I have a question. In FYTD #3, the text states that when the object is very far away, the image distance is about equal to the focal length of the lens. I believe we said the same thing about convex mirrors. I'm confused, however, as to what the ray diagram would look like there. How do the rays converge at the focal point and somehow manage to spread back out to make a 10 cm-tall image, taking essentially no distance to do it? I know the rays do go through the focal point because the image is inverted.
What does this ray diagram look like?
I have not done this activity as yet,but planning to explain them using this diagram. Considering the object is far off, most of light rays raching the lense will be almost parallel even though they are inclined to the principal axis as they pass through the focus before entering the double lens.