Averagesupernova said:
Dividing the horizontal scanning frequency no matter what it is by 525 will get the vertical scanning frequency. The original 15750/525 results in 30 hertz.
now how do you get to 29.97 Hz?
Although I didn't mention it, after color came along the sound carrier was indeed an integer harmonic of the horizontal scanning frequency. (I took the liberty of making that red). Yes, the 286th harmonic of Fh is the sound carrier of 4.5 Mhz.
after the introduction of color. there was no integer relationship before.
227.5 has significance why? Well the color subcarrier is the 227.5th harmonic of Fh and obviously the .5 part is to get the sidebands to fall in between each other. Nothing new here.
they could have plopped the chroma baseband between the 228
th and 229
th f
H (puttting it a little closer to the sound carrier), but they had to make a decision between which 2 harmonics they were putting the chroma baseband and halfway between 227 and 228 is where they decided.
As to why they picked 3.579545 in general as in that general part of the spectrum? It has to fall far enough away from luminance sidebands (the majority of luminance information is in the lower frequencies) and far enough away from the sound carrier to prevent the beat frequency due to intermodulation within a TV sets stage from being too low to easily filter out. The beat frequency is about 920 Khz and is the difference between the sound carrier and the chroma subcarrier.
very good. but whether it's off by 920 or 917 kHz doesn't make that much difference
except for the interlacing of lines.
Yes, the spectrum does not look as it does in the link in post#14. That diagram is a simplification. I believe I mentioned that in my first post also. The information is concentrated in the sidebands spaced at Fh.
it needs to show the interlacing of luminance and chroma sidebands.
Number 1: If the sound carrier were an integer harmonic of Fh (which it actually is)
only because they chose to make it that way (by fudging f
H down from 15750 Hz to 4500000/286 Hz).
... it would fall directly on a luminance sideband. There isn't a lot of information in the high end of the luminance spectrum so I would think a little loss in the high end of it due to filtering out the sound carrier (imperfect filter) wouldn't be a big deal.
correct. but the chroma signal is closer to the sound carrier. a lot closer.
After all, they were already filtering it out with black and white sets.
otherwize we would see 286 columns of lighter and darker image on the BW TV, with no cancellation of alternate lines.
Number 2: If the sound carrier were and integer + 1/2 times Fh (which it isn't) the sound carrier would fall directly on a chroma sideband. Is this what you are getting at?
yes, and it's closer to the chroma signal than it is to the luminance. think from the POV of the choma signal (so the 227.5 x f
H is at "zero", the luminance carrier is at -227.5 x f
H and the sound carrier is up at +58.5 x f
H). that's good. both are offset by 1/2 f
H and whatever effect of either that leaks through will have cancellation in alternate horizontal lines. you won't see twisted bars of messed up color intensity or hue.
Although I've never looked into it, the comb filter may help filter this out since its phase will change by 180 degrees the same way the luma does relative to chroma when the sound carrier falls in between the chroma sidebands (case #1).
now you get it (i think). BTW, comb filters are things we build with a delay line of some sort. not a problem now (with digital memory), but they didn't really have them (for cheap) back in 1950 or 1960. the issue was what would be least objectionable in the picture if any of this *did* leak through any filtering. it is true that interlacing the chroma sidebands
exactly halfway between the luma sidebands is optimal for comb filtering them out. but i don't think comb filters were all that common back then. the issue is what would those frequency components that are offset by 1/2 f
H look like in your picture?
I don't know if this was the motivation to put the color subcarrier where it is or not. I can tell you that TV sets back in the day had traps in the IF for the sound carrier, the adjacent channel sound carrier, and the adjacent channel picture carrier. They knew the issues of keeping unwanted signals out of the IF before color came along. My guess is that they knew it was easier to comb filter what was left of the sound carrier out of the color signal and use LC filtering to get the sound carrier out of the luminance signal the same way they had been doing with black and white.
i don't know what you think they were using for comb filters back then. what was their delay element? a piece of transmission line that is 1/15734 second long? i don't think so.
comb filters are a relatively modern signal processing tool. it normally requires digitization and computer memory for the needed delay element. (maybe SAW - surface acoustic wave.)
I think this is the point you were trying to get across and I'm sorry I misread it. Incidentally, the reason that they couldn't bump the main picture carrier and sound carrier was compatibility issues. They needed to maintain a 4.5 Mhz spacing as you pointed out.
but it rubs two ways. with f
H reduced to 15734 Hz, the existing TVs had to lock on to a detuned f
H . evidently that was less of a problem than the FM sound receiver locking on to 4.5045 MHz. or maybe it was the fixed trap at 4.5 MHz.
I've found the Bernard Grob book (I have several older ones of that author too) to be sufficient. Curious about the Bruce Carlson book now. Not really curious enough to look for it though. LOL I assume you mean there are some good spectral diagrams and such with decent detail?
i just wanted something that shows the line spectra at multiples of f
H and the interlacing of chroma into the luminance way up there at 227.5 x f
H .