Lenses are pieces of curved glass or some transparent material, and they bend light to create images. Lenses are commonly found in cameras, eyeglasses, microscopes and telescopes. The formation of an image by lenses is understood with the help of the lens formula, a mathematical expression that relates the object distance (u), image distance (v), and focal length (f) of a lens. In this article, we shall derive the lens formula step by step using simple ray diagrams and basic geometry, all for the benefit of a simple-to-understand concept for students and for application to numerical problems.
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The lens is a transparent object that may be made of glass or plastic, and it bends (or refracts) light rays to create images. These are lenses with curved surfaces that primarily use the principle of refraction. Lenses are found in eyeglasses, cameras, microscopes, and magnifying glasses.
Lenses are based on two basic types:
The lens is divided into two types depending on how the light rays behave when they travel through the lens. These are further divided into the following types.
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The lens equation or lens formula is an equation that links the focal length, image distance, and object distance.
$\frac{1}{v}-\frac{1}{u}=\frac{1}{f}$
where,
v is the distance of the image from the optical centre of the lens, u is the distance of the object from the optical centre of the lens and f is the focal length of the lens.
Let AB represent an object at a distance greater than the focal length f of the convex lens that is located at right angles to the primary axis. The image A' B' is generated between O and $F_1$ on the same side as the item, and it is virtual and erect.
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$\triangle O A B$ and $\triangle$ O A' B' are similar
$\because \angle B A O=\angle B^1 A^1 O=90^{\circ}$, vertex is common for both the triangles so $\angle A O B=\angle A^1 O B^1,$
$ \therefore \angle A B O=\angle A^1 B^1 O$
$\frac{A' B'}{A B}=\frac{O A'}{O A}---(1)$
$\triangle O C F_1$ and $\triangle F_1 A' B' $ are similar
$\frac{A' B'}{O C}=\frac{A' F_1}{O F_1}$
But from the ray diagram, we see that OC = AB
$\begin{aligned} & \frac{A' B'}{A B}=\frac{A' F_1}{O F_1}=\frac{O F_1-O A'}{O F_1} \\ & \frac{A' B'}{A B}=\frac{O F_1-O A'}{O F_1}---(2)\end{aligned}$
From equation (1) and equation (2), we get
$\begin{aligned} & \frac{O A'}{O A}=\frac{O F_1-O A'}{O F_1} \\ & \frac{-v}{-u}=\frac{-f--v}{-f} \\ & \frac{v}{u}=\frac{-f+v}{-f} \\ & -v f=-u f+u v\end{aligned}$
Dividing throughout by uvf
$-\frac{1}{u}=-\frac{1}{v}+\frac{1}{f}$
$\frac{1}{f}=\frac{1}{v}-\frac{1}{u}$
The lens formula helps us understand how and where an image is formed by a lens. Its main applications are:
1. To find the image position: By using the object distance ( $u$ ) and focal length ( $f$ ), we can calculate the image distance ( $v$ ).
2. To know the nature of the image: After finding $v$, we can check whether the image is real or virtual, inverted or erect, magnified or diminished.
3. To determine the focal length: If $u$ and $v$ are known from an experiment, the focal length $f$ can be easily calculate
4. To design optical instruments: Devices like cameras, microscopes, telescopes, and spectacles use the lens formula for proper image formation.
5. To correct vision problems: The formula helps in choosing the correct lens power for myopia and hypermetropia.
Frequently Asked Questions (FAQs)
Concave lenses can be found in a variety of real-world applications.
Telescopes and binoculars
Nearsightedness can be corrected with eyeglasses.
Cameras.
Flashlights.
A concave lens is used to correct myopia.
The lens maker formula was discovered by Rene Descartes.
The human eye has a convex (biconvex) lens.
1/f=1/v−1/u
Only when the object and image are on the same side of the lens is the picture generated by a concave lens virtual.
The combined lens works as a convex lens if the focal length of the second lens is greater than the focal length of the first lens.
The lens formula is the relationship between the object's distance u, the image's distance v, and the lens's focal length f. With the right sign conventions, this law can be applied to both concave and convex lenses.