Image Formation in Galilei Binoculars: Solving for the Image Position

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Homework Help Overview

The problem involves determining the image position in a Galilei binocular system, which consists of two lenses with given focal lengths and a specified distance between them. The scenario includes an object positioned at a distance from the objective lens.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the application of the lens formula for both lenses, questioning how to determine the object distance for the second lens based on the image produced by the first lens. There is also consideration of the signs of distances and the nature of the images (real vs. virtual).

Discussion Status

The discussion has progressed with participants sharing insights on the relationships between the distances and images produced by the lenses. Some guidance has been provided regarding the interpretation of distances and the implications of virtual images, though no consensus has been reached on the final image position.

Contextual Notes

Participants are working within the constraints of the problem setup, including the specific focal lengths and distances provided. There is an acknowledgment of the unconventional ray direction mentioned by one participant, which may affect the interpretation of the diagram.

Mulz
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Homework Statement


A galileibinocular consists of two lenses with ƒobjective = +30 cm and ƒokular = -10 cm. The distance between the lenses is 30 cm and the binocular is aimed at an object 90 cm away from the objective lens.

Where is the image of the object seen through the binoculars? (the binoculars are not in their normal position)

Homework Equations


1/a1 + 1/b1 = 1/ƒobjective
1/a2 + 1/b2 = 1/ƒokular
L = ƒobjective + ƒokular

The Attempt at a Solution



I started by:
[/B]
1/(90 cm) + 1/b1 = 1/(30 cm) which gave me b1 = 45 cm that is the image that the objective generates. Now I need to do the same for the okular but I don't know how to get a2.
 
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It's easiest to understand when all the distances are positive. Then the situation looks like this:

lens-3.jpg


The object is on the right, a distance ##a_1## from the the right lens. It produces an image on the left side of the right lens at a distance of ##b_1## from the lens. Then this image is a distance ##a_2## from the left lens. it produces an image on the left side of the left lens at a distance ##b_2## from the lens. The distance between the lenses is ##a_2 + b_1##.

The same general idea applies even when some of the parameters ##(a_1, b_1, f_1, a_2, b_2, f_2)## are negative. It's just that

  1. If ##b_2## is negative, that means that the first image is a virtual image, on the right side of the right lens.
  2. If ##a_2## is negative, that means that the first image serves as a virtual object of the left lens.
  3. If ##b_2## is negative, that means that the final image is a virtual image, on the right side of the left lens.
In a telescope or microscope or binoculars, you actually want ##b_2## to be negative, because you want to put your eye close to the left lens and see the image through the lens, on the right side of the lens.
 

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I agree with Steve*, but would draw it with the correct lenses and relative positions.

If b1 is 45 cm and the separation of the lenses is 30 cm, then you know the size of a2. The diagram will show what sort of object it is for the eyepiece lens.

* Edit: though IMO his ray direction is unconventional.
 
I solved it, thank you both.
 

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