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malolapjk
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- Homework Statement
- I have a two-lens system. Both principal axis coinciding. Separated by a distance 20cm. Both have focal length 15 cm. Will this act as a converging system or diverging system? If I consider a parallel beam of light is incident on it and I solve by first principles taking lens by lens I get a diverging system. A virtual image is formed between the two lens. But if I use the formula 1/f = (1/f1)+(1/f2)-(d/f1*f2), where fs are the focal lengths and d the separation between them I get a positive focal length. Which means it is a converging system forming a real image. How is that?
[b][LaTeX edited by a Mentor][/b]
- Relevant Equations
- 1/f = (1/f1)+(1/f2)-(d/f1*f2)
- Using the Lens Formula:
- The lens formula ##1f=1f1+1f2−df1f2\frac{1}{f} = \frac{1}{f_1} + \frac{1}{f_2} - \frac{d}{f_1 f_2}f1=f11+f21−f1f2d## is applicable for finding the effective focal length of the compound lens system.
- Here, ##f1=f2=15f_1 = f_2 = 15f1=f2=15 cm## (focal lengths of each lens), and ##d=20d = 20d=20 cm## (distance between the lenses).
- Calculation:
- Substitute the values into the formula: ##1f=115+115−2015×15\frac{1}{f} = \frac{1}{15} + \frac{1}{15} - \frac{20}{15 \times 15}f1=151+151−15×1520##.
- Simplify to find ##1f=215−20225\frac{1}{f} = \frac{2}{15} - \frac{20}{225}f1=152−22520##.
- ##1f=30−20225\frac{1}{f} = \frac{30 - 20}{225}f1=22530−20##.
- ##1f=10225\frac{1}{f} = \frac{10}{225}f1=22510##.
- ##f=22510f = \frac{225}{10}f=10225##.
- ##f=22.5f = 22.5f=22.5 cm##.
Lens-by-Lens Analysis
Lens 1:
- Parallel rays enter the first converging lens with ##f1=15f_1 = 15f1=15 cm##.
- These rays converge to a point 15 cm beyond the first lens.
Between Lens 1 and Lens 2:
- The distance between the two lenses is 20 cm.
- Thus, the rays would converge 5 cm before reaching the second lens.
Lens 2:
- The rays enter the second converging lens 5 cm after they would have converged if uninterrupted.
- The object for Lens 2 is virtual and located 5 cm on the object side (left side) of Lens 2.
- For Lens 2, the object distance (uuu) is −5-5−5 cm (negative because it is virtual).
Using the lens formula for Lens 2:
##1f2=1v2−1u2\frac{1}{f_2} = \frac{1}{v_2} - \frac{1}{u_2}f21=v21−u21##
where:
- ##f2=15f_2 = 15f2=15 cm##
- ##u2=−5u_2 = -5u2=−5 cm##
##115=1v2+15\frac{1}{15} = \frac{1}{v_2} + \frac{1}{5}151=v21+51##
##1v2=115−15=115−315=−215\frac{1}{v_2} = \frac{1}{15} - \frac{1}{5} = \frac{1}{15} - \frac{3}{15} = -\frac{2}{15}##
##v21=151−51=151−153=−152v2=−152=−7.5 cmv_2 = -\frac{15}{2} = -7.5 \, \text{cm}v2=−215=−7.5cm##
The negative value of v2v_2v2 indicates that the image formed by the second lens is virtual and located 7.5 cm on the object side (left side) of Lens 2. Therefore, the emergent rays are diverging after passing through Lens 2.
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