How Can Bessel's Method Determine the Focal Length of a Lens?

In summary, Bessel's method for finding the focal length of a lens involves an object and a screen that are separated by a distance greater than 4f. It is possible to place the lens at either of two locations, between the object and the screen, so that there is an image of the object on the screen. If the distance between those two lens locations is D, then the focal length is given by f=(1/4)(L2-D2)/L.
  • #1
w3390
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0

Homework Statement


In Bessel's method for finding the focal length f of a lens, an object and a screen are separated by distance L, where L is greater than 4f. It is then possible to place the lens at either of two locations, both between the object and the screen, so that there is an image of the object on the screen, in one case magnified and in the other case reduced. Show that if the distance between those two lens locations is D, then the focal length is given by f=(1/4)(L2-D2)/L.

Homework Equations


Thin lens equation: [tex]\frac{1}{s}[/tex]+[tex]\frac{1}{s'}[/tex]=[tex]\frac{1}{f}[/tex]
Focal length: [tex]\frac{1}{f}[/tex]=(([tex]\frac{n}{nair}[/tex])-1)([tex]\frac{1}{r1}[/tex]-[tex]\frac{1}{r2}[/tex])

The Attempt at a Solution


I know that you guys are not able to help me out until I show you my attempt, but I do not even know where to start. I guess if you guys could tell me whether or not these equations are relevant, then I could work from there and get back to you with an actual attempt.
 
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  • #2
The thin lens equation is relevant, the focal length equation isn't.

But there is another relevant equation. What can you say about s, s', and L?
Code:
o<-------- s -------->()<---- s' ---->|

 <---------------- L ---------------->
p.s. to get subscripts in Latex, type eg. n_{air} rather than [noparse]nair[/noparse]
 
  • #3
At one position of the lens s is the object distance and s' is the image distance. Let s<s'.When you shift the lens towards the screen, again you get a sharp image. In this position s and s' interchange. If D is the distance moved by the lens, then s + s' = L and s' - s = D. From these equations find s and s' and then f.
 
  • #4
Okay. Using the thin lens equation and the relationships between s, s', D, and L, I was able to solve for s and s' and plug them into the lens equation. However, doing this alone gets me only close to the right answer. I end up with f= (1/4)(L^2-D^2). I am missing the L term dividing into the (L^2-D^2). I think it has something to do with the relationship of L>4f. But in terms of f, this is L/4 which still isn't the right answer. Where am I going wrong?
 
  • #5
S = (L+D)/2 and s' = (L-D)/2 from these values find f.
 
  • #6
I know that those are the values for s and s' and I used them in the lens equation. What I was saying was that when I plugged them in and solved for f, I did not have the extra L term. I ended up with (1/4)(L^2-D^2) instead of (1/4)(L^2-D^2)/L. I have a feeling the L does not come from either the s or s' equation. I was wondering if it may have come from L>4f.
 
  • #7
w3390 said:
f= (1/4)(L^2-D^2).
I am missing the L term dividing into the (L^2-D^2).

Note that your equation is inconsistent in the units, in that it equates a length f with a length2 on the right-hand-side. That's a dead give-away that a mistake has been made.

Presumably you started with equations that were consistent in the units. Find out where in your derivation the units inconsistency first appears, and that is where the error is.
 
  • #8
The unit error occurs when I combine the denominators in the lens equation. Using the equation (1/s)+(1/s')=(1/f), where s=(1/2)(L-D) and s'=(1/2)(L+D). This gives me a good equation that relates L, D, and f. If I then want to find a common denominator, I multiply the two denominators together to get (1/4)(L^2-D^2). This is where I have length squared equaling a length. For the sake of units, I know I could just divide by L to make the units work out, but I am at a loss as to how the L enters the equation. My initial thought was that it had something to do with the initial condition given: f<(L/4).
 
  • #9
w3390 said:
If I then want to find a common denominator, I multiply the two denominators together to get (1/4)(L^2-D^2).

It probably would be helpful to review how to combine fraction expressions and getting a common denominator.

You realized that we desire a common denominator when combining the expressions

[tex]\frac{1}{\frac{L-D}{2}}+\frac{1}{\frac{L+D}{2}}
[/tex]

Multiply the first fraction by (L+D)/(L+D) to make it

[tex]\frac{L+D}{\ \frac{(L-D)(L+D)}{2} \ }[/tex]

or equivalently

[tex]\frac{2(L+D)}{L^2-D^2}[/tex]

If you do similarly for the 2nd fraction, you'll then be able to combine the two fractions.

(And notice that the units are "1/length" at each step so far.)
 
  • #10
Wow. Thanks a lot. I got it now. I'm really embarrassed to have made such a simple mistake in finding the common denominator. Thanks everyone for helping out. I greatly appreciate it.
 

1. What is Bessel's method in optics?

Bessel's method is a mathematical technique used in optics to describe the propagation of light waves through a medium. It involves the use of Bessel functions, which are special mathematical functions that can represent complex physical phenomena such as diffraction and interference.

2. How is Bessel's method used in optics?

Bessel's method is commonly used to analyze the behavior of light waves as they pass through optical elements such as lenses, mirrors, and diffraction gratings. It can also be used to calculate the intensity and spatial distribution of light after it passes through these elements.

3. What are some applications of Bessel's method in optics?

Bessel's method has many practical applications in optics, including the design of optical systems such as telescopes and microscopes, the study of optical phenomena such as diffraction and interference, and the development of new imaging techniques.

4. What are the advantages of using Bessel's method in optics?

One of the main advantages of Bessel's method is its ability to accurately describe the propagation of light waves through complex optical systems. It also allows for the analysis of both coherent and incoherent light, making it a versatile tool for studying a wide range of optical phenomena.

5. Are there any limitations to using Bessel's method in optics?

While Bessel's method is a powerful tool in optics, it does have some limitations. For example, it is only applicable to systems that are radially symmetric, meaning that the properties of the system do not change with direction. Additionally, it may not accurately describe the behavior of light waves in highly nonlinear or strongly scattering media.

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