GMT
- From: ihnp4.ucsd.edu!dog.ee.lbl.gov!agate!howland.reston.ans.net!europa.eng.gtefsd.com!emory!wa4mei!ke4zv!gary@network.ucsd.edu
- Subject: RF and AF speech processors. Was: FT-990 vs TS-850
- To: info-hams@ucsd.edu
-
- In article <CnE4xu.I03@srgenprp.sr.hp.com> alanb@sr.hp.com (Alan Bloom) writes:
- >Gary Coffman (gary@ke4zv.atl.ga.us) wrote:
- >: In article <Cn8Los.3Ln@srgenprp.sr.hp.com> alanb@sr.hp.com (Alan Bloom) writes:
- >: >Gary Coffman (gary@ke4zv.atl.ga.us) wrote:
- >: >
- >: >: Phfffft! The phase flatness through the audio phase shift networks
- >: >: used in amateur phasing SSB rigs was much worse than any phase
- >: >: distortion in a filter rig. The audio phasing network had to cover
- >: >: octaves while the crystal filter only has to work over a tiny fraction
- >: >: of an octave.
- >: >
- >: >Not true. A phasing-type SSB generator specifically depends on a
- >: >90 degree phase difference between the two channels. If the phase
- >: >flatness were bad, you would get terrible unwanted sideband supression.
- >
- >: No. Phasing exciters depend on *quadrature* at a given frequency to
- >: achieve SSB.
- >
- >*Sigh* Here we go again...
- >
- >"Quadrature" means exactly what I said above, a 90 degree phase difference.
-
- I know that. I'm not arguing with you, just introducing an alternate
- term for the I and Q channel phase relationship. Where I am arguing
- with you is on a slightly subtle point. See below.
-
- >: There must be a net 90 degree difference *at any given
- >: frequency*, but the phase at say 300 Hz vis 3000 Hz is irrelevant
- >: to the SSB generation, but not to the sound.
- >
- >True, but the way 90-degree phase shift networks work is to generate
- >two signals with phases that ramp linearly with frequency, but always
- >90 degrees out of phase. If the ramps weren't smooth, the phase
- >difference wouldn't be 90 degrees.
-
- Now this is where we differ. What's important to phasing SSB is that
- I - Q = 90 degrees at each given frequency. You can have that with
- an irregular frequency response as easily as you can with a smooth
- declining ramp. What I'm talking about is the phase relationship
- between different frequency components of the waveform. Let's assume that
- we have two frequencies X and Y. They will have a phase relationship at
- input defined as,
-
- X(t) - Y(t) = K(t)
-
- Now if we put this through a transmission media, a blackbox
- network we'll call B, then the following condition must apply
- if the phase relationship of the complex waveform is to be
- maintained.
-
- B(X)(t) - B(Y)(t) = K(t)
-
- But that's not the response we get with a first order smooth
- RC network with a declining linear phase delay versus frequency.
- I and Q have to have a 90 degree difference, but that can be
- generated a number of different ways. We can add delay in one
- branch only, so I' = I and Q' = Q + 90. Or we can use lead/lag
- networks so that I' = I + 45 and Q' = Q - 45. Or any mixture
- in between. All the SSB phasing network cares about is that
- there's quadrature at each given frequency. How each frequency
- gets quadrature is irrelevant to the phasing exciter, but it's
- not irrelevant to the resulting differential phase between two
- frequency components of the input.
-
- >: Ask yourself how many
- >: milliseconds is a 90 degree phase delay at 300 Hz, then ask yourself
- >: how many at 3000 Hz. ...
- >
- >That's why there is less phase shift at 300 Hz than 3000 Hz (phase ramps
- >linearly with frequency, see above.) Linear phase = constant group delay.
-
- I don't see what you're saying here. You need quadrature at every different
- frequency, at 300 Hz and at 3000 Hz. The phase shift has to be the *same*
- at every frequency (90 degrees), but that means the *delay* declines with
- increasing frequency since it takes less delay to get 90 degrees of phase
- shift at 3000 Hz than it does at 300 Hz. In other words, the high frequency
- components start to outrun the low frequency components as they go through
- the network because they suffer less delay. That can be seen in a television
- system as chroma/luminance misregistration, also known as differential
- phase distortion. Such delay characteristics aren't easily visible in
- complex audio waveforms with ordinary scopes, but it certainly can be
- heard. That's the click-boom effect I mentioned in the first post where
- a percussive strike's high frequency components have outrun the low
- frequency components.
-
- >: >Same thing with amplitude flatness. The phase shift network's two
- >: >channels must be matched to within a fraction of a dB to get good sideband
- >: >suppression.
- >
- >: Same thing with amplitude flatness. The amplitude has to match *at
- >: a given frequency* ...
- >
- >Again, the way to get amplitude matching is to make both channels flat.
-
- It's *a* way to do that, but it's not necessary, or likely in real
- circuits. All that's necessary for the SSB phasing exciter is that
- I and Q have the same amplitude at any given frequency. There could
- be many db of amplitude difference between two different frequencies
- in either the I or Q channel as long as the same difference exists
- in the complementary channel at that frequency. In other words, the
- bandpass amplitude response could be very lumpy as long as the lumps
- in both I and Q match. In fact, with a first order RC network, the
- response is going to change by 3 db per octave.
-
- >: >A typical SSB crystal filter has a couple dB peak-to-peak ripple across
- >: >the passband with similar ripples in the group delay. It is easy to
- >: >do much better than that with a phasing-type exciter.
- >
- >: How much time is a few degrees of phase shift at 9 MHz? How much effect
- >: does that have on a 300 Hz waveform? One 9 millionth of a second is a
- >: mighty small phase shift at 300 Hz.
- >
- >Doesn't matter -- the delay through a filter depends on the bandwidth,
- >not the center frequency. For example, if you built a 9 MHz crystal
- >filter with a fraction of a Hz bandwidth, you would have SECONDS of
- >delay through the filter. A 9 MHz SSB filter will have similar group
- >delay as an audio filter of similar bandwidth and rolloff characteristics.
-
- I've been scratching my head over this. Since the percentage bandwidth at
- 9 MHz is so small, the Q has to be much higher which translates into more
- filter ringing than in the very broad percentage bandwidth AF delay network.
- But it seems to me that the differential delay of the lower Q audio filter
- would be greater since the delta time span for a 90 degree phase shift is so
- much greater for a 5 octave span than for a fraction of an octave span.
- Perhaps they equate to the same percentage distortion, but is it the same
- *kind* of distortion?
-
- Gary
- --
- Gary Coffman KE4ZV | You make it, | gatech!wa4mei!ke4zv!gary
- Destructive Testing Systems | we break it. | uunet!rsiatl!ke4zv!gary
- 534 Shannon Way | Guaranteed! | emory!kd4nc!ke4zv!gary
- Lawrenceville, GA 30244 | |
-
- ------------------------------
-
- Date: Tue, 29 Mar 1994 14:39:25 GMT
- From: ihnp4.ucsd.edu!dog.ee.lbl.gov!agate!howland.reston.ans.net!europa.eng.gtefsd.com!emory!wa4mei!ke4zv!gary@network.ucsd.edu
- To: info-hams@ucsd.edu
-
- References <Cn15pI.L7H@news.Hawaii.Edu>, <2n7901$6n4@apple.com>, <CnECJu.2L0@news.Hawaii.Edu>
- Reply-To : gary@ke4zv.UUCP (Gary Coffman)
- Subject : Re: 1x1 Callsigns?
-
- In article <CnECJu.2L0@news.Hawaii.Edu> jherman@uhunix3.uhcc.Hawaii.Edu (Jeffrey Herman) writes:
- >
- >Kok: Know who first used `iff' in the literature? Hint: He used to be
- >Chairman of the U.H. Math Dept. (didn't stay long, though...) and he
- >is quite famous. [VERY big hint: his intials are P.H.]
-
- PAUL HARVEY used to be chairman of the UH math department???
-
- Gary
-
-
- :-)
-
- --
- Gary Coffman KE4ZV | You make it, | gatech!wa4mei!ke4zv!gary
- Destructive Testing Systems | we break it. | uunet!rsiatl!ke4zv!gary
- 534 Shannon Way | Guaranteed! | emory!kd4nc!ke4zv!gary
- Lawrenceville, GA 30244 | |
-
- ------------------------------
-
- End of Info-Hams Digest V94 #345
- ******************************
- ******************************
-