Andrew B. answered 05/11/24
PhD in Applied Physics with 10+ Years of College Teaching Experience
It can be helpful to rewrite the thin lens equation to solve for p directly in some of these:
1/s + 1/p = 1/f
1/p = 1/f - 1/s
p = 1 / (1/f - 1/s). Multiply the top and bottom by sf gives:
p = sf / (sf/f - sf/s)
p = sf / (s-f)
1a) Correct!
1b) Given s = 2.5 cm and f = +1.5 cm (since it converges), from p=sf/(s-f), I'm getting p = +3.75 cm, which means it's real and inverted
1c) Since the object distance is the same as the focal length (which is positive for converging lenses), the image distance must be at infinity: 1/s + 1/p = 1/f. If s = f, p = infinity
1d) Given s = 65 mm and f = -30 mm (since it diverges), using p = sf/(s-f), I'm getting p = -20.52 mm, which means it's virtual and upright
1e) Given s = 12 cm and f = -6 cm (since it diverges), using p = sf/(s-f), I'm getting p = -4 cm, which means it's virtual and upright
Ray tracing is a real pain! Starting with the object, draw a parallel line at some random height. Once that line hits the lens, draw a second line from that point to the focal length (behind the lens for a +f, in front of the lens for a -f). Next, draw a line from your original point through the center of the lens, onto the other side. Where those 2nd and 3rd lines intersect is where the image forms!
Below are links to some examples. First for a convex, converging lens.
https://image1.slideserve.com/2123350/ray-diagrams-l.jpg
Next, for a concave, diverging lens
https://www.leydenscience.org/physics/electmag/cavelens.jpg