Optics and photonics — Test methods for telescopic systems — Part 3: Test methods for telescopic sights

This document specifies test equipment and test procedures for determination of the following optical characteristics of telescopic sights: — axial parallax; — parallax; — eye relief range, eye relief, critical eye relief; — reticle tracking; — line of sight shift due to zooming; — line of sight shift due to focusing.

Optique et photonique — Méthodes d'essai pour systèmes télescopiques — Partie 3: Méthodes d'essai pour viseurs de tir

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Status
Published
Publication Date
22-Mar-2021
Current Stage
6060 - International Standard published
Start Date
23-Mar-2021
Due Date
22-May-2022
Completion Date
23-Mar-2021
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INTERNATIONAL ISO
STANDARD 14490-3
Third edition
2021-03
Optics and photonics — Test methods
for telescopic systems —
Part 3:
Test methods for telescopic sights
Optique et photonique — Méthodes d'essai pour systèmes
télescopiques —
Partie 3: Méthodes d'essai pour viseurs de tir
Reference number
ISO 14490-3:2021(E)
©
ISO 2021

---------------------- Page: 1 ----------------------
ISO 14490-3:2021(E)

COPYRIGHT PROTECTED DOCUMENT
© ISO 2021
All rights reserved. Unless otherwise specified, or required in the context of its implementation, no part of this publication may
be reproduced or utilized otherwise in any form or by any means, electronic or mechanical, including photocopying, or posting
on the internet or an intranet, without prior written permission. Permission can be requested from either ISO at the address
below or ISO’s member body in the country of the requester.
ISO copyright office
CP 401 • Ch. de Blandonnet 8
CH-1214 Vernier, Geneva
Phone: +41 22 749 01 11
Email: copyright@iso.org
Website: www.iso.org
Published in Switzerland
ii © ISO 2021 – All rights reserved

---------------------- Page: 2 ----------------------
ISO 14490-3:2021(E)

Contents Page
Foreword .v
1 Scope . 1
2 Normative references . 1
3 Terms and definitions . 1
4 Method of measurement of axial parallax . 1
4.1 Principle . 1
4.2 Test arrangement . 2
4.2.1 General. 2
4.2.2 Collimator . 2
4.2.3 Telescopic sight . 2
4.2.4 Dioptric tester . 3
4.3 Measurement procedure . 3
4.4 Test report . 3
5 Method of measurement of parallax . 3
5.1 Principle . 3
5.2 Test arrangement . 4
5.2.1 General. 4
5.2.2 Collimator . 4
5.2.3 Telescopic sight . 4
5.2.4 Light stop . 4
5.2.5 Auxiliary telescope . 5
5.3 Measurement procedure . 5
5.4 Test report . 6
6 Method of measurement of eye relief range, eye relief and critical eye relief.6
6.1 Principle . 6
6.2 Test arrangement . 6
6.2.1 General. 6
6.2.2 Collimator . 6
6.2.3 Telescopic sight . 6
6.2.4 Measuring magnifier . 7
6.3 Measurement procedure . 7
6.4 Test report . 8
7 Method of measurement of reticle tracking . 8
7.1 Principle . 8
7.2 Test arrangement . 8
7.2.1 General. 8
7.2.2 Collimator . 8
7.3 Test procedure . 9
7.4 Test report . 9
8 Method of measurement of line of sight shift due to zooming . 9
8.1 Principle . 9
8.2 Test arrangement . 9
8.2.1 General. 9
8.2.2 Test specimen mounting .11
8.2.3 Auxiliary telescope .11
8.3 Test procedure .11
8.3.1 Preparation of the test assembly .11
8.3.2 Determination of the measurement values .11
8.4 Precision of the measurement .12
8.5 Test report .12
9 Method of measurement of line of sight shift due to focusing .12
© ISO 2021 – All rights reserved iii

---------------------- Page: 3 ----------------------
ISO 14490-3:2021(E)

9.1 Principle .12
9.2 Test arrangement .12
9.2.1 General.12
9.2.2 Collimator .13
9.2.3 Telescopic sight .14
9.2.4 Auxiliary telescope .14
9.3 Test procedure .14
9.3.1 Preparation of the test assembly .14
9.3.2 Determination of the measurement values .14
9.4 Precision of the measurement .14
9.5 Test report .14
10 General test report .15
Bibliography .16
iv © ISO 2021 – All rights reserved

---------------------- Page: 4 ----------------------
ISO 14490-3:2021(E)

Foreword
ISO (the International Organization for Standardization) is a worldwide federation of national standards
bodies (ISO member bodies). The work of preparing International Standards is normally carried out
through ISO technical committees. Each member body interested in a subject for which a technical
committee has been established has the right to be represented on that committee. International
organizations, governmental and non-governmental, in liaison with ISO, also take part in the work.
ISO collaborates closely with the International Electrotechnical Commission (IEC) on all matters of
electrotechnical standardization.
The procedures used to develop this document and those intended for its further maintenance are
described in the ISO/IEC Directives, Part 1. In particular, the different approval criteria needed for the
different types of ISO documents should be noted. This document was drafted in accordance with the
editorial rules of the ISO/IEC Directives, Part 2 (see www .iso .org/ directives).
Attention is drawn to the possibility that some of the elements of this document may be the subject of
patent rights. ISO shall not be held responsible for identifying any or all such patent rights. Details of
any patent rights identified during the development of the document will be in the Introduction and/or
on the ISO list of patent declarations received (see www .iso .org/ patents).
Any trade name used in this document is information given for the convenience of users and does not
constitute an endorsement.
For an explanation of the voluntary nature of standards, the meaning of ISO specific terms and
expressions related to conformity assessment, as well as information about ISO's adherence to the
World Trade Organization (WTO) principles in the Technical Barriers to Trade (TBT), see www .iso .org/
iso/ foreword .html.
This document was prepared by Technical Committee ISO/TC 172, Optics and photonics, Subcommittee
SC 4, Telescopic systems.
This third edition cancels and replaces the second edition (ISO 14490-3:2016), which has been
technically revised. The main changes compared to the previous edition are as follows:
— critical eye relief added in the test method according to ISO 14135 series and ISO 14132-3.
A list of all parts in the ISO 14490 series can be found on the ISO website.
Any feedback or questions on this document should be directed to the user’s national standards body. A
complete listing of these bodies can be found at www .iso .org/ members .html.
© ISO 2021 – All rights reserved v

---------------------- Page: 5 ----------------------
INTERNATIONAL STANDARD ISO 14490-3:2021(E)
Optics and photonics — Test methods for telescopic
systems —
Part 3:
Test methods for telescopic sights
1 Scope
This document specifies test equipment and test procedures for determination of the following optical
characteristics of telescopic sights:
— axial parallax;
— parallax;
— eye relief range, eye relief, critical eye relief;
— reticle tracking;
— line of sight shift due to zooming;
— line of sight shift due to focusing.
2 Normative references
The following documents are referred to in the text in such a way that some or all of their content
constitutes requirements of this document. For dated references, only the edition cited applies. For
undated references, the latest edition of the referenced document (including any amendments) applies.
ISO 14132-1, Optics and photonics — Vocabulary for telescopic systems — Part 1: General terms and
alphabetical indexes of terms in ISO 14132
ISO 14132-3, Optics and photonics — Vocabulary for telescopic systems — Part 3: Terms for telescopic sights
ISO 14135-1:2021, Optics and photonics — Specifications for telescopic sights — Part 1: General-purpose
instruments
ISO 14135-2:2021, Optics and photonics — Specifications for telescopic sights — Part 2: High-performance
instruments
3 Terms and definitions
For the purposes of this document, the terms and definitions given in ISO 14132-1 and ISO 14132-3 apply.
4 Method of measurement of axial parallax
4.1 Principle
This test method describes the measurement of the axial distance between the reticle of a telescopic
sight and an image, formed by the objective lens of this telescopic sight (where the reticle is in the first
image plane) or by the objective lens and erecting system (where the reticle is in the second image
© ISO 2021 – All rights reserved 1

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ISO 14490-3:2021(E)

plane). The distance between the reticle of the telescopic sight and image plane of the collimator reticle
−1
along the optical axis, p′ , is expressed in dioptres (m ) and measured with the auxiliary telescope.
ax
4.2 Test arrangement
4.2.1 General
Measurement of the axial parallax shall be carried out with the test arrangement shown in Figure 1.
It shall be possible to adjust the alignment of the collimator and the telescopic sight relative to each
other. This can be achieved by adjusting the collimator and/or the telescopic sight.
Key
1 collimator 6 filter
2 telescopic sight 7 reticle of collimator
3 dioptric tester 8 reticle of telescopic sight
4 observer’s eye 9 image plane of collimator reticle
5 illumination unit 10 reticle of dioptric tester
Figure 1 — Test arrangement for measuring axial parallax
4.2.2 Collimator
The collimator shall have a useful diameter larger than the objective lens diameter of the telescopic
sight under test and a focal length of at least ten times the diameter of the collimator lens.
The reticle of the collimator should have geometric features appropriate to assess the offset, e.g. a
cross-hair. The axial position of this reticle shall be correctly adjusted to form an image at the specified
parallax-free distance of the telescopic sight under test.
The illumination unit shall create a uniform brightness over the aperture of the collimator.
To avoid chromatic aberrations, a green filter (~0,55 µm) shall be used.
4.2.3 Telescopic sight
The telescopic sight and/or the collimator shall be adjusted relative to each other so that both optical
axes are parallel and in such a position that the objective lens of the telescopic sight is completely
illuminated.
The centre of the reticle of the telescopic sight shall be near the optical axis of the sight.
2 © ISO 2021 – All rights reserved

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ISO 14490-3:2021(E)

4.2.4 Dioptric tester
The dioptric tester shall have an aperture larger than the exit pupil of the telescopic sight and a
magnifying power sufficient to ensure a precise measurement (i.e. ×3 to ×6).
4.3 Measurement procedure
Set the dioptric tester to zero with its eyepiece adjusted to obtain a sharp image of its own reticle.
The eyepiece of the telescopic sight shall be focused on the reticle of the telescopic sight to obtain a
sharp image while viewing through the dioptric tester.
For telescopic sights with a fixed eyepiece, use the dioptric tester to focus on the reticle of the
telescopic sight.
The dioptre setting of the dioptric tester shall be adjusted to obtain a sharp image of the collimator
reticle.
The axial parallax in the image space, p′ , shall be determined by the difference of the two readings on
ax
the dioptric tester.
−1
The uncertainty of measurement for p′ (expressed in m ) shall not exceed Formula (1):
ax
27,
−1
uncertaintymp′≤ (1)
ax
62
10 ⋅D′
where
-1
p′ is the axial parallax in the image space in m ;
ax
D' is the exit pupil diameter of the telescopic sight expressed in metres.
For exit pupil diameters larger than 7 mm, the value in the formula shall be D′ = 0,007 m.
The axial parallax in the object space, p , is calculated as given in Formula (2):
ax
p′
ax
p = (2)
ax
2
Γ
where Γ is the magnifying power of the telescopic sight under test.
NOTE The image quality of the test setup (including the telescopic sight under test) influences the
measurement error.
4.4 Test report
A test report shall be presented and shall include the general information specified in Clause 10 and the
result of the test as specified in 4.3.
5 Method of measurement of parallax
5.1 Principle
This method describes the determination of the angular deviation between the aiming lines for on-axis
and off-axis observation.
NOTE For exit pupil diameters of approximately 2 mm or less, only the test method for axial parallax is
appropriate.
© ISO 2021 – All rights reserved 3

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ISO 14490-3:2021(E)

5.2 Test arrangement
5.2.1 General
Measurement of the parallax shall be carried out with the test arrangement shown in Figure 2.
It shall be possible to adjust the alignment of the collimator and the telescopic sight relative to each
other. This can be achieved by adjusting the collimator and/or the telescopic sight.
Key
1 collimator 6 filter
2 telescopic sight 7 reticle of collimator
3 auxiliary telescope 8 light stop, off-axis
4 observer’s eye 9 reticle of telescopic sight
5 illumination unit 10 reticle of auxiliary telescope
Figure 2 — Test arrangement for measuring parallax
5.2.2 Collimator
The collimator shall have a diameter larger than the objective lens diameter of the telescopic sight
under test and a focal length of at least ten times the diameter of the collimator lens.
The reticle of the collimator should have geometric features appropriate to assess the offset, e.g. a
cross-hair. The axial position of this reticle shall be correctly adjusted to form an image at the specified
parallax-free distance of the telescopic sight under test.
The illumination unit shall create a uniform brightness over the aperture of the collimator. To avoid
chromatic aberrations, a green filter (~0,55 µm) shall be used.
5.2.3 Telescopic sight
The telescopic sight and/or the collimator shall be adjusted relative to each other so that both optical
axes are parallel and in such a position that the objective lens of the telescopic sight is completely
illuminated.
The centre of the reticle of the telescopic sight shall be near the optical axis of the sight.
5.2.4 Light stop
The light stop shall have a diameter, d, in millimetres, (see Figure 2) of d = (1,2 ± 0,1) Γ where Γ is the
magnifying power of the telescopic sight under test.
The light stop shall be adjustable in a horizontal direction over the whole diameter of the entrance
pupil of the telescopic sight.
4 © ISO 2021 – All rights reserved

---------------------- Page: 9 ----------------------
ISO 14490-3:2021(E)

5.2.5 Auxiliary telescope
The auxiliary telescope shall have an aperture larger than the exit pupil of the telescopic sight and a
magnification sufficient to ensure a precise measurement.
The auxiliary telescope reticle shall have a scale in minutes of arc on its horizontal axis, with
subdivisions of at most 2 min of arc (MOA).
The auxiliary telescope shall be focused to infinity.
5.3 Measurement procedure
The eyepiece of the telescopic sight shall be focused on the reticle of the telescopic sight to obtain a
sharp image while viewing through the auxiliary telescope.
Adjust the light stop to two opposite positions, so that in each of them, its outer edge corresponds to the
edge of the entrance pupil of the telescopic sight.
Use the auxiliary telescope to determine the change, α, in MOA, of the angular deviation between the
images of the collimator reticle and the telescopic sight reticle in the two light stop positions (see
Figure 3).
Key
1 telescopic sight
2 reticle of telescopic sight
3 image plane of collimator reticle
α change, in MOA, of the angular deviation between the images of the collimator reticle and the telescopic sight
reticle in the two light stop positions
Figure 3 — Explanation of measurement of quantity, α
The parallax p′ in the image space is calculated as given in Formula (3):
α
p′= (3)
2
The maximum parallax in the object space p is calculated as given in Formula (4):
p′
p= (4)
Γ
where Γ is the magnifying power of the telescopic sight under test.
© ISO 2021 – All rights reserved 5

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ISO 14490-3:2021(E)

The uncertainty of measurement for p′ shall not exceed 1,0 MOA.
NOTE For practical purposes, the relations between parallax and axial parallax are given by the following
formulae:
D′
pp′′= expressed in milliradians;
ax
2
D′
pp′′=×3,438 expressed in minutes of arc;
ax
2
where D′ is the exit pupil diameter, expressed in millimetres.
5.4 Test report
A test report shall be presented and shall include the general information specified in Clause 10 and the
result of the test as specified in 5.3.
6 Method of measurement of eye relief range, eye relief and critical eye relief
6.1 Principle
This method describes the determination of that eye position range along the optical axis of a telescopic
sight, which still allows observation of the full field of view.
For this method, a mean daylight eye pupil of 3 mm in diameter is assumed.
For an illustration of eye relief range, eye relief and critical eye relief see Figure 4. For documentation
purposes, the eye relief range is given as “d to d ”. Eye relief is d and critical eye relief is d .
min max max rim
6.2 Test arrangement
6.2.1 General
Measurement of the eye relief range shall be carried out with the test arrangement shown in Figure 4.
It shall be possible to adjust the alignment of the collimator and the telescopic sight relative to each
other. This can be achieved by adjusting the collimator and/or the telescopic sight.
6.2.2 Collimator
The collimator shall have a useful diameter larger than that of the objective lens of the telescopic sight
under test and a focal length of at least ten times the diameter of the collimator lens.
The collimator shall have two point-shaped light sources positioned in the focal plane of the collimator.
In the case of a telescopic sight without parallax adjustment, the two point-shaped light sources shall
be positioned in such way that their images appear in the parallax-free distance. These light sources
shall be adjustable symmetrically about the optical axis in correspondence to the field of view of the
telescopic sight.
To avoid chromatic aberration, a green filter (~0,55 µm) shall be used.
6.2.3 Telescopic sight
The reticle of the telescopic sight shall be near the optical axis of the sight. The telescopic sight shall be
adjustable relative to the collimator around two mutually orthogonal axes lying in a plane perpendicular
to the optical axis.
6 © ISO 2021 – All rights reserved

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ISO 14490-3:2021(E)

6.2.4 Measuring magnifier
The measuring magnifier should have a magnifying power of approximately ten times and a reticle with
a graduation of 0,1 mm. The graduated side of the reticle is positioned as close to the diffusing surface
of the screen as possible.
The optical axis of the measuring magnifier is positioned parallel to the optical axis of the telescopic
sight. The measuring magnifier is adjustable in the axial direction.
Dimensions in millimetres
Key
1 collimator
2 telescopic sight
3 diffusing screen
4 glass with scale
5 measuring magnifier
NOTE Sectional views A-A, B-B and C-C show appearance of ray bundles at distances d , d and d ,
min med max
respectively.
Figure 4 — Test arrangement for measuring eye relief range, eye relief and critical eye relief
6.3 Measurement procedure
Adjust the distance between the two light sources of the collimator corresponding to the field of view of
the telescopic sight under test.
Align the telescopic sight so that the edge line of the field of view corresponds with the images of the
two light sources.
© ISO 2021 – All rights reserved 7

---------------------- Page: 12 ----------------------
ISO 14490-3:2021(E)

Move the measuring magnifier, starting from a position close to the telescopic sight, along the optical
axis until the inner edges of the two ray bundles are at a distance of 2 mm (see Figure 4, section A-A).
In this position, 0,5 mm of the meridional extension of each of the two ray bundles are covered by a
mean daylight eye pupil of 3 mm in diame
...

FINAL
INTERNATIONAL ISO/FDIS
DRAFT
STANDARD 14490-3
ISO/TC 172/SC 4
Optics and photonics — Test methods
Secretariat: DIN
for telescopic systems —
Voting begins on:
2020-12-24
Part 3:
Voting terminates on:
Test methods for telescopic sights
2021-02-18
Optique et photonique — Méthodes d'essai pour systèmes
télescopiques —
Partie 3: Méthodes d'essai pour viseurs de tir
RECIPIENTS OF THIS DRAFT ARE INVITED TO
SUBMIT, WITH THEIR COMMENTS, NOTIFICATION
OF ANY RELEVANT PATENT RIGHTS OF WHICH
THEY ARE AWARE AND TO PROVIDE SUPPOR TING
DOCUMENTATION.
IN ADDITION TO THEIR EVALUATION AS
Reference number
BEING ACCEPTABLE FOR INDUSTRIAL, TECHNO-
ISO/FDIS 14490-3:2021(E)
LOGICAL, COMMERCIAL AND USER PURPOSES,
DRAFT INTERNATIONAL STANDARDS MAY ON
OCCASION HAVE TO BE CONSIDERED IN THE
LIGHT OF THEIR POTENTIAL TO BECOME STAN-
DARDS TO WHICH REFERENCE MAY BE MADE IN
©
NATIONAL REGULATIONS. ISO 2021

---------------------- Page: 1 ----------------------
ISO/FDIS 14490-3:2021(E)

COPYRIGHT PROTECTED DOCUMENT
© ISO 2021
All rights reserved. Unless otherwise specified, or required in the context of its implementation, no part of this publication may
be reproduced or utilized otherwise in any form or by any means, electronic or mechanical, including photocopying, or posting
on the internet or an intranet, without prior written permission. Permission can be requested from either ISO at the address
below or ISO’s member body in the country of the requester.
ISO copyright office
CP 401 • Ch. de Blandonnet 8
CH-1214 Vernier, Geneva
Phone: +41 22 749 01 11
Email: copyright@iso.org
Website: www.iso.org
Published in Switzerland
ii © ISO 2021 – All rights reserved

---------------------- Page: 2 ----------------------
ISO/FDIS 14490-3:2021(E)

Contents Page
Foreword .v
1 Scope . 1
2 Normative references . 1
3 Terms and definitions . 1
4 Method of measurement of axial parallax . 1
4.1 Principle . 1
4.2 Test arrangement . 2
4.2.1 General. 2
4.2.2 Collimator . 2
4.2.3 Telescopic sight . 2
4.2.4 Dioptric tester . 3
4.3 Measurement procedure . 3
4.4 Test report . 3
5 Method of measurement of parallax . 3
5.1 Principle . 3
5.2 Test arrangement . 4
5.2.1 General. 4
5.2.2 Collimator . 4
5.2.3 Telescopic sight . 4
5.2.4 Light stop . 4
5.2.5 Auxiliary telescope . 5
5.3 Measurement procedure . 5
5.4 Test report . 6
6 Method of measurement of eye relief range, eye relief and critical eye relief.6
6.1 Principle . 6
6.2 Test arrangement . 6
6.2.1 General. 6
6.2.2 Collimator . 6
6.2.3 Telescopic sight . 6
6.2.4 Measuring magnifier . 7
6.3 Measurement procedure . 7
6.4 Test report . 8
7 Method of measurement of reticle tracking . 8
7.1 Principle . 8
7.2 Test arrangement . 8
7.2.1 General. 8
7.2.2 Collimator . 8
7.3 Test procedure . 9
7.4 Test report . 9
8 Method of measurement of line of sight shift due to zooming . 9
8.1 Principle . 9
8.2 Test arrangement . 9
8.2.1 General. 9
8.2.2 Test specimen mounting .11
8.2.3 Auxiliary telescope .11
8.3 Test procedure .11
8.3.1 Preparation of the test assembly .11
8.3.2 Determination of the measurement values .11
8.4 Precision of the measurement .12
8.5 Test report .12
9 Method of measurement of line of sight shift due to focusing .12
© ISO 2021 – All rights reserved iii

---------------------- Page: 3 ----------------------
ISO/FDIS 14490-3:2021(E)

9.1 Principle .12
9.2 Test arrangement .12
9.2.1 General.12
9.2.2 Collimator .13
9.2.3 Telescopic sight .14
9.2.4 Auxiliary telescope .14
9.3 Test procedure .14
9.3.1 Preparation of the test assembly .14
9.3.2 Determination of the measurement values .14
9.4 Precision of the measurement .14
9.5 Test report .14
10 General test report .15
Bibliography .16
iv © ISO 2021 – All rights reserved

---------------------- Page: 4 ----------------------
ISO/FDIS 14490-3:2021(E)

Foreword
ISO (the International Organization for Standardization) is a worldwide federation of national standards
bodies (ISO member bodies). The work of preparing International Standards is normally carried out
through ISO technical committees. Each member body interested in a subject for which a technical
committee has been established has the right to be represented on that committee. International
organizations, governmental and non-governmental, in liaison with ISO, also take part in the work.
ISO collaborates closely with the International Electrotechnical Commission (IEC) on all matters of
electrotechnical standardization.
The procedures used to develop this document and those intended for its further maintenance are
described in the ISO/IEC Directives, Part 1. In particular, the different approval criteria needed for the
different types of ISO documents should be noted. This document was drafted in accordance with the
editorial rules of the ISO/IEC Directives, Part 2 (see www .iso .org/ directives).
Attention is drawn to the possibility that some of the elements of this document may be the subject of
patent rights. ISO shall not be held responsible for identifying any or all such patent rights. Details of
any patent rights identified during the development of the document will be in the Introduction and/or
on the ISO list of patent declarations received (see www .iso .org/ patents).
Any trade name used in this document is information given for the convenience of users and does not
constitute an endorsement.
For an explanation of the voluntary nature of standards, the meaning of ISO specific terms and
expressions related to conformity assessment, as well as information about ISO's adherence to the
World Trade Organization (WTO) principles in the Technical Barriers to Trade (TBT), see www .iso .org/
iso/ foreword .html.
This document was prepared by Technical Committee ISO/TC 172, Optics and photonics, Subcommittee
SC 4, Telescopic systems.
This third edition cancels and replaces the second edition (ISO 14490-3:2016), which has been
technically revised. The main changes compared to the previous edition are as follows:
— critical eye relief added in the test method according to ISO 14135 series and ISO 14132-3.
A list of all parts in the ISO 14490 series can be found on the ISO website.
Any feedback or questions on this document should be directed to the user’s national standards body. A
complete listing of these bodies can be found at www .iso .org/ members .html.
© ISO 2021 – All rights reserved v

---------------------- Page: 5 ----------------------
FINAL DRAFT INTERNATIONAL STANDARD ISO/FDIS 14490-3:2021(E)
Optics and photonics — Test methods for telescopic
systems —
Part 3:
Test methods for telescopic sights
1 Scope
This document specifies test equipment and test procedures for determination of the following optical
characteristics of telescopic sights:
— axial parallax;
— parallax;
— eye relief range, eye relief, critical eye relief;
— reticle tracking;
— line of sight shift due to zooming;
— line of sight shift due to focusing.
2 Normative references
The following documents are referred to in the text in such a way that some or all of their content
constitutes requirements of this document. For dated references, only the edition cited applies. For
undated references, the latest edition of the referenced document (including any amendments) applies.
ISO 14132-1, Optics and photonics — Vocabulary for telescopic systems — Part 1: General terms and
alphabetical indexes of terms in ISO 14132
ISO 14132-3, Optics and photonics — Vocabulary for telescopic systems — Part 3: Terms for telescopic sights
ISO 14135-1:—, Optics and photonics — Specifications for telescopic sights — Part 1: General-purpose
instruments
ISO 14135-2:—, Optics and photonics — Specifications for telescopic sights — Part 2: High-performance
instruments
3 Terms and definitions
For the purposes of this document, the terms and definitions given in ISO 14132-1 and ISO 14132-3 apply.
4 Method of measurement of axial parallax
4.1 Principle
This test method describes the measurement of the axial distance between the reticle of a telescopic
sight and an image, formed by the objective lens of this telescopic sight (where the reticle is in the first
image plane) or by the objective lens and erecting system (where the reticle is in the second image
© ISO 2021 – All rights reserved 1

---------------------- Page: 6 ----------------------
ISO/FDIS 14490-3:2021(E)

plane). The distance between the reticle of the telescopic sight and image plane of the collimator reticle
−1
along the optical axis, p′ , is expressed in dioptres (m ) and measured with the auxiliary telescope.
ax
4.2 Test arrangement
4.2.1 General
Measurement of the axial parallax shall be carried out with the test arrangement shown in Figure 1.
It shall be possible to adjust the alignment of the collimator and the telescopic sight relative to each
other. This can be achieved by adjusting the collimator and/or the telescopic sight.
Key
1 collimator 6 filter
2 telescopic sight 7 reticle of collimator
3 dioptric tester 8 reticle of telescopic sight
4 observer’s eye 9 image plane of collimator reticle
5 illumination unit 10 reticle of dioptric tester
Figure 1 — Test arrangement for measuring axial parallax
4.2.2 Collimator
The collimator shall have a useful diameter larger than the objective lens diameter of the telescopic
sight under test and a focal length of at least ten times the diameter of the collimator lens.
The reticle of the collimator should have geometric features appropriate to assess the offset, e.g. a
cross-hair. The axial position of this reticle shall be correctly adjusted to form an image at the specified
parallax-free distance of the telescopic sight under test.
The illumination unit shall create a uniform brightness over the aperture of the collimator.
To avoid chromatic aberrations, a green filter (~0,55 µm) shall be used.
4.2.3 Telescopic sight
The telescopic sight and/or the collimator shall be adjusted relative to each other so that both optical
axes are parallel and in such a position that the objective lens of the telescopic sight is completely
illuminated.
The centre of the reticle of the telescopic sight shall be near the optical axis of the sight.
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ISO/FDIS 14490-3:2021(E)

4.2.4 Dioptric tester
The dioptric tester shall have an aperture larger than the exit pupil of the telescopic sight and a
magnifying power sufficient to ensure a precise measurement (i.e. ×3 to ×6).
4.3 Measurement procedure
Set the dioptric tester to zero with its eyepiece adjusted to obtain a sharp image of its own reticle.
The eyepiece of the telescopic sight shall be focused on the reticle of the telescopic sight to obtain a
sharp image while viewing through the dioptric tester.
For telescopic sights with a fixed eyepiece, use the dioptric tester to focus on the reticle of the
telescopic sight.
The dioptre setting of the dioptric tester shall be adjusted to obtain a sharp image of the collimator
reticle.
The axial parallax in the image space, p′ , shall be determined by the difference of the two readings on
ax
the dioptric tester.
−1
The uncertainty of measurement for p′ (expressed in m ) shall not exceed Formula (1):
ax
27,
−1
uncertaintymp′≤ (1)
ax
62
10 ⋅D′
where
-1
p′ is the axial parallax in the image space in m ;
ax
D' is the exit pupil diameter of the telescopic sight expressed in metres.
For exit pupil diameters larger than 7 mm, the value in the formula shall be D′ = 7 mm.
The axial parallax in the object space, p , is calculated as given in Formula (2):
ax
p′
ax
p = (2)
ax
2
Γ
where Γ is the magnifying power of the telescopic sight under test.
NOTE The image quality of the test setup (including the telescopic sight under test) influences the
measurement error.
4.4 Test report
A test report shall be presented and shall include the general information specified in Clause 10 and the
result of the test as specified in 4.3.
5 Method of measurement of parallax
5.1 Principle
This method describes the determination of the angular deviation between the aiming lines for on-axis
and off-axis observation.
NOTE For exit pupil diameters of approximately 2 mm or less, only the test method for axial parallax is
appropriate.
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ISO/FDIS 14490-3:2021(E)

5.2 Test arrangement
5.2.1 General
Measurement of the parallax shall be carried out with the test arrangement shown in Figure 2.
It shall be possible to adjust the alignment of the collimator and the telescopic sight relative to each
other. This can be achieved by adjusting the collimator and/or the telescopic sight.
Key
1 collimator 6 filter
2 telescopic sight 7 reticle of collimator
3 auxiliary telescope 8 light stop, off-axis
4 observer’s eye 9 reticle of telescopic sight
5 illumination unit 10 reticle of auxiliary telescope
Figure 2 — Test arrangement for measuring parallax
5.2.2 Collimator
The collimator shall have a diameter larger than the objective lens diameter of the telescopic sight
under test and a focal length of at least ten times the diameter of the collimator lens.
The reticle of the collimator should have geometric features appropriate to assess the offset, e.g. a
cross-hair. The axial position of this reticle shall be correctly adjusted to form an image at the specified
parallax-free distance of the telescopic sight under test.
The illumination unit shall create a uniform brightness over the aperture of the collimator. To avoid
chromatic aberrations, a green filter (~0,55 µm) shall be used.
5.2.3 Telescopic sight
The telescopic sight and/or the collimator shall be adjusted relative to each other so that both optical
axes are parallel and in such a position that the objective lens of the telescopic sight is completely
illuminated.
The centre of the reticle of the telescopic sight shall be near the optical axis of the sight.
5.2.4 Light stop
The light stop shall have a diameter, d, in millimetres, (see Figure 2) of d = (1,2 ± 0,1) Γ where Γ is the
magnifying power of the telescopic sight under test.
The light stop shall be adjustable in a horizontal direction over the whole diameter of the entrance
pupil of the telescopic sight.
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ISO/FDIS 14490-3:2021(E)

5.2.5 Auxiliary telescope
The auxiliary telescope shall have an aperture larger than the exit pupil of the telescopic sight and a
magnification sufficient to ensure a precise measurement.
The auxiliary telescope reticle shall have a scale in minutes of arc on its horizontal axis, with
subdivisions of at most 2 min of arc (MOA).
The auxiliary telescope shall be focused to infinity.
5.3 Measurement procedure
The eyepiece of the telescopic sight shall be focused on the reticle of the telescopic sight to obtain a
sharp image while viewing through the auxiliary telescope.
Adjust the light stop to two opposite positions, so that in each of them, its outer edge corresponds to the
edge of the entrance pupil of the telescopic sight.
Use the auxiliary telescope to determine the change, α, in MOA, of the angular deviation between the
images of the collimator reticle and the telescopic sight reticle in the two light stop positions (see
Figure 3).
Key
1 telescopic sight
2 reticle of telescopic sight
3 image plane of collimator reticle
α change, in MOA, of the angular deviation between the images of the collimator reticle and the telescopic sight
reticle in the two light stop positions
Figure 3 — Explanation of measurement of quantity, α
The parallax p′ in the image space is calculated as given in Formula (3):
α
p′= (3)
2
The maximum parallax in the object space p is calculated as given in Formula (4):
p′
p= (4)
Γ
where Γ is the magnifying power of the telescopic sight under test.
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ISO/FDIS 14490-3:2021(E)

The uncertainty of measurement for p′ shall not exceed 1,0 MOA.
NOTE For practical purposes, the relations between parallax and axial parallax are given by the following
formulae:
D′
pp′′= expressed in milliradians;
ax
2
D′
pp′′=×3,438 expressed in minutes of arc;
ax
2
where D′ is the exit pupil diameter, expressed in millimetres.
5.4 Test report
A test report shall be presented and shall include the general information specified in Clause 10 and the
result of the test as specified in 5.3.
6 Method of measurement of eye relief range, eye relief and critical eye relief
6.1 Principle
This method describes the determination of that eye position range along the optical axis of a telescopic
sight, which still allows observation of the full field of view.
For this method, a mean daylight eye pupil of 3 mm in diameter is assumed.
For an illustration of eye relief range, eye relief and critical eye relief see Figure 4. For documentation
purposes, the eye relief range is given as “d to d ”. Eye relief is d and critical eye relief is d .
min max max rim
6.2 Test arrangement
6.2.1 General
Measurement of the eye relief range shall be carried out with the test arrangement shown in Figure 4.
It shall be possible to adjust the alignment of the collimator and the telescopic sight relative to each
other. This can be achieved by adjusting the collimator and/or the telescopic sight.
6.2.2 Collimator
The collimator shall have a useful diameter larger than that of the objective lens of the telescopic sight
under test and a focal length of at least ten times the diameter of the collimator lens.
The collimator shall have two point-shaped light sources positioned in the focal plane of the collimator.
In the case of a telescopic sight without parallax adjustment, the two point-shaped light sources shall
be positioned in such way that their images appear in the parallax-free distance. These light sources
shall be adjustable symmetrically about the optical axis in correspondence to the field of view of the
telescopic sight.
To avoid chromatic aberration, a green filter (~0,55 µm) shall be used.
6.2.3 Telescopic sight
The reticle of the telescopic sight shall be near the optical axis of the sight. The telescopic sight shall be
adjustable relative to the collimator around two mutually orthogonal axes lying in a plane perpendicular
to the optical axis.
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ISO/FDIS 14490-3:2021(E)

6.2.4 Measuring magnifier
The measuring magnifier should have a magnifying power of approximately ten times and a reticle with
a graduation of 0,1 mm. The graduated side of the reticle is positioned as close to the diffusing surface
of the screen as possible.
The optical axis of the measuring magnifier is positioned parallel to the optical axis of the telescopic
sight and adjustable in the axial direction.
Dimensions in millimetres
Key
1 collimator
2 telescopic sight
3 diffusing screen
4 glass with scale
5 measuring magnifier
NOTE Sectional views A-A, B-B and C-C show appearance of ray bundles at distances d , d and d ,
min med max
respectively.
Figure 4 — Test arrangement for measuring eye relief range, eye relief and critical eye relief
6.3 Measurement procedure
Adjust the distance between the two light sources of the collimator corresponding to the field of view of
the telescopic s
...

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