High School Huygens Question - Using a Pinhole Box in the Giant Pinhole Irvine

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The discussion centers on the functionality of a shoebox pinhole camera when used inside the Giant Irvine pinhole camera. It is clarified that the shoebox camera, when pointed at the light source, will only capture a small image of the lower portion of the scene, primarily ground features, due to the limitations of light reaching the pinhole. The image produced will be dim and potentially indistinct, as it is occluded by the larger camera's aperture. Participants emphasize that no magical replication of the entire scene occurs; instead, the image is a tiny spot reflecting what is geometrically in line with the pinhole. Overall, the principles of light travel in straight lines and the effects of diffraction are key to understanding the limitations of the shoebox camera's output.
  • #31
ndvcxk123 said:
Thx for the corrections. Amazingly, looking through my own pinhole shoebox ab. a month ago, I did not remember it being inverted. (Hence the diag. error). Re focusing, it is interesting though, that it become less sharp if the aperture is widened (due to addit. light entry).View attachment 329844
There's a problem with that diagram. It appears that the small camera is actually looking at the front of the big camera, which has just a small bright spot in it. The brightness of that spot corresponds to the brightness of the scene in that direction.
We (or at least some of us) may have been talking at cross purposes. What was the actual question - in the light of that possible mis-understanding?
 
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  • #32
The fundamental misunderstanding in this thread is manifest in the title. The Huyghens construction (and in fact any diffractive effect) has essentially nothing to do with this analysis because of the sizes involved. Strictly Ray optics... one needs only a ruler and notion of aperture area. All else is irrelevant.
 
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  • #33
hutchphd said:
The fundamental misunderstanding in this thread is manifest in the title. The Huyghens construction (and in fact any diffractive effect) has essentially nothing to do with this analysis because of the sizes involved. Strictly Ray optics... one needs only a ruler and notion of aperture area. All else is irrelevant.
Lensless imaging is a hot topic in some quarters of google searches. This link and this link would suggest that the optimum pinhole size includes consideration of diffraction as well as ray geometry. For 200mm deep camera the optimum pinhole size is about 0.5mm so, although an impractical design (far too dim images) it's worth thinking about and not completely irrelevant.
 
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  • #34
For the situation described I will respectfully disagree.
One of the hallmarks of the art piece described is its mammoth size.
Using your numbers for the small camera the pinhole angular resolution limit ~.5/200=1/ 400 but the diffraction limit for 500nm (bluegreen ) light will be ~500nm/0.5mm=1/1000 so it would not be high on the list. (Honestly it is bigger than I had anticipated!!)
 
  • #35
sophiecentaur said:
Lensless imaging is a hot topic in some quarters of google searches. This link and this link would suggest that the optimum pinhole size includes consideration of diffraction as well as ray geometry. For 200mm deep camera the optimum pinhole size is about 0.5mm so, although an impractical design (far too dim images) it's worth thinking about and not completely irrelevant.
I would agree. The OP seems to be on a learning curve when it comes to optics and pinhole cameras, (as well as diffraction theory), but we should not discourage him from getting what he can out of what should be a good learning experience.

Edit: To comment on post 34, which I just saw=the OP should soon figure out if he hasn't already, that there is little to gain by using a pinhole camera on the image of another pinhole camera. In any case, he picked a good topic, and we ought to be able to at least point out a couple of things of interest for him.
 
  • #36
Charles Link said:
I would agree. The OP seems to be on a learning curve when it comes to optics and pinhole cameras, (as well as diffraction theory), but we should not discourage him from getting what he can out of what should be a good learning experience.
But getting the picture the right way round is pretty important. What is he trying to image with the small camera? Is it an image of a pinhole or an image of the large camera image? This is not a mere detail imo.
 
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  • #37
sophiecentaur said:
But getting the picture the right way round is pretty important. What is he trying to image with the small camera? Is it an image of a pinhole or an image of the large camera image? This is not a mere detail imo.
Or even the scene with the first camera absent. From what I can gather, he seems to want to try all 3 cases, and see if there is something of interest for each.
 
  • #38
sophiecentaur said:
Lensless imaging is a hot topic in some quarters of google searches. This link and this link would suggest that the optimum pinhole size includes consideration of diffraction as well as ray geometry.
This was covered in #2:
Charles Link said:
Diffraction effects with a very small aperture can make for some blurring, but if the pinhole is too large, you also get reduced resolution, because of blurring determined by a point source making a finite sized spot from geometric optics when the aperture is finite. In general, there is an optimal aperture size, where diffraction effects are minimal, and where the spot size from a point source using geometric optics (i.e. using the straight line principle=the aperture shows up on the screen, etc. using ray tracing ) is also reasonably minute.

From the article linked in #1:
A seamless piece of muslin cloth was made light sensitive by coating it with 21 US gallons (80 l) of gelatin silver halide emulsion and then hung from the ceiling at a distance of about 80 feet (24 m) from a pinhole, just under 6 millimeters (0.24 in) in diameter
From the aperture size calculator linked in #33:
Focal length of camera in millimeters 24000
Optimal pinhole size: 5.7... mm

But none of this affects the key point that the image you get can be simply determined by ray tracing (it just means that the image is blurred due to (1) rays from opposing extremes of the aperture hitting the screen at different points and (2) individual rays forming diffraction patterns. The smaller you make the aperture the better you make (1) but the worse you make (2) as well as image brightness (increasing exposure time), and vice versa.
 
  • #39
pbuk said:
The smaller you make the aperture the better you make (1) but the worse you make (2) as well as image brightness (increasing exposure time), and vice versa.
That point was already made and there are links quoted with some actual figures.
As for diffraction limiting image quality, that's clear because astrophotography (and observing) requires apertures as big as your can afford.
 
  • #40
hutchphd said:
For the situation described I will respectfully disagree.
After thinking more about the OP, I have to agree that the whole scheme has very modest requirements for resolution. My comments were basically about squeezing the last juice from the imaging lemon so we can ignore diffraction in this project. in fact, the 'pinhole' should to be as big as possible, consistent with the acuity of the viewers and their distance from the screen - i.e the old 'five times picture height' rule for viewing distance with standard definition TV would set the size of hole for best picture brightness / sharpness tradeoff. The Irvine 4mm (?) camera hole may have got it fairly right. But this appears to have been more of a 'record breaking stunt'. The resolution would not have been very special, with brightness the more important for impressiveness.
 
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  • #41
hutchphd said:
The fundamental misunderstanding in this thread is manifest in the title. The Huyghens construction (and in fact any diffractive effect) has essentially nothing to do with this analysis because of the sizes involved. Strictly Ray optics... one needs only a ruler and notion of aperture area. All else is irrelevant.
Well, I wondered whether sampling with a small opening might recreate the full wave entering...
 
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  • #42
sophiecentaur said:
But getting the picture the right way round is pretty important. What is he trying to image with the small camera? Is it an image of a pinhole or an image of the large camera image? This is not a mere detail imo.
Well, was not sure what the result would be....
 
  • #43
ndvcxk123 said:
Well, I wondered whether sampling with a small aperture might recreate the full wave entering...
You would need to explain that more fully. I have made assumptions:

There is a tradeoff between aperture and resolving power. The smaller the aperture, the wider the diffraction pattern. Assuming you could describe the resultant wave from light entering from all across a scene then a tiny aperture would not allow discrimination between light from all the different elements of the scene. So you'd just get a (slightly weighted) value at one emerging angle from your small aperture which is a sum of light flux from all different directions.
The nearest thing to the "full wave entering" would be obtained with a massive aperture.
 
  • #44
sophiecentaur said:
But getting the picture the right way round is pretty important. What is he trying to image with the small camera? Is it an image of a pinhole or an image of the large camera image? This is not a mere detail imo.
Re learning curve: After constructing first pinhole shoebox cam, find that it works, but I'm running out of breathing air quickly closing black coat around it + my head ! :) The other aspect interesting me is image reflection w. out a lens, bec. still, from the middle of the image there are just slightly diagonal lines which should cover the other middle objects. However, pinhole images, while weak, are still really precise. To me, that's surprising.
 
  • #45
Pinhole cameras are a lot of fun and useful teaching tools, but are really quite simple. Here is how they work:

Light from the object travels in straight line through the hole to the image.

That's all you need to know 99.9% of the time
 
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  • #46
ndvcxk123 said:
However, pinhole images, while weak
"Weak"? In terms of galactic distances, the James Webb Space Telescope is a pinhole. You can hardly say that's weak when it gets us back to the formation of the Universe. :wink:
JWST does need some very long exposures to get there, though.
 
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  • #47
hutchphd said:
Pinhole cameras are a lot of fun and useful teaching tools, but are really quite simple. Here is how they work:

Light from the object travels in straight line through the hole to the image.

That's all you need to know 99.9% of the time
 
  • #48
hutchphd said:
Pinhole cameras are a lot of fun and useful teaching tools, but are really quite simple. Here is how they work:

Light from the object travels in straight line through the hole to the image.

That's all you need to know 99.9% of the time
"The straight line" you mention is part of the standard description. But (sorry), it seems to me to be inadequate, or too symbolic. Consider the roof tiles, tow. center. Take one of the tiles. The space next to it is another tile. Would you not accept that light from the first, at equal intensity, also covers the left and right tile ? Should we not say that cones (small though they are) enter the aperture ? Too me, it seems that each source object throws a cone of light larger than the pinhole, i.e. each feature reflection covers the pinhole completely +causes entry of a pinhole-sized cone.. (I realize this contradicts noninterference on the screen)
Thx.

pinholeprojection.GIF
 
  • #49
ndvcxk123 said:
The space next to it is another tile. Would you not accept that light from the first, at equal intensity, also covers the left and right tile
No I would not.
Please show me how that works. If you just mean that the pinhole has some finite size then that will provide blur. The light (ignoring diffraction) will travel in a straight line. The angular effect of diffrraction ~lambda/d where d is the diameeeter of the pinhole (so very tiny for the giant camera).
 
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  • #50
ndvcxk123 said:
Too me, it seems that each source object throws a cone of light larger than the pinhole
Light from parts of the object that are close to the hole will form a 'cone' with a bigger angle than parts in the background. But, if you actually do the sums, the angles are all 'small' in a working pinhole camera. If not, then use a smaller pinhole or only look at distant objects.
BUT it's only the cone of light that actually gets through the pinhole. The rest is cut off.
 
  • #51
hutchphd said:
No I would not.
Please show me how that works. If you just mean that the pinhole has some finite size then that will provide blur. The light (ignoring diffraction) will travel in a straight line. The angular effect of diffrraction ~lambda/d where d is the diameeeter of the pinhole (so very tiny for the giant camera).
 
  • #52
Yes?
 
  • #53
Note the small white dots at the tip of the arrow within the projected image of the Irvine pinhole, (diameter 6mm). Multiple, superthin lasers can project rectilinearly straight through the hole. For convenience, assume that the white paint dots of interest are precisely centered. Now, moving the laser a nanometer would still allow moving the projection point a bit, (just a bit, else one is outside of the pinhole). So now, the case of diffuse light: These little dots, like millons of other source, fill the pinhole completely, I would have thought they would start to cover each other, spreading ? Yet they are clearly defined. Why is there not more "coning"? Thx.
 
  • #54
(Its not allowing posting of the image, sorry...)
 
  • #55
ndvcxk123 said:
Why is there not more "coning"? Thx.
ndvcxk123 said:
"The straight line" you mention is part of the standard description. But (sorry), it seems to me to be inadequate, or too symbolic. Consider the roof tiles, tow. center. Take one of the tiles.
Because the "'standard description" is, in fact, completely adequate despite your misgivings. Shall I repeat it, only louder ...or less symbolically somehow?.
The sources are considered points and hundreds of meters away across the harbor so the amount of ''coning" can be easilly shown to be very very small (make a scale drawing using straight lines). This means that the angular size of the image matches that of the object.
 
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  • #56
ndvcxk123 said:
(Its not allowing posting of the image, sorry...)
Use the "Attach files" link below the Edit window to upload a JPEG or PDF file.
 
  • #57
pbuk said:
No pinhole has any "image creation effect", all the pinhole does is block light from most of the outside world from reaching the screen.
That is a very sweeping statement. If you acknowledge that a convex lens has an "image creation effect" then the same has to be said about a pinhole. A lens with an extremely small aperture is effectively a plane sheet of glass because the angles for all light paths from object element to image are more or less the same.
 
  • #58
sophiecentaur said:
That is a very sweeping statement.
Indeed that seems a bit overstated. An image is to my reckoning any continuous one to one (usually) optical mapping. A pinhole lens does not provide any focus is probably a better way to put it.
 
  • #59
hutchphd said:
A pinhole lens does not provide any focus is probably a better way to put it.
A form of aberration, along with all the others. But definitely nothing special, except that the simplest ray optics will show how a pinhole works (at a basic level). I am hoping that the OP is now able to do that simple (and universal) ray optics for a range of optical imaging arrangements.
 
  • #60
sophiecentaur said:
If you acknowledge that a convex lens has an "image creation effect"
Yes, a convex lens creates an image of an object (which is at a distance >> 2f) just beyond its focal plane.

sophiecentaur said:
then the same has to be said about a pinhole.
No it doesn't. Where would that image be?

sophiecentaur said:
A lens with an extremely small aperture is effectively a plane sheet of glass because the angles for all light paths from object element to image are more or less the same.
This is not correct. A lens with a focal length of 35 mm has a focal length of 35 mm no matter how small its aperture. Edit: With a tiny aperture it is only possible to get a tiny image, With any aperture the further you move the screen (or film) away from the lens the more out of focus the image becomes. With a plane sheet of glass (or none at all) this does not happen: because there is no focus it cannot become "less focussed", as you move the screen away from the pinhole the image gets larger and stays just as "blurry" with the amount of "blurryness" dependent only on the aperture.
 
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