How Does Pinhole Diameter Affect Image Sharpness in Rayleigh Criterion?

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The discussion focuses on how the diameter of a pinhole affects image sharpness in a pinhole camera, specifically in relation to the Rayleigh criterion. It highlights that while a smaller pinhole reduces blurring from the finite size of the hole, it increases diffraction, leading to a trade-off for optimal sharpness. The relationship between the pinhole diameter and the distance to the film is explored, with an emphasis on the geometric implications of ray tracing. Practical considerations are noted, such as the need for a larger pinhole to allow sufficient light for exposure, making pinhole cameras less practical for general photography. The pinhole camera is suggested to be more effective for specific applications like observing solar eclipses.
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Homework Statement


'A scientist wants to take a picture of a distant yellow object using a pinhole camera such that the picture is of maximum sharpness. Let ##\lambda## =wavelength of yellow light, ##d## = diameter of pinhole, ##D = ## distance of pinhole to film. Find ##d##.

Homework Equations


Rayleigh:
$$ sin(\theta_{R}) = 1.22 \frac{\lambda}{D} $$

The Attempt at a Solution


[/B]
If I can express ##\theta_{R}## in terms of something else this is easy - just apply small angle approximation and rearrange [since know ##\theta << 1 rad ##].

The answers I've got tell me that:
$$ 2\theta_{R} = \frac{d}{D} $$
But I can't see any geometric way to justify this? Does anyone know where this result comes from? It's just stated as if it's patently obvious, but I've never seen it before...

Thanks!
 
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You need to consider what a pinhole camera is. Using ray tracing, the light travels in straight lines, so that a finite sized-hole will introduce some blurring. (The pinhole camera basically inverts left and right and up and down. ) The ray (a small light source ) in the object plane puts a small bright spot on the image plane after passing through the pinhole... This tells you that for the sharpest picture, if ray-tracing applies, that you want the (pin)hole as small as possible. Diffraction theory has the opposite effect=the smaller the hole, the greater the angular spread as the wave tries to get through the hole. The optimal case=minimal blurring, occurs when the blurring from diffraction is equal to the ray-trace blurring from the finite sized hole. ...Additional info. : In practice, unless you have very sensitive film or a very bright object, you widen the hole somewhat to get enough light to make an exposure of the film. Normally, cameras use lenses=the pinhole camera is an alternative that because of the low light levels, is rather impractical for photographic use. Perhaps the best application for a pinhole camera is in observing a solar eclipse=you view the image of the sun on the screen after light from the sun passes through the pinhole. If your screen is far enough away from the pinhole, you can get quite a good sized image of the sun as it is being eclipsed. The sun subtends an angle of approximately ## \theta=.01 radians ## so that if the screen is one meter from the pinhole, the image of the sun is about 1 centimeter across...
 
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The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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