Varifocal optical system and associated electro-mechanical control

Claim 2

A varifocal optical system controlled electro-mechanically for focal distance variation and thus magnification, temperature correction focussing and finite distance focussing, comprising four single element lenses, two of said lenses being movable and axially translatable to vary the magnification, only one of the two movable lenses being adapted for temperature correction focussing and finite distance focussing, and electro-mechanical means for controlling the movement of the two movable lenses in a discrete manner.

Claim 3

A varifocal optical system as claimed in claim 1, wherein a convergence adjustment of the two remaining non-movable lenses is carried out during assembly of the system so as to compensate for rotational errors (curvature of the lenses, thicknesses) caused during manufacture of the lenses and for positioning errors of the tubes on which said lenses are mounted.

Claim 4

A varifocal optical system as claimed in claim 1 or 2, wherein the electro-mechanical means for controlling the movements of the two movable lenses, includes a computing unit, taking into account for focussing corrections discrete proximity values and discrete temperature values computed in such a way that the image remains sharp without compensation between two successive values, the corrections being made in terms of elementary increments so that the computing unit is required to perform additions only.

Claim 5

A varifocal optical system as claimed in claim 1, whose electro-mechanical means for independently controlling the independent movements of the two movable lenses comprise two motors for moving two carriages on which the tubes for the two movable lenses are fixed, wherein the two motors are connected to the two carriages by means of two screws without clearance.

Claim 6

A varifocal optical system as claimed in claim 1, wherein temperature corrections for focussing and finite distance focussing corrections are treated in terms of perturbations with respect to the normal configuration: nominal temperature T and object situated at infinity, and in that the temperature corrections for focussing are decorrelated with the finite distance focussing corrections, which means that for a temperature T+Δt and an object at finite distance a first correction is carried out by refocussing for an object situated at infinity at the temperature T+Δt, a second correction is carried out by refocussing while taking the proximity of the object into account and assuming the temperature to be equal to T.

Claim 7

A varifocal optical system as claimed in claim 1, wherein the four lenses are constructed and adjusted in conformity with the following Table of values in which the term "radius" denotes the radius of curvature of a surface, "next thickness" denotes the interval between a said surface and the next surface, which interval is measured along the optical axis, "radius", "next thickness" and "1/2 useful diameter" are expressed in mm, ______________________________________ Number of 1/2 Useful Next the surface Radius diameter Next material thickness ______________________________________ 2 172.779 58.662 Ge 8.659 3 conical 56.929 Air 137.553 4 conical 20.191 Ge 3.570 5 207.799 20.191 Air 3.010 6 conical 22.683 Ge 3.618 7 -434.666 22.683 Air 16.108 8 1823.132 24.874 Ge 4.272 9 -402.556 24.874 Air 101.605 ______________________________________ while the surfaces no. 3, 4 and 6 are defined in a coordinate system as follows: ______________________________________ Surface no. 3: R.sub.3 = 232.897 K.sub.3 = -3539 × 10.sup.-1 α.sub.1 = 0; i = 2, . . . ,5 Surface no. 4: R.sub.4 = -299.906 K.sub.4 = -1.0387 × 10 α.sub.1 = 0; i = 2, . . . ,5 Surface no. 6: R.sub.6 = 2446.328 K.sub.6 = -6.963 × 10.sup.3 α.sub.1 = 0; i = 2, . . . ,5 ______________________________________ said coordinate system having orthogonal axes XOY in which O is the apex of the surfaces and OX is the optical axis, and being interpreted by the following general formula, ##EQU2## in which X is a value of a point on a surface projected on the optical axis OX, Y is the height of said point which is also on a meridian including the apex, p denotes the inverse value of the radius of curvature of said meridian at the apex, K denotes the coefficient of conicity and α i denotes the general coefficients of asphericity.

Claim 8

A varifocal optical system as claimed in claim 1, wherein the four lenses do not have any aspherical surface and are realized and adjusted in conformity with the following Table of values in which the term "radius" denotes the radius of curvature of the surface, "next thickness" denotes the interval between the said surface and the next surface, which interval is measured along the optical axis, while "radius", "next thickness" and "1/2 useful diameter" are expressed in mm, ______________________________________ Number of 1/2 Useful Next the surface Radius diameter Next material thickness ______________________________________ 2 184.061 23.064 Ge 7.467 3 271.718 21.871 Air 12.488 4 -268.122 17.435 Ge 4.975 5 436.944 17.170 Air 48.633 6 -805.109 16.619 Ge 5.494 7 -273.040 17.080 Air 44.322 8 939.345 24.873 Ge 6.520 9 -597.199 25.001 Air 121.846. ______________________________________