What is the object distance for the right surface?
(1/24) + (1.60/s') = (1.60-1.00)/6
Simplifying I get
[(0.60/6)-(1/24)]*1.60=1/s'=7/75
s'=75/7
This puts s' to the left hand (same side as incoming light) of the lens on the left hand side, so the distance to the lens on the right hand side would just be L+s'? For that I get 39+(75/7) which gives us about 43.412cm, but that is apparently wrong.
I've written this out with my tablet to make the formatting easier to read, and also a drawing in case I am visualizing this wrong.
There's more parts later on, but I am already stuck.
Simplifying should be:
[(0.60/6)-(1/24)]/1.60=1/s'=17/192
Which gives:
s' = 192/17 or about 11.29cm
Adding to L to find S2 would give about 50.294cm, but I'm still not sure I've done that right? Corrected image attached.
If S' being positive puts it to the right of the optical surface, then the diagram should look like the below and then S2 would be L-S'?
In that case this is the best that can be done on the basis of the information provided in the statment of the problem. Note that "hemispherical" surfaces at the two ends are literally half-spheres and that the separation between ends (assumed to be the "vertices") are 39 cm apart. Draw a ray diagram of the ray from the tip of the arrow which is at left end of the axis but too small to be drawn to scale.
On edit
This figure is probably not what the author meant. See post #12.
Review the sign conventions associated with the equation ##\frac{n_1}{s} + \frac {n_2} {s'} = \frac{n_2 - n_1}{R}##.
Yes, that's right. Check that this is correct for both ##S' < L## and ##S' > L##. You'll need to know the sign conventions.
Interesting. I did not interpret the problem this way. But I see now that the problem does state "hemispherical."In that case this is the best that can be done on the basis of the information provided in the statment of the problem. Note that "hemispherical" surfaces at the two ends are literally half-spheres and that the separation between ends (assumed to be the "vertices") are 39 cm apart. Draw a ray diagram of the ray from the tip of the arrow which is at left end of the axis but too small to be drawn to scale.View attachment 374749
Personally, I don't think that this problem is instructive. Where did you find it?
@rogue_system : Make the sign correction mentioned above in post #8 and see if you get the expected answer.
Yes. I think either interpretation would yield the same answer.
The top figure has the full hemispheres. The bottom figure is a cylinder cut out of the top figure.
The height of the object is small compared to the radii of the hemispheres, and we assume paraxial rays. So, the rays traveling in the top figure will remain inside the cylindrical portion.
The smaller cylinder with curved ends matching the radius of the curvature is more or less how I pictured it (basically a camera lens without the metal barrel around it). Switching the sign got me to the correct distance for S' and thus ##S_{2}##.Yes. I think either interpretation would yield the same answer.The top figure has the full hemispheres. The bottom figure is a cylinder cut out of the top figure.
The height of the object is small compared to the radii of the hemispheres, and we assume paraxial rays. So, the rays traveling in the top figure will remain inside the cylindrical portion.
I had switched S to be negative on the left hand side because of the 'similar' explanation given by Pearson here. (The equation they use isn't rendering properly on my monitor, I am more and more understanding the importance of LaTeX, and will try use it more often.)
Since the image is still inside the optical system, even though the lens on the right hand side hasn't been accounted for, I guess it's considered a "real" instead of "virtual" image? If the optical system were shorter than S', and the image created by the left hand side fell outside of the optical system would it be considered virtual?
Edit: There is apparently something I am still not understanding, trying to figure out what S' is for the right hand side of the optical system.
$$\frac {1.60} {S_{2}} + \frac 1 {S'_{2}} = \frac {1-1.6} {-12}$$
Disregard, I've gone around in circles enough that I mixed up S' and ##{S_{2}}## in my calculations.
For this problem, a sketch shows that the rod's diameter would have to be very small to cause a problem.
Here is a diagram that I tried to draw to scale.
Each small square has a side of 1 cm. The object is given to be only 0.18 cm tall. But I drew it 1 cm tall to make it easier to see. So, the object is actually only about 1/5 the size shown.
I drew only one ray from the tip of the object, parallel to the optical axis. It passes through the focal point, F, associated with the left end of the rod. Calculation shows that F is 16 cm to the right of the left end and the image of the left end is 27.4 cm to the right of the left end. You can see that it strikes the right end of the rod at about 1.4 cm below the axis. If I had drawn the object 0.18 cm tall, then the ray would hit the right end at approximately ##\frac{1}{5} \cdot 1.4## cm ## \approx 3 ## mm below the axis. So, the rod only needs to have a diameter greater than about 6 mm. A rod 6 mm in diameter and 39 cm long would be a very thin rod.
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