On 02/02/07, Sauerwald Mark <mark_sauerwald@xxxxxxxxx> wrote:
That is true, but for a conventional lens there is a limit to the diameter that you can make a lens and still maintain a given focal length, with this arrangement, there is not a limit - as the disk gets larger, you have more internal reflecting surfaces (those would be equivanent to the elements in a conventional lens), and the aperture would grow as the square of the diameter - so a larger lens gets more and more light gathering capability.
Assume for the moment that the air-glass interface losses are 0% (realistic values are dealt with in my next paragraph), then in order for an Origami lens to achieve the same light gathering power as traditional multi-element lens, it would need to have approx TWICE its diameter!! [1] OK so perhaps that is not a big deal in the applications mentioned (such as surveillance aircraft, cell phones and infrared night vision applications where the lenses are already small in diameter), but it would take some getting used to if I had to replace my 62mm diameter (f=35-135mm) lens for my 35mm film camera with a lens that is 112mm in diameter ! Also, in a conventional lens, there is a fairly large amount of light loss
from passing through the air-glass surface, in this case the entire light path is within one piece of glass, so those losses should be minimal - think of how many internal reflections light has when travelling through a piece of fiber optic cable.
The light losses are not that great. In fact in a hypothetical 6 element lens using efficient antireflective coating<http://www.globalspec.com/FeaturedProducts/Detail/JMLOpticalIndustries/Antireflective_Coatings_for_Efficient_Transmission/27932/1>, only 3% of the light would be lost to internal reflections. regards Peter [1] Looking at this <http://www.jacobsschool.ucsd.edu/uploads/news_release/2007/light_path.jpg>detailed picture of the Origami lens, I estimate that the width of the circumferential annulus is 5mm when the diameter is 60mm. Preserving that ratio means that the annulus width is 1/6th the radius length. Therefore the annulus' surface area, Ao = PI *((Ro)^2 - (Ro*5/6)^2) where Ro=radius of Origami lens and Ao=Area of Origami's annulus. Let surface area of traditional multi-element lens, At = PI * (Rt)^2 For equivalent light gathering power, set At=Ao and solve for Ro as a function of Rt therefore PI * (Rt)^2 = PI *((Ro)^2 - (Ro*5/6)^2) therefore (Rt)^2 = (9/36)* (Ro)^2 therefore Rt = [sqrt(11)/9]* Ro therefore Rt ≈ 0.55* Ro hence Ro ≈ 1.8 * Rt