01. Geometric Optics (ray transfer matrix, linear/angular magnification, chief/marginal rays)

Lecture notes: drive.google.com/drive/folder...
Many thanks to Zhe Hou for providing helpful feedback.
0:45 Pinhole camera
2:08 Convex lens
2:42 Construction of a real image
3:26 Construction of a virtual image
4:23 Virtual object in front of a lens
5:42 Virtual object behind the lens
6:35 Concave lens
7:34 Ray transfer matrix analysis
8:35 Ray transfer matrix for free-space propagation, paraxial approximation
9:41 Ray transfer matrix for a thin lens
11:25 Extracting information from a system transfer matrix
11:44 Finding the imaging condition
12:12 Finding the magnification
12:36 Finding the front focal plane and back focal plane
13:37 Example: single-lens system
14:54 Optical instruments
15:30 Motivation for angular magnification
16:52 Angular magnification for small nearby objects
17:18 Magnifying glass
18:30 Two-lens microscope
19:28 Angular magnification for large far-away objects
21:00 Two-lens telescope
21:51 Aperture stop
22:24 Entrance pupil and exit pupil
23:34 Chief rays and marginal rays
24:24 Through-focus behaviour
25:21 Telecentric system
27:21 Aberrations

Пікірлер: 11

  • @jitesh26071991
    @jitesh260719913 жыл бұрын

    Love this lecture series - concise, informative and highly conceptual. Thanks!

  • @NicolasSchmidMusic
    @NicolasSchmidMusic2 жыл бұрын

    I am so happy each time I google a precise subject and find one of your videos talking exactly about what I am looking for !

  • @lukschs1
    @lukschs13 жыл бұрын

    Fabuloso , no dejes de hacer estos videos, es un gran aporte para la cultura y los Físicos del mundo.

  • @mathieul4275
    @mathieul42755 жыл бұрын

    Excellent video for my level, thanks a lot

  • @mightbin
    @mightbin2 жыл бұрын

    a little nervous when watching this lecture, for there are so many concepts. However, i suggest we shold watch this video closely ,and better more times , it is really informative and enlightening

  • @sammyapsel1443
    @sammyapsel14438 ай бұрын

    at 25:07 , why do you suppose that the upper bundle(green) creates a shallower divergence and the marginal bundle (yellow) a bigger divergence resulting in smaller and bigger blur respectively? shouldn't the divergence of each of these bundles be the same?

  • @SanderKonijnenberg

    @SanderKonijnenberg

    8 ай бұрын

    Could you explain why the divergence of the bundles would have to be the same? It seems to me that once you define your exit pupil plane and your image plane, the divergences of the bundles through each image point follow automatically. If the distance between the two planes is finite, I'd think the bundles would necessarily have different divergences.

  • @sammyapsel1443

    @sammyapsel1443

    8 ай бұрын

    @@SanderKonijnenberg just looking it from a geometrical perspective, if i have an aperture stop and i draw a cone that goes through this stop, i can simply choose the angle of this cone exiting the aperture stop meaning that it would result in the same "divergence". Otherwise, I'd be interested to learn why you suppose that the divergence becomes smaller as you direct the cone more towards the axis.

  • @SanderKonijnenberg

    @SanderKonijnenberg

    7 ай бұрын

    @@sammyapsel1443 Given the two constraints 1) The rays in a cone must fill the exit pupil, 2) The rays in a cone must intersect at a single image point, I don't see a way to draw the rays any differently than I have. And from the traced rays, the divergences follow.

  • @sammyapsel1443
    @sammyapsel14438 ай бұрын

    at 24:12, you defined m.r. for on axis points, however i saw that in this lecture (MIT course in Optics) kzread.info/dash/bejne/kZ5_qsejm5ebg8o.html , at 26:15,the professor defines it for an off-axis point, is there a significant difference?

  • @SanderKonijnenberg

    @SanderKonijnenberg

    7 ай бұрын

    At 27:08 the professor says 'I can define them for any point I like'. I think it makes sense: according to his definition, any ray that hits the margin of the aperture stop is a marginal ray. However, many other sources (including Wikipedia en.wikipedia.org/wiki/Ray_(optics) ) require that the marginal ray goes through an on-axis object point.