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Optical power

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In optics, optical power (also referred to as dioptric power, refractive power, focal power, focusing power, or convergence power) is the degree to which a lens, mirror, or other optical system converges or diverges light.^[1] It is equal to the reciprocal of the focal length of the device; high optical power corresponds to short focal length. The SI unit for optical power is the inverse metre (m⁻¹), which is also called a dioptre (symbol: dpt or D) when used as a unit of optical power.

Explanation

[edit]

The optical power $P$ of a device is related to its focal length $f$ by $P = 1/ f$ .^[2]

Converging lenses have positive optical power, while diverging lenses have negative power. When a lens is immersed in a refractive medium, its optical power and focal length change.

For two or more thin lenses close together, the optical power of the combined lenses is approximately equal to the sum of the optical powers of each lens: $P = P 1 + P 2$ . Similarly, the optical power of a single lens is roughly equal to the sum of the powers of each surface. These approximations are commonly used in optometry.

An eye that has too much or too little refractive power to focus light onto the retina has a refractive error. A myopic eye has too much power so light is focused in front of the retina. This is noted as a minus power. Conversely, a hyperopic eye has too little power so when the eye is relaxed, light is focused behind the retina. An eye with a refractive power in one meridian that is different from the refractive power of the other meridians has astigmatism. This is also known as a cylindrical power. Anisometropia is the condition in which one eye has a different refractive power than the other eye.

References

[edit]

^ Basu, Dipak (2018-10-08). Dictionary of Pure and Applied Physics. CRC Press. ISBN 978-1-4200-5022-6.
^ Greivenkamp, John E. (2004). Field Guide to Geometrical Optics. SPIE Field Guides. Vol. FG01. SPIE. p. 7. ISBN 0-8194-5294-7.

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Optical power, also known as dioptric power or refractive power, is a measure of the ability of a lens, curved mirror, or other optical element to converge or diverge light rays, quantified as the reciprocal of its focal length.^[1] The optical power

P

of an optical system is given by the formula

P = \frac{1}{f}

, where

f

is the focal length in meters.^[2] This distinguishes it from radiant power, which refers to the energy flux of light in watts and is a separate concept in photonics.^[3] The standard unit of optical power is the diopter (symbol D), defined such that 1 D = 1 m⁻¹, allowing for straightforward calculation of lens strength in vision correction and optical design.^[4] For converging lenses (convex), which focus parallel rays to a real focal point, the focal length

f

is positive, resulting in positive optical power; conversely, diverging lenses (concave) have negative focal length and thus negative power, spreading rays as if from a virtual focal point.^[5] This sign convention is essential in the thin-lens equation,

\frac{1}{f} = \frac{1}{d_o} + \frac{1}{d_i}

, where

d_o

is the object distance and

d_i

the image distance, both measured with consistent sign rules.^[1] In practical applications, optical power plays a central role in human vision and corrective optics, where the eye's components—such as the cornea with approximately 43.5 D and the lens with about 15.6 D—combine to yield a total power of roughly 59 D for normal focus at infinity.^[2] For multiple lenses in contact, the total optical power is the algebraic sum of individual powers, simplifying the design of compound optical systems like eyeglasses or microscopes.^[4] High optical power corresponds to short focal lengths and strong refraction, critical for applications ranging from corrective eyewear to precision imaging in scientific instruments.^[3]

Fundamentals

Definition

Optical power is a measure of an optical element's ability to converge or diverge a beam of light, quantifying the degree to which it bends light rays passing through or reflecting off its surface.^[3] It is defined as the reciprocal of the focal length

f

of the element, expressed in the formula

P = \frac{1}{f}

, where

f

is in meters and

P

is in diopters (D).^[4] Positive power corresponds to converging elements, such as convex lenses, while negative power indicates diverging elements, like concave lenses.^[3] In ray optics, optical power describes how parallel rays of light are redirected by the element: for positive power, they converge to a single focal point after refraction or reflection, establishing the element's focusing strength.^[4] This bending arises from the variation in refractive index or curvature at the element's surface, which alters the direction of light propagation according to Snell's law, with higher power indicating greater deviation of the rays from their original path.^[6] The term "diopter" for optical power originated in the 19th century, proposed by French ophthalmologist Ferdinand Monoyer in 1872 to standardize the description of lens strength in optometry and optics.^[7] This naming drew from earlier uses of "dioptrice" by Johannes Kepler in 1611, but Monoyer's definition formalized it as the unit of reciprocal focal length.^[8]

Units and Conventions

The primary unit for optical power is the diopter (symbol: D), equivalent to m⁻¹, defined as the reciprocal of the focal length in meters for a lens or optical element.^[9]^[10] This unit quantifies the ability of an optical element to converge or diverge light rays, where a power of +1 D corresponds to a focal length of 1 meter.^[11] Historically, focal lengths were often expressed in inches or centimeters, particularly in early optometry and lens manufacturing, leading to non-standardized power calculations.^[12] Standardization to the metric system, with diopters based on meters, was formalized in the late 19th century following the proposal of the dioptre by French ophthalmologist Ferdinand Monoyer in 1872, promoting consistency in optical measurements worldwide.^[13] The sign convention for optical power follows the Cartesian system in ray optics, where power is positive for converging elements that produce a real focal point (e.g., convex lenses or concave mirrors) and negative for diverging elements that produce a virtual focal point (e.g., concave lenses or convex mirrors).^[14]^[15] This convention ensures consistent application across optical calculations, with the basic relation

P = 1/f

(where

f

is the focal length) yielding the appropriate sign based on the element's behavior.^[16] Conversion factors facilitate transitions from other units: optical power in diopters is calculated as

P = 100 / f

where

f

is in centimeters, or approximately

P = 40 / f

where

f

is in inches, aligning all measurements to the meter-based standard.^[12]^[11]

Power of Optical Elements

Thin Lenses

The thin lens approximation in optics assumes that the lens thickness is negligible compared to its focal length, and that light rays are paraxial, meaning they make small angles with the optical axis.^[17] Under these conditions, the optical power of a thin lens arises from refraction at its two spherical surfaces, where power is defined as the reciprocal of the focal length,

P = 1/f

.^[18] The power of a single spherical refracting surface separating two media with refractive indices

n_1

(incident side) and

n_2

(transmitted side) is given by

P = (n_2 - n_1)/R

, where

R

is the radius of curvature of the surface.^[17] This formula follows from the paraxial ray approximation of Snell's law applied to the surface, with the sign convention that

R

is positive if the center of curvature lies to the right of the surface (assuming light travels left to right). Convex surfaces toward the incident light yield positive power for converging effects when

n_2 > n_1

.^[19] For a thin lens in air (surrounding medium refractive index

n = 1

), the total power is the sum of the powers of its two surfaces, leading to the lensmaker's formula:

P = (n_l - 1) \left( \frac{1}{R_1} - \frac{1}{R_2} \right)

, where

n_l

is the refractive index of the lens material, and

R_1

R_2

are the radii of curvature of the first and second surfaces, respectively.^[18] The sign convention assigns positive radii for centers of curvature to the right of each surface. This formula indicates that the lens power increases with higher

n_l

or greater surface curvatures (smaller

|R|

), and the sign of

P

determines whether the lens is converging (positive) or diverging (negative).^[17] The influence of surface curvatures is evident in common lens designs. For a plano-convex lens with the curved surface facing the incident light (

R_1 = R > 0

R_2 = \infty

), the power simplifies to

P = (n_l - 1)/R

, providing convergence through a single curved interface.^[18] In contrast, a symmetric biconvex lens (

R_1 = R > 0

R_2 = -R < 0

) has power

P = 2(n_l - 1)/R

, doubling the effect for the same radius magnitude due to contributions from both surfaces, which enhances focusing efficiency but may introduce aberrations if not balanced.^[20]

Spherical Mirrors

Spherical mirrors are reflective optical elements shaped as segments of a sphere, used to converge or diverge light rays based on their curvature. The optical power

P

of a spherical mirror, defined as the reciprocal of its focal length

f

(in meters), quantifies its ability to bend light, with units in diopters (D). For a spherical mirror, the focal length is half the radius of curvature

R

, given by

f = \frac{R}{2}

, leading to the power formula

P = \frac{1}{f} = \frac{2}{R}

. The sign convention assigns positive values to

R

(and thus

P

) for concave mirrors, which converge light, and negative values for convex mirrors, which diverge light. Unlike refractive elements such as lenses, spherical mirrors achieve focusing solely through reflection at the surface, without involvement of a material's refractive index, avoiding issues like chromatic dispersion. In these systems, the primary focal point—where parallel incident rays converge after reflection—and the secondary focal point—from which rays diverge to become parallel after reflection—coincide at the same position along the optical axis, as the light remains in the same medium before and after reflection. These relations hold under the paraxial approximation, which assumes rays are near the optical axis and the mirror's aperture is small relative to

R

, allowing all rays to focus at a single point. For larger incident angles or wider apertures, this approximation fails, resulting in spherical aberration where marginal rays focus closer to the mirror than paraxial rays, degrading image quality and effectively reducing the mirror's defined power.

Power in Optical Systems

Combined Power

In optical systems comprising multiple thin lenses, the total power is additive when the lenses are in contact, with no separation between them. For two thin lenses with individual powers

P_1

and

P_2

, the combined power

P_\text{total}

is given by

P_\text{total} = P_1 + P_2

.^[21] When two thin lenses are separated by a distance

d

in air, the combined power is reduced compared to the contact case, particularly for positive lenses. The formula for the total power is

P_\text{total} = P_1 + P_2 - d \, P_1 P_2,

where the negative term

-d \, P_1 P_2

accounts for the separation's effect on ray convergence, leading to a longer effective focal length and lower overall power when both

P_1 > 0

and

P_2 > 0

.^[21] For multi-element systems, the back focal length (BFL) is the distance from the rear surface of the last element to the system's rear focal point, while the front focal length (FFL) is the distance from the front surface of the first element to the front focal point. These lengths describe the system's focal positions relative to its physical boundaries and differ from the effective focal length, which is referenced to the principal planes.^[21]^[22]

Effective Focal Length and Power

The effective focal length (EFL) of an optical system is defined as the distance from the rear principal plane to the rear focal point, where parallel incoming rays converge after passing through the system.^[23] This measure allows complex systems to be treated equivalently to a single thin lens for paraxial ray analysis. The effective optical power

P_{\text{eff}}

is then given by the reciprocal of the EFL,

P_{\text{eff}} = \frac{1}{\text{EFL}}

, typically expressed in diopters when the EFL is in meters.^[24] Principal planes are hypothetical planes perpendicular to the optical axis where the refraction of rays in a system can be considered to occur, simplifying the analysis of ray bending.^[25] In multi-element systems, these planes are located by extrapolating incident and emergent rays to their intersection points, with the front principal plane relevant for object-side rays and the rear for image-side rays.^[26] The EFL is measured relative to these planes, enabling consistent characterization of systems beyond simple thin lenses, such as those with separated elements or varying thicknesses. For a thick lens, which accounts for the physical separation between its refracting surfaces, the effective power extends the thin-lens approximation by incorporating the lens thickness

t

and refractive index

n

. The formula, known as Gullstrand's equation, is

P = P_1 + P_2 - \frac{t}{n} P_1 P_2

, where

P_1

and

P_2

are the surface powers of the first and second surfaces, respectively.^[27] This correction term

-\frac{t}{n} P_1 P_2

reduces the total power compared to the thin-lens sum due to the propagation distance within the lens material, becoming negligible as

t

approaches zero. For example, a biconvex thick lens with surface powers of +10 D and +10 D, thickness 5 mm, and

n = 1.5

yields an effective power of approximately +19.7 D, illustrating the impact of thickness on system performance. In more complex multi-element systems, the system matrix method, or ABCD ray transfer matrix analysis, provides a systematic way to compute the effective power. Each optical element or propagation distance is represented by a 2×2 matrix

\begin{pmatrix} A & B \\ C & D \end{pmatrix}

, which transforms input ray height and angle to output values under paraxial approximation.^[28] The overall matrix for the system yields the EFL as

\text{EFL} = -\frac{1}{C}

, with the effective power

P_{\text{eff}} = -C

, assuming the determinant

AD - BC = 1

for systems in air.^[29] This approach facilitates design of telescope objectives or microscope objectives by chaining matrices for lenses, spaces, and mirrors. While thin lenses in contact have effective power simply as the sum of individual powers, the matrix method naturally handles separations and thicknesses in general arrangements.^[30]

Applications and Measurement

In Vision Correction

Optical power plays a central role in vision correction by compensating for refractive errors in the human eye through appropriately powered lenses. In cases of myopia, or nearsightedness, the eye's excessive converging power causes distant objects to focus in front of the retina, requiring diverging lenses with negative dioptric values to shift the focus onto the retina. Conversely, hyperopia, or farsightedness, results from insufficient converging power, leading to a focus behind the retina; this is corrected using converging lenses with positive dioptric power to achieve proper focus.^[9]^[31] Presbyopia, an age-related loss of the eye's ability to accommodate for near vision due to reduced lens flexibility, typically begins around age 40 and affects most individuals over 50. It is corrected with positive power lenses, such as reading glasses or the near-vision segment in bifocals or progressive lenses, with additions usually ranging from +1.00 to +2.75 diopters depending on the required near working distance.^[32] Astigmatism arises from irregular corneal or lenticular curvature, creating unequal refractive power along different meridians and resulting in blurred vision at all distances. Correction typically involves cylindrical lenses, which provide power in a specific meridian to neutralize the astigmatic error, combined with spherical lenses for any accompanying myopia or hyperopia. Prescriptions are denoted in sphero-cylindrical form, such as "sphere power + cylinder power × axis," where the cylinder power corrects the astigmatic component and the axis indicates its orientation.^[33]^[34] When prescribing contact lenses versus spectacles, adjustments for vertex distance—the separation between the lens and the corneal vertex—are essential, as this distance affects the effective power. Spectacles typically sit about 12 mm from the cornea, necessitating a power conversion for contact lenses to ensure equivalent correction, particularly for higher prescriptions where the difference can exceed 0.25 diopters.^[35]^[36] The classification of refractive errors traces back to the work of Dutch ophthalmologist Franciscus Cornelis Donders, whose 1864 publication On the Anomalies of Accommodation and Refraction of the Eye provided a systematic foundation for understanding and correcting them. The diopter unit for measuring lens power was later formalized in 1872 by Louis Émile Javal at the International Congress of Ophthalmology, with Donders' support, enabling standardized clinical prescriptions and modern vision correction practices.^[37]^[38]

Measurement Techniques

One common method to determine the optical power of a converging lens involves measuring its focal length using a collimated beam setup. In this technique, a collimated laser beam of known diameter is directed through the lens, forming a focused spot whose position is measured relative to the lens principal plane; the focal length

f

is the distance from the lens to this spot, and the power

P

is calculated as

P = 1/f

(in meters, yielding diopters). For diverging lenses, the method can be adapted by using an auxiliary converging lens to form a real image, from which the virtual focal length is determined. This approach leverages paraxial optics and can achieve uncertainties on the order of 0.1% for well-aligned systems, depending on beam quality and positioning accuracy.^[39]^[23] For higher precision, autocollimation methods are employed, particularly in locating focal points and nodal planes. Here, a light source and objective lens project a reticle image to infinity, which reflects off a mirror placed near the test lens's focal plane; the lens is rotated about its rear nodal point until the reflected image aligns with the original, allowing measurement of the vertex-to-focal-point distance to compute

f

.^[40] This nodal slide variant provides focal length determinations with precision limited by depth-of-focus effects, typically achieving resolutions better than 0.5 mm for visible wavelengths.^[23] Interferometric techniques offer sub-micron accuracy for optical power measurement, essential for high-precision optics. Laser interferometry, such as Fizeau or Shack-Hartmann wavefront sensing, analyzes the curvature of the wavefront after passing through the lens by comparing interference fringes or local slopes to a reference; the effective focal length is derived from the wavefront radius of curvature.^[41] These methods can resolve focal lengths with uncertainties below 0.5%, enabling sub-micron precision in power calculations for components like microlens arrays.^[42]^[23] Direct measurement of surface radii using a lens clock or spherometer provides an alternative for computing power via the lensmaker's formula. A lens clock, a specialized spherometer with three contact points, measures the sagitta (sag) of the lens surface over a fixed baseline

D

, yielding radius

R \approx D^2 / (8 \cdot \text{sag})

; power is then obtained assuming a refractive index.^[43] Spherometers offer greater accuracy by using a micrometer for sag over a larger ring or pins, suitable for convex or concave surfaces with resolutions around 1-10 μm.^[43] In modern applications, particularly for ophthalmic lenses, wavefront aberrometers assess effective power by mapping aberrations across the pupil. Devices like Shack-Hartmann sensors capture the full wavefront distortion, deriving the low-order defocus term (equivalent to sphere power) alongside higher-order aberrations; this yields the effective optical power for customized lenses with resolutions down to 0.01 diopters.^[44] Such tools enable precise characterization of aspheric or progressive lenses, improving outcomes in vision correction design.^[45]

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