Smallest distance between object and image - lens.

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SUMMARY

The smallest distance between an object and its real image formed by a lens with focal distance f is 4f. This conclusion is derived from the lens formula \(\frac{1}{s} + \frac{1}{p} = \frac{1}{f}\), where s is the object distance and p is the image distance. By setting D = s + p and solving for the conditions of extremum, it is established that both s and p equal 2f, leading to D = 4f. Understanding the distinction between real and virtual images is crucial for applying this concept effectively.

PREREQUISITES
  • Understanding of the lens formula \(\frac{1}{s} + \frac{1}{p} = \frac{1}{f}\)
  • Knowledge of real and virtual images in optics
  • Familiarity with the concept of extremum in calculus
  • Basic understanding of magnification and its signs for different types of images
NEXT STEPS
  • Study the derivation of the lens formula and its applications in optics
  • Learn about the characteristics of real and virtual images in detail
  • Explore the concept of magnification and its implications in lens systems
  • Investigate the conditions for extremum in calculus and how they apply to physical problems
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Students of physics, particularly those studying optics, as well as educators and anyone seeking to clarify the principles of lens behavior and image formation.

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Homework Statement



Find the smallest distance between the object and a real image, when the focal distance of the lens is f

Homework Equations



\frac{1}{s}+ \frac{1}{p} = \frac{1}{f}, where s is the distance of the object from the lens and p is the distance of the image.

The Attempt at a Solution



I'm not even sure, what I'm trying to do here, since the definition of a real and virtual image is a bit vague to me. But I've got something...

Let D=s+p be the desired distance. From the equation above we get p = \frac{sf}{s-f} so D= \frac{s^2}{s-f}. Then \frac{ \partial D}{ \partial s}= \frac{2s^2-2sf-s^2}{(s-f)^2}=0 \Rightarrow s=0 or s=2f. We get the same for p, so the distance would be D=4f. Is this correct and does this apply for the minimum distance only or are the real image and the object always equal length from the lens?
 
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Kruum said:

The Attempt at a Solution



I'm not even sure, what I'm trying to do here, since the definition of a real and virtual image is a bit vague to me. But I've got something...

Let D=s+p be the desired distance. From the equation above we get p = \frac{sf}{s-f} so D= \frac{s^2}{s-f}. Then \frac{ \partial D}{ \partial s}= \frac{2s^2-2sf-s^2}{(s-f)^2}=0 \Rightarrow s=0 or s=2f. We get the same for p, so the distance would be D=4f. Is this correct and does this apply for the minimum distance only or are the real image and the object always equal length from the lens?

You have just arrived at this value as a condition for an extremum (or a stationary value). What do you feel should be the answer? The value is correct, by the way . Can you find values of s and p such that s+p\neq4f?

Not understanding the distinction between a real and a virtual image is not very conducive to learning Physics. Please read up or ask for help here.
 
Shooting Star said:
Not understanding the distinction between a real and a virtual image is not very conducive to learning Physics. Please read up or ask for help here.

That's the thing, I have read and listened and either misunderstood or then have had contradicting information. First I learned that the magnification for real image is m<0, the image is up-side down, and for virtual image m>0. Now I'm taught that virtual image always appears on the other side of the lens (or mirror). For converging lenses the image appears on the other side of the lens with m<0. :rolleyes:
 
hi there! I'm someone else asking the same question. so is the answer 4f? I don't understand what you mean by extremum and find the values of s and p so that it cannot equal 4f.
 

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