ISO 5-1-2009 Photography and graphic technology - Density measurements - Part 1 Geometry and functional notation《摄影和印刷技术 密度测量 第1部分 几何和功能符》.pdf

《ISO 5-1-2009 Photography and graphic technology - Density measurements - Part 1 Geometry and functional notation《摄影和印刷技术 密度测量 第1部分 几何和功能符》.pdf》由会员分享，可在线阅读，更多相关《ISO 5-1-2009 Photography and graphic technology - Density measurements - Part 1 Geometry and functional notation《摄影和印刷技术 密度测量 第1部分 几何和功能符》.pdf（24页珍藏版）》请在麦多课文档分享上搜索。

1、 Reference number ISO 5-1:2009(E) ISO 2009INTERNATIONAL STANDARD ISO 5-1 Second edition 2009-12-01 Photography and graphic technology Density measurements Part 1: Geometry and functional notation Photographie et technologie graphique Mesurages de la densit Partie 1: Gomtrie et notation fonctionnelle

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5、ven below. COPYRIGHT PROTECTED DOCUMENT ISO 2009 All rights reserved. Unless otherwise specified, no part of this publication may be reproduced or utilized in any form or by any means, electronic or mechanical, including photocopying and microfilm, without permission in writing from either ISO at th

6、e address below or ISOs member body in the country of the requester. ISO copyright office Case postale 56 CH-1211 Geneva 20 Tel. + 41 22 749 01 11 Fax + 41 22 749 09 47 E-mail copyrightiso.org Web www.iso.org Published in Switzerland ii ISO 2009 All rights reservedISO 5-1:2009(E) ISO 2009 All rights

7、 reserved iiiContents Page Foreword iv Introduction.v 1 Scope1 2 Normative references1 3 Terms and definitions .1 4 Equations .4 5 Instrument representation5 6 Coordinate system 6 7 Description of geometry .7 8 Functional notation .8 8.1 General .8 8.2 Geometric conditions8 8.3 Spectral conditions .

8、11 8.4 Examples of functional notation12 Annex A (informative) Terms and definitions used in other parts of ISO 5 13 Bibliography16 ISO 5-1:2009(E) iv ISO 2009 All rights reservedForeword ISO (the International Organization for Standardization) is a worldwide federation of national standards bodies

9、(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, g

10、overnmental 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. International Standards are drafted in accordance with the rules given in the ISO/I

11、EC Directives, Part 2. The main task of technical committees is to prepare International Standards. Draft International Standards adopted by the technical committees are circulated to the member bodies for voting. Publication as an International Standard requires approval by at least 75 % of the mem

12、ber bodies casting a vote. 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. ISO 5-1 was prepared by ISO/TC 42, Photography, and ISO/TC 130, Graphic te

13、chnology, in a Joint Working Group. This second edition cancels and replaces the first edition (ISO 5-1:1984), which has been technically revised. In the course of this technical revision, all parts of ISO 5 have been reviewed together, and the terminology, nomenclature and technical requirements ha

14、ve been made consistent across all parts. ISO 5 consists of the following parts, under the general title Photography and graphic technology Density measurements: Part 1: Geometry and functional notation Part 2: Geometric conditions for transmittance density Part 3: Spectral conditions Part 4: Geomet

15、ric conditions for reflection density ISO 5-1:2009(E) ISO 2009 All rights reserved vIntroduction The measurement of the transmission and reflection characteristics of objects is essential to the science of photography and graphic arts. When light, or other radiant energy, is incident upon an object,

16、 it is either absorbed or propagated. Propagation can involve reflection, transmission, refraction, diffraction, scattering, fluorescence, and polarization. The propagated light is distributed in various directions about the object. In most practical applications it is neither necessary nor desirabl

17、e to consider the light distributed in every direction, but only that which leaves the object in the direction for which there is response by a receiver, such as the eye. The object modulates the flow of radiant energy from the illuminator to the receiver. The time rate of flow of radiant energy is

18、called radiant flux, or simply flux. This part of ISO 5 provides methods to describe the measurements of the flux modulation in any system. To specify such a system accurately, geometric characteristics of the system, the spectral distribution of the flux incident on the object to be measured, and t

19、he spectral responsivity of the receiver need to be given. If the reflection characteristics of the illuminator or receiver affect the measurement, as they do in transmission measurements by the opal glass method, they need to be specified. The area under consideration is defined by a sampling apert

20、ure, the dimensions of which can be important in some applications and need to be specified if the object has appreciable non-uniformity. If the measurement is to quantify the way the object would modulate flux in a given practical application, such as viewing or contact printing, the geometric and

21、spectral conditions of measurement need to simulate those conditions in the practical application. Modulation is measured and expressed as a dimensionless ratio of fluxes; that is, the flux propagated in the direction of the receiver and that part of the spectrum of interest divided by some referenc

22、e flux. The reference flux can be the incident flux or the flux propagated through the system when the object is replaced by an ideal object. For some purposes, a logarithmically scaled measure of modulation is more useful than the measured arithmetic ratio. In such cases, it is customary to use opt

23、ical density defined as the negative logarithm to base 10 of the ratio. Most geometric arrangements used in photographic and graphic arts optical systems can be conveniently and adequately described in terms of uniform rays of flux bounded by right circular cones. A point on the object is often illu

24、minated by such a conic distribution, and the geometric form of the pencil of rays reaching the receiver is generally conic. The pupil of the eye, for example, subtends a conic solid angle at an object point. In projection systems, the projection lens subtends a conic solid angle at the specimen poi

25、nt. This part of ISO 5 specifies a conic distribution by the half-angle of the cone and the direction of its axis. A working knowledge of radiometry is generally required to obtain primary standard measurements of transmittance and reflectance. In good radiometric practice, for example, the effects

26、of stray light are minimized by the use of appropriate baffles and proper blackening of certain surfaces. Because the principles and practice of radiometry are well known and are fully described in the Handbook of Applied Photometry 10 , it is considered unnecessary to provide a detailed specificati

27、on of radiometric procedures in this part of ISO 5. INTERNATIONAL STANDARD ISO 5-1:2009(E) ISO 2009 All rights reserved 1Photography and graphic technology Density measurements Part 1: Geometry and functional notation 1 Scope This part of ISO 5 establishes terms, symbols, functional notations and a

28、coordinate system to describe geometric and spectral conditions for the measurement of the degree to which a specimen modulates radiant flux for applications in photography, graphic technology, and radiometry. This part of ISO 5 primarily provides a system for describing methods of measuring or spec

29、ifying the transmission and reflection properties of photographic and graphic arts materials. The geometric and spectral conditions associated with such measurement are specified in ISO 5-2, ISO 5-3 and ISO 5-4. 2 Normative references The following referenced documents are indispensable for the appl

30、ication 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 5-2, Photography and graphic technology Density measurements Part 2: Geometric conditions for transmittance de

31、nsity ISO 5-3, Photography and graphic technology Density measurements Part 3: Spectral conditions ISO 5-4, Photography and graphic technology Density measurements Part 4: Geometric conditions for reflection density 3 Terms and definitions For the purposes of this document, the following terms and d

32、efinitions apply 1) . 3.1 absolute reference reflected flux rAradiant flux that would be reflected by a perfect reflecting diffuser 1) For the convenience of the user, Annex A lists those terms and definitions used in other parts of ISO 5 that are not used in this part of ISO 5. ISO 5-1:2009(E) 2 IS

33、O 2009 All rights reserved3.2 absolute reference transmitted flux tAradiant flux that would be transmitted by a perfect transmitting diffuser 3.3 anormal angle angle between the normal of the reference plane and a direction NOTE Adapted from ASTM E1767. 3.4 azimuthal angle angle between the x-axis o

34、f the reference plane and the projection of a direction onto the reference plane NOTE Adapted from ASTM E284. 3.5 cone half-angle angle between the central axis and the edge of the pupil with the apex at the centre of the sampling aperture 3.6 efflux radiant flux collected by the receiver from the r

35、eference plane NOTE Adapted from ASTM E1767. 3.7 illuminator axis central axis of the illuminator, usually the optical axis 3.8 illuminator region intersection of the illuminator beam with the reference plane 3.9 incident flux iradiant flux incident upon the sampling aperture 3.10 influx radiant flu

36、x projected by the illuminator onto the reference plane NOTE Adapted from ASTM E1767. 3.11 influx spectrum S spectral distribution of the radiometric quantity, such as radiance, irradiance or radiant flux, incident upon the sampling aperture NOTE This is a function of the source and optics used for

37、the illumination. ISO 5-1:2009(E) ISO 2009 All rights reserved 33.12 ISO 5 standard density density value obtained using an instrument conforming to one of the geometries specified in ISO 5-2 or ISO 5-4, and one of the spectral definitions in ISO 5-3 3.13 receiver axis central axis of the receiver,

38、usually the optical axis 3.14 receiver region intersection of the receiver beam with the reference plane 3.15 reflectance ratio of the reflected flux to the incident flux under specified geometrical and spectral conditions of measurement NOTE Adapted from ASTM E284. 3.16 reflectance density D negati

39、ve logarithm to the base 10 of the reflectance 3.17 reflectance factor R ratio of the reflected flux to the absolute reference reflected flux under the same geometrical and spectral conditions of measurement 3.18 reflected flux rradiant flux that emerges from the specimen surface on which the incide

40、nt flux falls 3.19 reflection density D Rnegative logarithm to the base 10 of the reflectance factor NOTE The International Commission on Illumination (CIE) designates the measurement referred to as “reflection density” in ISO 5 as “reflectance factor density”. (See IEC 60050-845:1987 CIE 17.4:1987.

41、) 3.20 spectral responsivity s output signal of a receiver per unit input of radiant flux as a function of wavelength NOTE Adapted from ASTM E284. 3.21 transmission density D Tnegative logarithm to the base 10 of the transmittance factor ISO 5-1:2009(E) 4 ISO 2009 All rights reserved3.22 transmittan

42、ce ratio of the transmitted flux to the incident flux under specified geometrical and spectral conditions of measurement NOTE 1 In practical instruments for transmittance measurements, the incident flux is defined by the combination of all of the components that are placed before the reference plane

43、 (influx), so the incident flux is provided by the surface of the opal diffuser for diffuse transmittance and by the film gate for projection density. NOTE 2 Adapted from ASTM E284. 3.23 transmittance density D negative logarithm to the base 10 of the transmittance NOTE The subscript is the lower ca

44、se Greek letter tau. 3.24 transmittance factor T ratio of the transmitted flux to the absolute reference transmitted flux under the same geometrical and spectral conditions of measurement NOTE Adapted from ASTM E284. 3.25 transmitted flux tradiant flux that passes through the specimen and emerges fr

45、om a surface other than that on which the incident flux falls 4 Equations The terms and equations applicable to density measurements are given in Table 1. Table 1 Terms and equations for density measurements Term Equation Term Equation Transmittance t i = Transmittance density 10 log D = Reflectance

46、 r i = Reflectance density 10 log D = Transmittance factor t tA T = Transmission density 10 log T D T = Reflectance factor r rA R = Reflection density 10 log R D R = ISO 5-1:2009(E) ISO 2009 All rights reserved 55 Instrument representation Every instrument used to perform optical density measurement

47、s of a specimen typically has three components: an illuminator to project radiant flux onto the specimen, a reference plane at which the specimen is placed, and a receiver to measure the radiant flux from the specimen. These components are shown schematically in Figure 1 for a general instrument. Th

48、e illuminator consists of a source for providing radiant flux, and a director, which directs the radiant flux from the source onto the reference plane. Likewise, the receiver consists of a collector, which guides the radiant flux from the reference plane to the detector, which is a device that conve

49、rts radiant flux into a measurable signal. Examples of sources are incandescent and arc lamps, while examples of detectors are photodiodes and photomultiplier tubes. The central axes, marginal rays, and chief rays of the illuminator and receiver are also shown in Figure 1 as dashed, thin, and thick lines, respectively. The illuminator and receiver are optical systems with aperture and field stops. These stops determine the illuminator and receiver