Optical invariants are mathematical expressions representing several optical parameters. The values for each optical invariant are constant despite the fact that optical parameters change from one part or element of the optical system to another.

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Optical invariants are significant during optical systems design because they make it possible to achieve quicker results while avoiding mistakes in optical paramtersβ calculations.

There are 4 main invariants of optical systems:

Lagrange-Helmholtz invariant for paraxial optics

Abbe sine condition for high aperture systems

Straubel invariant for illuminating optical systems with light pencils transformation

Etendue invariant for illuminating optical systems with extended source

## Lagrange-Helmholtz invariant

- π¦ and π¦β² are heights of object and image
- πΌ and πΌβ aperture angles in object and image spaces
- π and πβ are indices of refraction in object and image spaces

In case of small angles and ray heights, the relation between these parameters is represented below.

This is a well known invariant of Lagrange-Helmholtz. It shows that the product of aperture angle and field height is constant in image and object space. This relation works for any optical system with any number of optical components.

This invariant defines the relation between image aperture angle and image height when the object aperture angle and height are known and fixed. The main optical parameters of the optical system can then be defined.

In an existing optical system, Lagrange-Helmholtz makes it possible to estimate the relation between two pair parameters of object and image.

### Modifications of Lagrange-Helmholtz invariant for different methods of object to image conjugation

#### Infinite to finite conjugation

Example: Objective lens of camera

Where Ο is field angle, D0/2 is half of aperture diameter, F is f-number.

#### Infinite to infinite conjugation

Example: Galilean telescope system

Where Ο is field angle, D0/2 is half of aperture diameter, F is f-number.

### Lagrange-Helmholtz invariant application

Lagrange-Helmholtz invariant is very important for estimating the relation of parameters of systems in paraxial region, where apertures and fields of view are quite small.

This invariant defines the main parameters of paraxial optical systems: focal lengths, magnification, positions of object and image, entrance and exit pupil, and principal planes.

## Abbe sine condition

Lagrange-Helmholtz invariant is true for any optical system with relatively small y (Ο) and Ξ±. For an optical system where essential Ξ± is similar to a microscope lens, a more accurate invariant is needed, the Abbe sine condition.

Comparison of Lagrange-Helmholtz invariant with Abbe sine condition shows that Sine condition uses the sinus of aperture angles instead of their values.

### Abbe sine condition application

Sine condition is true for optical systems that donβt have spherical aberrations and coma. Vice versa, if sine condition is true for a given optical system, that system doesnβt have spherical aberration and coma. It is named aplanatic. In other words, sine condition is a condition of aplanatism. This is a key indicator of a microscope lens performance.

Β If the optical system has residual aberrations, this can be characterized as OSC (offense against the sine condition). The level of deviation from sine condition shows the extent of proximity of the concerned optical system to an aplanatic one.

One effect from sine condition is that the maximal aperture aplanatic systems is 0.5, though non achievable.

## Light pencil invariant and Straubel theorem for transferring

Letβs consider the propagation of a light pencil beam through the refractive surface (Fig. 5).Β The volume of a light pencil is limited by surfaces ππ1, ππΒ and the marginal rays between them. Two light pencil beams are presented on Fig. 5:

Between ππ1 surface and refractive surface ππ

Between refractive surface ππ and surface ππ2

Rays propagating between surfaces form several solid angles are πΞ©, πΞ©1, and πΞ©2. The light pencil invariant demonstrates the interrelation of these angles and surfaces:

Straubel theorem takes into account the media refraction coefficient with different indices refraction π and πβ.

This equation is valid for any number of reflections and/or refractions.

## Etendue invariant

A real optical system works with extended sources with square π and finite apertures determined by the sizes and system construction. The light spot area generated by rays passed through the optical system is determined by the Etendue invariant:

where S and Sβ are areas of source and its image and Ξ© is the solid angle which is defined as follows:

where π’ is aperture angle.

Accordingly, the Etendue invariant is:

### Etendue invariant application

#### The limit of light spot size

We can use the Etendue invariant to find the ratio of source area and the light spot area formed with the help of optics.

The maximum value of sine function for the image aperture angle is 1 when the angle π’β=90Β°. In this case, the ratio will have a maximum value (πΆπππ₯). Its formula is:

#### Throughput of LED illumination optical system

If the optics are not large enough to overcome the source Etendue, there will be an additional efficiency loss. In this case,the source Etendue will be limited by optics Etendue; the Etendue invariant will not work. It can however help in finding loss levels and even in optimizing them with the help of this formula:

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