The Lens Formula is a fundamental equation in optics that establishes a relationship between the object distance, image distance, and focal length of a lens. Whether dealing with a convex or concave lens, this formula provides a precise mathematical way to calculate the position of the image formed by a lens. Understanding the derivation of lens formula in physics helps in gaining deeper insights into how lenses manipulate light to form images. In this article, we will explore the derivation of the lens formula, highlighting the underlying principles of ray optics and the geometry involved in image formation by thin lenses.
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The lens is a piece of transparent material with two refracting surfaces such that at least one surface is curved and the refractive index of its material is different from that of the surroundings.
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.
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 center of the lens
u is the distance of the object from the optical center of the lens
f is the focal length of the lens
The relationship between a lens' focal length, the refractive index of its material, and the radii of curvature of its two surfaces is known as the lens maker's formula. Lens manufacturers use it to build lenses with a specific power from glass with a specific refractive index. The focal length, f, is described by the lens maker formula:
$\frac{1}{f}=(n-1)\left(\frac{1}{R_1}-\frac{1}{R_2}\right)$
where
R1 and R2 are the radii of curvature
n is the index of refraction
Focal length
The focal length of an optical system is the inverse of the system's optical power; it measures how strongly the system converges or diverges light. A system with a positive focal length converges light, while one with a negative focal length diverges light.
Power
It is the reciprocal of the focal length and is measured in dioptre(D). Power is positive for converging lenses and negative for diverging lenses.
A thin lens is defined as one whose thickness is insignificant in comparison to its curvature radii. The thickness (t) is significantly lower than the two curvature radii R1 and R2.
The focal length, image distance, and object distance are all connected in the lens formula for concave and convex lenses. The given formula can be used to establish this link.
$$\frac{1}{u}+\frac{1}{v}=\frac{1}{f}$$
where,
f is the focal length of the lens
v is the distance of the generated image from the lens' optical center
u is the distance between an item and the optical center of the lens.
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There are two types of thin lenses- convex lens and concave lens. Read the below table to learn more about these.
Converging (convex) Lens | Diverging (concave) Lens |
• The focal length is positive (+ve) | • The focal length is negative (-ve) |
• A convex lens is thicker at the center and thinner at the edges | • A concave lens is thicker at the edges and thinner at the center |
• Use for correction of long-sightedness | • Use for correction of short-sightedness |
• On passing the light through the lens, it bends the light rays towards each other | • On passing the light through the lens, it bends the light rays away from each other |
• The image formed can be real, virtual, enlarged, or diminished | • The image formed is always virtual and diminished |
• The principal focus is real | The principal focus is virtual |
• It is also called a positive lens | • It is also called a negative lens |
• Human eye, camera | • Lights, flashlights |
The lens maker formula is derived using the assumptions listed below.
The whole derivation of the lens maker formula is provided further below. We can say that, using the formula for refraction at a single spherical surface,
For the first surface,
Object Distance = -u
Image Distance = v = x
Radius of Curvature= R1
Thus the formula becomes,
$\frac{n_2}{v}-\frac{n_1}{u}=\frac{n_2-n_1}{R_1} \ldots$
By substituting we get
$\frac{n_b}{x}-\frac{n_a}{u}=\frac{n_b-n_a}{R_1} \ldots$ --------------(1)
For the second surface,
$\frac{n_2}{v}-\frac{n_1}{x}=\frac{n_2-n_1}{-R_2}$ --------------- ( 2)
Now adding equation (1) and (2),
$\begin{aligned} & \frac{n_a}{v}-\frac{n_b}{u}=\left(n_b-n_a\right)\left[\frac{1}{R_1}-\frac{1}{R_2}\right] \\ \\& \Rightarrow \frac{1}{v}-\frac{1}{u}=\left(\frac{n_b}{n_a}-1\right)\left[\frac{1}{R_1}-\frac{1}{R_2}\right]\end{aligned}$
We know that,
$\frac{1}{v}-\frac{1}{u} =\frac{1}{f} $
Hence the equation becomes,
$\frac{1}{f}=\left(\frac{n_2}{n_1}-1\right)\left[\frac{1}{R_1}-\frac{1}{R_2}\right]$
Therefore, we can say that,
$\frac{1}{f}=(\mu-1)\left(\frac{1}{R_1}-\frac{1}{R_2}\right)$
Where μ is the material's refractive index.
This is the derivation of the lens maker formula. Examine the constraints of the lens maker's formula to have a better understanding of the lens maker's formula derivation.
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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 A1B1 is generated between O and F1 on the same side as the item, and it is virtual and erect.
$\triangle O A B$ and $\triangle O A^1 B^1$ are similar
$\left[\begin{array}{l}\because \angle B A O=\angle B^1 A^1 O=90^{\circ}, \text { vertex is common for both the triangles } \\ \text { so } \angle A O B=\angle A^1 O B^1, \therefore \angle A B O=\angle A^1 B^1 O\end{array}\right]$
$\frac{A^1 B^1}{A B}=\frac{O A^1}{O A}---(1)$
$\triangle O C F_1$ and $\triangle F_1 A^1 B^1$ are similar
$\frac{A^1 B^1}{O C}=\frac{A^1 F_1}{O F_1}$
But from the ray diagram, we see that OC = AB
$\begin{aligned} & \frac{A^1 B^1}{A B}=\frac{A^1 F_1}{O F_1}=\frac{O F_1-O A^1}{O F_1} \\ & \frac{A^1 B^1}{A B}=\frac{O F_1-O A^1}{O F_1}---(2)\end{aligned}$
From equation (1) and equation (2), we get
$\begin{aligned} & \frac{O A^1}{O A}=\frac{O F_1-O A^1}{O F_1} \\ & \frac{-v}{-u}=\frac{-f--v}{-f} \\ & \frac{v}{u}=\frac{-f+v}{-f} \\ & -v f=-u f+u v\end{aligned}$
Dividing throughout by uvf
$-\frac{1}{u}=-\frac{1}{v}+\frac{1}{f}$
$\frac{1}{f}=\frac{1}{v}-\frac{1}{u}$
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It's not enough to know the thin lens formula for convex lenses. The characteristics of a ray of light going through converging and diverging lenses must be understood.
A concave or divergent lens has a negative focal length. When the picture is generated on the side where the object is positioned, the image distance is also negative. The image is virtual in this case. A converging or convex lens, on the other hand, has a positive focal length.
The lens formula is used to determine the position and size of the image formed by the lens. The lens formula applies to both diverging and converging lenses. The lens makers' formula helps in determining the focal length of a lens based on its curvature and the refractive index of the material from which it is made. This formula is crucial for creating lenses with precise focusing properties.
1f=1v−1u
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.
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.
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