Virtual Image Location for Negative Lens System?

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Homework Help Overview

The discussion revolves around the location of a virtual image created by a negative lens system, specifically focusing on the application of the thin lens formula and the implications of sign conventions in optics.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the use of the thin lens formula and the challenges of applying it to a system involving a virtual object. Questions arise regarding the treatment of image distances and the nature of virtual objects in relation to lens systems.

Discussion Status

The conversation is ongoing, with some participants providing insights into the application of the thin lens formula and the necessary sign conventions. There is an acknowledgment of the need for further clarification on the reasoning behind these conventions.

Contextual Notes

Participants are navigating the complexities of optics, specifically regarding virtual images and the implications of using the thin lens formula in a multi-lens system. There is a mention of potential confusion regarding the definitions of object and image distances.

mrlevis
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Homework Statement


6pmeyv.jpg


S is a lighted object, height=1.
what is the final image that is created by the system?

Homework Equations





The Attempt at a Solution


i just don't understand how do i find the location of a virtual image created by a negative lens when the rays converge to a point beyond its focal point

thnks for helpers.
 
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Why can't you just use the thin lens formula?
 
you mean this?:
1/f=1/U+1/V

i used this for the lens 1, and found that V, image distance, is 12, which means it is located 6 to the negative's right, 2 after the focal point.

So how can i use the equation for the second lens? U is supposed to be an object, not converging rays.
 
mrlevis said:
you mean this?:
1/f=1/U+1/V

i used this for the lens 1, and found that V, image distance, is 12, which means it is located 6 to the negative's right, 2 after the focal point.
All good.
So how can i use the equation for the second lens? U is supposed to be an object, not converging rays.
The image from the first lens becomes the object for the second. But since it's past the second lens, it must be treated as a virtual object. Just use the usual sign convention: If an object before the lens has a positive object distance, one after the lens would have a negative object distance.
 
oh... you right.
i don't know, for some reason i didnt think it would work.

but can you explain why is that? is there a simple proof to it?
 
I suggest that you review the derivation of the thin lens formula.
 
ok, thanks for help
 

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