Re: k1 pixel shift - can you see the different?
3
flektogon wrote:
James O'Neill wrote:
So if the K1 sensor could resolve 3680 Monochrome light and dark line pairs over its width, (i.e. 7360 pixels) and the lens can also resolve 3680 light/dark pairs over that width, (i.e. both resolve a line 1/200th mm wide) the finest line we can see in the output is 1/100th mm wide. (This is sometimes quoted as 1/image_res = 1/lens_res + 1/recording_res) . So your theoretical "36M detail" lens and a 36MP sensor can only resolve 9 million ~details.
James, that formula is perfectly valid for a combination of lens and film! But not for the digital film (i.e. sensor). If a given lens can deliver the same amount of details as is the sensor pixel count, it is possible that all those details will be recorded. but...
Imagine that the lens is projecting on a sensor a board with black-and-white fields (like a chess board) having together 36 million fields.
It doesn't work like that. The resolution of a lens is not perfect up so many line pairs per mm and then grey mush.
Imagine six chessboards. suck together to form a 24 x 16 square grid. 192 black squares and 192 white ones. When the lens forms an image of that the transition from white to black isn't perfect / instantaneous. A little of the light that should be in a white square spills into the 4 neighbouring black squares. But if this the whole of a 36x24 image with each square will be 1.5 mm wide and 1.5mm tall and I was talking about a lens with a blur of 0.002 mm So we have a smudge which is 0.1333% of the square width/height Really easy to resolve black and white squares.
Now make it 600 chessboards 240x160 squares. 19,200 black and white Now each square is .15 mm wide with a .002mm smudge. 1.3% Still easy to tell black from white.
Same again to give 2400 x 1600 squares , 1,920,000 each of black and white 0.015mm wide with a 0.002 mm smudge. 13% of the width. Still OK
Lets go to 4800 x 3200 , 7,680,000 black/white . with , 0.0075 wide with a 0.002 mm smudge. Now its getting hard to see the blacks and whites they're smaller (.0035mm) than the transitions (0.004mm) but there are still blacks and whites to see.
Lets go to 9600 x 6400 , 15,360,000 black/white . with , 0.00375 wide with a 0.002 mm smudge. Now smudges meet and we can no longer resolve the pattern.
If such a subject was perfectly projected on (aligned with) the sensor pixels, all 36 million fields will be recorded. One field, one pixel.
As the Spartans famously said IF.
If we are right at the resolution limit for the lens ANY imperfection, 1/1000th of a pixel width horizontally or vertically, means the can no longer resolve the 36 million fields.
And where with the image even at 0.0075 squares with a 0.002 mm smudge, we still get spots of maximum black and maximum white, on a digital sensor, perfectly aligned we get 80% in white squares and 20% in the black ones. We normally say a 50% difference between "black" and "white" is "resolved" so it doesn't take much offset to bring it down to 75-25.
The average offset is 1/4 pixel horizontally and 1/4 vertically. So even if the grid projected had perfect dots with no smudge, on average the white dots would get 3/4 x 3/4 = 9/16 of the light. So the blacks would be 7/16. I.e. 2n MP sensor can't resolve n million back and n million white dots.
Of course, just a half point shift in both dimensions and you would get just one, gray field. So, statistically you can record 18 mega details. Well, this "statistics" may not be valid as it is my invention ,
Back to basics,
some of the light from white squares falls in black squares due to lens imperfections, diffraction etc.. The amount determines how small the squares or lines can be and still be resolved
Additional light from white squares falls in black squares due to misalignment with pixel boundaries. This also determines the smallest square or thinnest line.
"Smudge" from the lens is 1/Lines_per_mm
"Smudge" from the recording medium is also 1/Lines_per_mm
So add them and you get the total smudge, and 1/total_smudge is effective lines per mm.