Aberration in Lenses: Formula & Relation Explained

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    Aberration Lenses
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Discussion Overview

The discussion revolves around the mathematical relations and formulas related to aberration in lenses, specifically focusing on the characteristics of plano concave and plano convex lenses. Participants explore both theoretical and experimental aspects of lens aberration, including the complexities involved in calculations and the implications of different lens shapes and materials.

Discussion Character

  • Exploratory
  • Technical explanation
  • Experimental/applied
  • Debate/contested

Main Points Raised

  • Some participants inquire about the existence of a formula or relation to quantify aberration in lenses, noting that plano concave lenses have negative aberration while plano convex lenses are used for correction.
  • One participant mentions that while there are no simple formulas, aberration coefficients can be calculated given the optical design, and highlights the complexity of aberration theory involving Seidel and Zernike coefficients.
  • Another participant suggests using optical design simulation software, such as Zemax or WinLens Basic, to analyze aberrations, noting the challenges associated with these tools.
  • Some participants discuss the experimental observation that rays parallel to the principal axis do not focus at a single point, indicating the presence of aberration, and express a desire to quantify this effect.
  • A participant proposes a thought experiment involving the calculation of focal points as a function of convergence angle, emphasizing the resulting caustic beam profile and the impact of different angles on focusing.
  • There is a suggestion to use an iris diaphragm to vary the numerical aperture and measure the movement of the focal point as a method to quantify aberration.
  • One participant requests a diagram to clarify the discussion about angles and rays, indicating a need for visual aids to better understand the concepts being discussed.

Areas of Agreement / Disagreement

Participants express varying levels of understanding and approaches to the topic, with no consensus on a single formula or method for quantifying aberration. Multiple competing views on the best methods for analysis and the implications of lens design remain evident throughout the discussion.

Contextual Notes

The discussion highlights the complexity of aberration calculations and the dependence on specific lens designs and experimental setups. There are references to various coefficients and methods, but no definitive resolution on the best approach to quantify aberration is reached.

VVS2000
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Is there any formula or a mathematical relation to find aberration in lenses? I read recently that plano concave lens has a negative aberration and plano convex lens is used to correct it. I am not sure what those statements mean. Is there some type of relation that explains these statements or is it like an experimental fact?
 
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Wiki does it for the thin-lens approximation.
 
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VVS2000 said:
Is there any formula or a mathematical relation to find aberration in lenses? I read recently that plano concave lens has a negative aberration and plano convex lens is used to correct it. I am not sure what those statements mean. Is there some type of relation that explains these statements or is it like an experimental fact?
The short answer is "no, but you can calculate the various aberration coefficients given the optical design". There are 'stop-shift formulas', but I don't think that's what you mean. It's important to note that there are aberrations caused by the shape(s) of the lens element(s) and different aberrations (chromatic) caused by the material(s) the element(s) are made of. Then, of course, there are aberrations caused by misalignment :).

The calculation gets extremely complicated very quickly, and there aren't any simple references, either. In general, aberration theory is rooted in either Seidel coefficients or Zernike coefficients, and converting between the two is non-trivial.

Kingslake's book is a standard:
https://www.amazon.com/dp/012374301X/?tag=pfamazon01-20

And Buchdahl's book is the most comprehensive:
https://www.abebooks.com/Optical-Ab...MI9fPZ7N6q9QIVzGtvBB2NGAfrEAQYASABEgJWvvD_BwE
 
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If you have an optical design in hand, the best route to go is to simulate your optical design in an appropriate software product. There are many, but the most popular in research is Zemax. The problem is it's expensive as heck and their anti-pirating security measures make it a real pain in the butt for legitimate paying users (hardware keys, remote access versions, etc.).

There are software packages that offer limited free trial versions. I'm partial to WinLens Basic from QIoptiq, but I'm sure you could find others out there. You can find WinLens Basic tutorial videos on youtube.

If you're curious, these software products use ray-tracing methods to calculate aberrations. There are also analytical formulas, which I'm sure you could find in either of the books @Andy Resnick listed.

VVS2000 said:
I read recently that plano concave lens has a negative aberration and plano convex lens is used to correct it.
This is highly dependent on what you're trying to accomplish. There's no one-size-fits-all solution.

Now, if you're trying to build understanding about spherical aberration (which is what it sounds like you're talking about in the first post), then I recommend you try this exercise:

Consider a converging beam of light initially with a convergence angle of ##\theta## that passes through a slab of glass at normal incidence. Calculate the focal point as a function of ##\theta##. Notice that the answer depends on ##\theta##. That means the center of the beam has a different focal point than the outer rim of the beam. This results in a caustic beam profile (as opposed to a Gaussian beam).

If you solve the above problem but approximate the ##\sin \theta## in Snell's law by ##\theta##, you get the answer in the absence of all aberrations. If you solve it by approximating Snell's law by ##\theta + \frac{1}{3!} \theta^3 ##, you get the answer including 3rd order spherical aberration, and so on. I hope that gives you a little insight into what's going on.
 
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Andy Resnick said:
The calculation gets extremely complicated very quickly, and there aren't any simple references, either. In general, aberration theory is rooted in either Seidel coefficients or Zernike coefficients, and converting between the two is non-trivial.
Well not soo deep at the theoretical level but The thing I want to understand is on more of an experimental level. Coz I was doing experiments with lenses which have 10cm diameter and 15 cm focal length, and all rays parallel to principal axis don't focus on the focal point. So aberration does exist but I cannot or don't know how to quantitatively put it across
 
Twigg said:
Consider a converging beam of light initially with a convergence angle of θ that passes through a slab of glass at normal incidence. Calculate the focal point as a function of θ. Notice that the answer depends on θ. That means the center of the beam has a different focal point than the outer rim of the beam. This results in a caustic beam profile (as opposed to a Gaussian beam
I am so sorry but do you have like a diagram that shows what you're trying to say, I might not able to get which angle and rays that you might be referring to
 
VVS2000 said:
Coz I was doing experiments with lenses which have 10cm diameter and 15 cm focal length, and all rays parallel to principal axis don't focus on the focal point.
The diameter of the lens is more or less irrelevant (assuming you have a separate stop that isn't the lens itself). It's the radial distance of the marginal rays (or equivalently the numerical aperture (NA)) that matters.

If you want to quantify the amount of aberration in your system, try using an iris diaphragm to vary the NA of your system. Measure how much the focal point moves when you close the iris vs when you fully open the iris. The more the focal point moves, the worse your aberration is.

VVS2000 said:
I am so sorry but do you have like a diagram that shows what you're trying to say, I might not able to get which angle and rays that you might be referring to
Yeah, sorry I was being lazy. Here you go:

1641969090110.png

Two rays incident at angle ##\theta## on a rectangular slab of glass. When they hit the glass, they're separated by a distance of ##2h##. Slab has a thickness ##t##. Find the position of the focal point from ##\theta##, ##h##, ##t##, and ##n## (index of the slab). Expand your answer as a series for small ##\theta##. The lowest term should be cubic and it refers to 3rd order spherical aberration.

Notice that your optical design contains a range of values of ##\theta## from 0 up to your aperture stop. That means your focal point will be smeared out over a range, giving you a caustic.
 
Twigg said:
The diameter of the lens is more or less irrelevant (assuming you have a separate stop that isn't the lens itself). It's the radial distance of the marginal rays (or equivalently the numerical aperture (NA)) that matters.

If you want to quantify the amount of aberration in your system, try using an iris diaphragm to vary the NA of your system. Measure how much the focal point moves when you close the iris vs when you fully open the iris. The more the focal point moves, the worse your aberration is.Yeah, sorry I was being lazy. Here you go:

View attachment 295381
Two rays incident at angle ##\theta## on a rectangular slab of glass. When they hit the glass, they're separated by a distance of ##2h##. Slab has a thickness ##t##. Find the position of the focal point from ##\theta##, ##h##, ##t##, and ##n## (index of the slab). Expand your answer as a series for small ##\theta##. The lowest term should be cubic and it refers to 3rd order spherical aberration.

Notice that your optical design contains a range of values of ##\theta## from 0 up to your aperture stop. That means your focal point will be smeared out over a range, giving you a caustic.
Ok, will do it
Thanks for the image!
 

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