FprEN ISO 80000-11
(Main)This document gives names, symbols and definitions for characteristic numbers used in the description of transport and transfer phenomena.
Größen und Einheiten - Teil 11: Kenngrößen der Dimension Zahl (ISO 80000-11:2019)
Grandeurs et unités - Partie 11: Nombres caractéristiques (ISO 80000-11:2019)
Le présent document donne noms, les symboles et les définitions des nombres caractéristiques utilisés dans la description des phénomènes de transfert.
Veličine in enote - 11. del: Značilna števila (ISO 80000-11:2019)
General Information
RELATIONS
Standards Content (sample)
SLOVENSKI STANDARD
oSIST prEN ISO 80000-11:2017
01-marec-2017
9HOLþLQHLQHQRWHGHO=QDþLOQDãWHYLOD,62',6
Quantities and units - Part 11: Characteristic numbers (ISO/DIS 80000-11:2017)
Größen und Einheiten - Teil 11: Kenngrößen der Dimension Zahl (ISO/DIS 80000-
11:2017)
Grandeurs et unités - Partie 11: Nombres caractéristiques (ISO/DIS 80000-11:2017)
Ta slovenski standard je istoveten z: prEN ISO 80000-11ICS:
01.060 9HOLþLQHLQHQRWH Quantities and units
oSIST prEN ISO 80000-11:2017 en,fr,de
2003-01.Slovenski inštitut za standardizacijo. Razmnoževanje celote ali delov tega standarda ni dovoljeno.
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oSIST prEN ISO 80000-11:2017
DRAFT INTERNATIONAL STANDARD
ISO/DIS 80000-11
ISO/TC 12 Secretariat: SIS
Voting begins on: Voting terminates on:
2017-01-03 2017-03-27
Quantities and units —
Part 11:
Characteristic numbers
Grandeurs et unités —
Partie 11: Nombres caractéristiques
ICS: 01.060
This document is circulated as received from the committee secretariat.
THIS DOCUMENT IS A DRAFT CIRCULATED
This draft is submitted to a parallel vote in ISO and in IEC.
FOR COMMENT AND APPROVAL. IT IS
THEREFORE SUBJECT TO CHANGE AND MAY
NOT BE REFERRED TO AS AN INTERNATIONAL
STANDARD UNTIL PUBLISHED AS SUCH.
IN ADDITION TO THEIR EVALUATION AS
ISO/CEN PARALLEL PROCESSING
BEING ACCEPTABLE FOR INDUSTRIAL,
TECHNOLOGICAL, COMMERCIAL AND
USER PURPOSES, DRAFT INTERNATIONAL
STANDARDS MAY ON OCCASION HAVE TO
BE CONSIDERED IN THE LIGHT OF THEIR
POTENTIAL TO BECOME STANDARDS TO
WHICH REFERENCE MAY BE MADE IN
Reference number
NATIONAL REGULATIONS.
ISO/DIS 80000-11:2017(E)
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 SUPPORTING DOCUMENTATION. ISO 2017
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oSIST prEN ISO 80000-11:2017
ISO/DIS 80000-11:2017(E)
COPYRIGHT PROTECTED DOCUMENT
© ISO 2017, Published in Switzerland
All rights reserved. Unless otherwise specified, 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
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Tel. +41 22 749 01 11
Fax +41 22 749 09 47
copyright@iso.org
www.iso.org
ii © ISO 2017 – All rights reserved
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oSIST prEN ISO 80000-11:2017
ISO/DIS 80000-11:2017(E)
Contents Page
Foreword ................................................................................................................................................................................... iv
1 Scope ............................................................................................................................................................................. 1
2 Normative references ............................................................................................................................................. 1
3 Names, symbols, and definitions ........................................................................................................................ 1
4 Momentum transfer................................................................................................................................................. 2
5 Transfer of heat...................................................................................................................................................... 15
6 Transport of matter in a binary mixture ...................................................................................................... 22
7 Constants of matter............................................................................................................................................... 29
8 Magnetohydrodynamics ..................................................................................................................................... 31
9 Miscellaneous ......................................................................................................................................................... 38
Bibliography........................................................................................................................................................................... 39
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oSIST prEN ISO 80000-11:2017
ISO/DIS 80000-11:2017(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 on 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 the following URL: www.iso.org/iso/foreword.html.
The committee responsible for this document is ISO/TC 12, Quantities and units.This second edition cancels and replaces the first edition (ISO 80000-11:2008).
ISO 80000 consists of the following parts, under the general title Quantities and units:
Part 1: General Part 2: Mathematics
Part 3: Space and time
Part 4: Mechanics
Part 5: Thermodynamics
Part 7: Light and Radiation
Part 8: Acoustics
Part 9: Physical chemistry and molecular physics
Part 10: Atomic and nuclear physics
Part 11: Characteristic numbers
iv © ISO 2017 – All rights reserved
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oSIST prEN ISO 80000-11:2017
ISO/DIS 80000-11:2017(E)
Part 12: Condensed matter physics
IEC 80000 consists of the following parts (in collaboration with IEC/TC 25), under the general title Quantities
and units: Part 6: Electromagnetism
Part 13: Information science and technology
Part 14: Telebiometrics related to human physiology
© ISO 2017 – All rights reserved v
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oSIST prEN ISO 80000-11:2017
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oSIST prEN ISO 80000-11:2017
DRAFT INTERNATIONAL STANDARD ISO/DIS 80000-11:2017(E)
Quantities and units — Part 11: Characteristic numbers
1 Scope
ISO 80000-11 gives the names, symbols and definitions for characteristic numbers used in the description of
transport and transfer phenomena.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 80000-3:2006, Quantities and units — Part 3: Space and timeISO 80000-4:2006, Quantities and units — Part 4: Mechanics
ISO 80000-5:2007, Quantities and units — Part 5: Thermodynamics
IEC 80000-6:2008, Quantities and units — Part 6: Electromagnetism
ISO 80000-8:2007, Quantities and units — Part 8: Acoustics
ISO 80000-9:2009, Quantities and units — Part 9: Physical chemistry and molecular physics
ISO 80000-9:2009, Quantities and units — Part 12: Condensed matter physics3 Names, symbols, and definitions
The names, symbols, and definitions for characteristic numbers are given on the following pages.
Characteristic numbers are physical quantities of dimension number 1, although commonly and falsely
called dimensionless quantities. They are used in the studies of natural and technical processes, and [may]
present information about the behaviour of the process, or reveal similarities between different processes.
Characteristic numbers often are described as ratios of forces; in some cases however they are ratios of
energy or work, although noted as forces in the literature; sometimes it is the ratio of characteristic times.
Characteristic numbers may be defined by the same equation, but carry different names if they are
concerned with different kinds of processes.Characteristic numbers may be expressed as products or fractions of other characteristic numbers if these
are valid for the same kind of process. So the following tables are arranged according to some groups of
processes.As the amount of characteristic numbers is tremendous, and their use in technology and science is not
uniform, only a small amount of them is given here. The choice largely was depending of their common use.
Besides there was made a restriction on the kind of processes, which are displayed by the section headings.
Nevertheless several characteristic numbers are found in different representations of the same physical
information, e.g. multiplied by a numerical factor, as the square, the square root, or the inverse of other
representation. Only one of these have been chosen, the other ones declared as deprecated or mentioned in
the remarks column.© ISO 2017 – All rights reserved
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oSIST prEN ISO 80000-11:2017
DRAFT INTERNATIONAL STANDARD ISO/DIS 80000-11:2017(E)
4 Momentum transfer
The transfer of momentum (ISO 80000-4:2006, item 4-8) basically occurs during a collision of 2 bodies, and is governed by the law of momentum conservation. Energy
dissipation may occur. In a more generalized meaning momentum transfer occurs during the interaction of 2 subsystems moving with velocity 𝑣 relative to each other.
Typically one of the subsystems is solid and possibly rigid, with a characteristic length, which may be a length, width, radi us, etc. of a solid object, often the effective length is
given by the ratio of a body’s volume to the area of its surface.The other subsystem is a fluid, in general liquid or gaseous, with the following properties amongst others:
— mass density 𝜌 (ISO 80000-4:2006, item 4-2);— dynamic viscosity 𝜂 (ISO 80000-4:2006, item 4-23);
— kinematic viscosity 𝜈 = 𝜂 𝜌 (ISO 80000-4:2006, item 4-24), or
— pressure drop 𝛥𝑝 (ISO 80000-4:2006, item 4-15.1).
The field of science is mainly fluid dynamics (mechanics). Characteristic numbers of this kind allow the comparison of objects of different sizes. It also may give some
estimation about the change of laminar flow to turbulent flow.No. Name Symbol Definition Remarks
11-4.1 Reynolds ratio of inertial forces to viscous forces in a fluid flow
The value of the Reynolds number gives an estimate on
𝜌 𝑣 𝑙 𝑣 𝑙
number
(11-4.1)
the flow state: laminar flow or turbulent flow.
= = ; where
𝜂 𝜈
𝜌 is mass density (ISO 80000-4:2006, item 4-2),
In rotating movement the speed 𝑣 is 𝑙 , where 𝑙 is the
𝑣 is speed (ISO 80000-3:2006, item 3-8.1),
distance from the rotation axis and 𝜔 is the angular
𝑙 is a characteristic length (ISO 80000-3:2006, item 3-1.1),
velocity.
𝜂 is dynamic viscosity (ISO 80000-4:2006, item 4-23), and
𝜈 is kinematic viscosity (ISO 80000-4:2006, item 4-24)
Euler number
11-4.2 relationship between pressure drop in a flow to kinetic energy per The Euler number is used to characterize losses in the
flow.(11-4.2) volume for flow of fluids in a pipe
𝛥𝑝
= ; where
2 A modification of the Euler number is considering the
𝜌 𝑣
© ISO 2017 – All rights reserved
𝐸𝑢
𝐸𝑢
𝑅𝑒
𝑅𝑒
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oSIST prEN ISO 80000-11:2017
ISO/DIS 80000-11:2017(E)
No. Name Symbol Definition Remarks
dimensions of the containment (pipe):
𝛥𝑝 is drop of pressure (ISO 80000-4:2006, item 4-15.1),
𝜌 is mass density (ISO 80000-4:2006, item 4-2), and
𝛥𝑝 𝑑 𝑑
𝐸 𝑢 = = ; where
𝑣 is speed (ISO 80000-3:2006, item 3-8.1) 2
𝑙 𝜌 𝑣 𝑙
𝑙 is length (ISO 80000-3:2006, item 3-1.1),and
𝑑 is inner diameter (ISO 80000-3:2006, item 3-1.7) of
the pipe.
The Froude number may be modified by buoyancy.
11-4.3 Froude ratio of a body’s inertial forces to its gravitational forces for flow of
𝐹𝑟number
(11-4.3) fluids
Sometimes the square and sometimes the inverse of the
𝐹𝑟 = ; where
Froude number as defined here is called the Froude
√𝑙 𝑔
number.
𝑣 is speed (ISO 80000-3:2006, item 3-8.1) of flow,
𝑙 is a characteristic length (ISO 80000-3:2006, item 3-1.1), and
The definition given here reflects that of the existing
𝑔 is acceleration of free fall (ISO 80000-3:2006, item 3-9.2)
standard. However In the majority of references the
squared value is used.
11-4.4 Grashof ratio of buoyancy forces due to thermal expansion which results in a Heating can occur near hot vertical walls, in pipes, or by a
number bluff body.(11-4.4) change of mass density to viscous forces for free convection due to
temperature differences
The characteristic length can be the vertical height of a
3 2
= 𝑙 𝑔 𝛼 𝛥𝑇 /𝜈 ; where
hot plate, the diameter of a pipe, or the effective length of
𝑙 is a characteristic length (ISO 80000-3:2006, item 3-1.1),
a body.
𝑔 is acceleration of free fall (ISO 80000-3:2006, item 3-9.2),
See also Rayleigh number (item 11-5.3).
𝛼 is thermal cubic expansion coefficient (ISO 80000-5:2007, item 5-
3.2),
𝛥𝑇 is difference of thermodynamic temperature 𝑇 (ISO 80000-5:2007,
item 5-1) between surface of the body and the fluid far away from
the body, and
𝜈 is kinematic viscosity (ISO 80000-4:2006, item 4-24)
11-4.5 Weber relationship of inertial forces compared to capillary forces for bubbles The characteristic length is commonly the diameter of
number bubbles or drops.(11-4.5) or drops in a fluid
= 𝜌 𝑣 𝑙 𝛾 ; where
The square root of the Weber number is called Rayleigh
𝜌 is mass density (ISO 80000-4:2006, item 4-2),
number.
𝑣 is speed (ISO 80000-3:2006, item 3-8.1),
© ISO 2017 – All rights reserved
𝑊𝑒
𝑊𝑒
𝐺𝑟
𝐺𝑟
𝐸𝑢
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oSIST prEN ISO 80000-11:2017
ISO/DIS 80000-11:2017(E)
No. Name Symbol Definition Remarks
𝑙 is a characteristic length (ISO 80000-3:2006, item 3-1.1), and Sometimes the square root of the Weber number as
𝛾 is surface tension (ISO 80000-4:2006, item 4-25) defined here is called the Weber number. That definition
is deprecated.Mach number
11-4.6 ratio of the speed of flow to the speed of sound The Mach number represents the relationship of inertial
forces compared to compression forces.(11-4.6) = 𝑣 𝑐 ; where
𝑣 is speed (ISO 80000-3:2006, item 3-8.1) of the body and
For an ideal gas
𝑐 is speed of sound (ISO 80000-8:2007, item 8-14.1) of the fluid
𝑝 𝑅𝑇
𝑐 = 𝛾 = √𝛾 = √𝛾 ; where 𝛾 is ratio of the specific
𝜌 𝑀 𝑚
heat capacities (ISO 80000-5:2007, item 5-17.1).
11-4.7 Knudsen ratio of mean free path of a particle to characteristic length for gas flow The Knudsen number is a measure to estimate whether
(11-4.7) number = 𝜆 𝑙 ; where the gas in flow behaves like a continuum.𝜆 is mean free path (ISO 80000-9:2009, item 9-44), and
The length 𝑙 can be a characteristic size of the gas flow
𝑙 is length (ISO 80000-3:2006, item 3-1.1)
region like a pipe diameter.
11-4.8 Strouhal ratio of characteristic frequency to characteristic speed for unsteady The characteristic length 𝑙 can be the diameter of an
𝑆𝑟 , 𝑆 ℎ(11-4.8) number flow with periodic behaviour obstacle in the flow which can cause vortex shedding, or
the length of it.𝑆𝑟 = 𝑓 𝑙 /𝑣 ; where
(Thomson
𝑓 is frequency (ISO 80000-3:2006, item 3-15.1) of vortex shedding,
number)
𝑙 is a characteristic length (ISO 80000-3:2006, item 3-1.1), and
𝑣 is speed (ISO 80000-3:2006, item 3-8.1) of flow
11-4.9 drag ratio of the effective drag force to inertial forces for a body moving in a The drag coefficient is strongly dependant on the shape of
coefficient the body.- fluid
2𝐹
𝑐 = ; where:
𝜌 𝑣 𝐴
𝐹 is drag force (ISO 80000-4:2006, item 4-9.1) on the body,
𝜌 is mass density (ISO 80000-4:2006, item 4-2) of the fluid,
𝑣 is speed (ISO 80000-3:2006, item 3-8.1) of the body, and
𝐴 is the cross sectional area (ISO 80000-3:2006, item 3-3)
11-4.10 Bagnold ratio of drag force to gravitational force for a body moving in a fluid The characteristic length 𝑙 is the body’s volume divided by
𝐵𝑔© ISO 2017 – All rights reserved
𝐾𝑛
𝐾𝑛
𝑘𝑇
𝑀𝑎
𝑀𝑎
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oSIST prEN ISO 80000-11:2017
ISO/DIS 80000-11:2017(E)
No. Name Symbol Definition Remarks
number 𝑐 𝜌 𝑣 its cross sectional area.
𝐵𝑔 =
𝑙 𝑔 𝜌
𝑐 is drag coefficient (item 11-4.9) on the body,
𝜌 is mass density (ISO 80000-4:2006, item 4-2), of fluid,
𝑣 is speed (ISO 80000-3:2006, item 3-8.1) of the body,
𝜌 is mass density (ISO 80000-4:2006, item 4-2), of the body,
𝑔 is acceleration of free fall (ISO 80000-3:2006, item 3-9.2), and
𝑙 is a characteristic length (ISO 80000-3:2006, item 3-1.1)
11-4.11 Bagnold ratio of drag force to viscous force in a fluid transporting solid particles
𝐵 𝑎- number 1 2
⁄( )
𝐵 𝑎 = √1 𝑓 − 1 ; where
solid 𝜂
particles>
𝜌 is mass density (ISO 80000-4:2006, item 4-2) of particles,
𝑑 is diameter (ISO 80000-3:2006, item 3-1.7) of particles,
𝛾 ̇ = 𝑣 /𝑑 is shear rate, time derivative of shear strain (ISO 80000-
4:2006, item 4-16.2),
𝜂 is dynamic viscosity (ISO 80000-4:2006, item 4-23) of fluid, and
𝑓 is volumic fraction of solid particles
lift coefficient The lift coefficient is dependent on the shape of the wing.
11-4.12 ratio of the lift force available from a wing at a given angle of attack to
𝑐 , 𝑐l A
- the inertial force for a wing shaped body moving in a fluid
2𝐹 𝐹
𝑙 𝑙
𝑐 = = ; where
𝑙 2
𝜌 𝑣 𝑆
𝐹 is lift force (ISO 80000-4:2006, item 4-9.1) on the wing,
𝜌 is mass density (ISO 80000-4:2006, item 4-2) of the fluid,
𝑣 is speed (ISO 80000-3:2006, item 3-8.1) of the body,
𝑞 = 𝜌 𝑣 /2 is dynamic pressure, and
𝑆 = 𝐴 cos𝛼 is effective area (ISO 80000-3:2006, item 3-3) when 𝛼 is the
angle of attack and A is area of the wing
11-4.13 thrust ratio of the effective thrust force available from a propeller to the The thrust coefficient is dependent on the shape of the
coefficient propeller.- inertial force in a fluid
2 4
⁄( )
𝑐 = 𝐹 𝜌 𝑛 𝑑 ; where
t T
𝐹 is thrust force (ISO 80000-4:2006, item 4-9.1) of the propeller;
© ISO 2017 – All rights reserved
𝑞𝑆
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oSIST prEN ISO 80000-11:2017
ISO/DIS 80000-11:2017(E)
No. Name Symbol Definition Remarks
𝑛 is rotational frequency (ISO 80000-3:2006, item 3-15.2),
𝑑 is tip diameter (ISO 80000-3:2006, item 3-1.7) of the propeller, and
𝜌 is mass density (ISO 80000-4:2006, item 4-2) of the fluid
11-4.14 Dean number ratio of centrifugal force to inertial force for flow of fluids in curved
- pipes2 𝑟
1⁄2
( )( )
= 𝑣 𝑑 𝜌 /𝜂 𝑑 /2𝑅 = ; where
𝜈 𝑅
𝑣 is (axial) speed (ISO 80000-3:2006, item 3-8.1),
𝑑 is diameter (ISO 80000-3:2006, item 3-1.7) of pipe,
𝜌 is mass density (ISO 80000-4:2006, item 4-2),
𝜂 is dynamic viscosity (ISO 80000-4:2006, item 4-23),
𝜈 is kinematic viscosity (ISO 80000-4:2006, item 4-24)
𝑟 = 𝑑 /2 is radius of pipe
𝑅 is the radius of curvature (ISO 80000-3:2006, item 3-1.13) of the
path of the pipe
Bejan number A similar number exists for heat transfer (item 11-5.9).
11-4.15 ratio of mechanical work to frictional energy loss in fluid dynamics in a
𝐵𝑒- pipe
2 2
Δ𝑝 𝑙 𝜌 Δ𝑝 𝑙
𝐵𝑒 = = ; where
𝜂 𝜈 𝜂
Δ𝑝 is drop of pressure (ISO 80000-4:2006, item 4-15.1) along a pipe,
𝑙 is length (ISO 80000-3:2006, item 3-1.1),
𝜂 is dynamic viscosity (ISO 80000-4:2006, item 4-23),
𝜌 is mass density (ISO 80000-4:2006, item 4-2), and
𝜈 is kinematic viscosity (ISO 80000-4:2006, item 4-24), momentum
diffusivity
The Lagrange number is also given by
11-4.16 Lagrange ratio of mechanical work to frictional energy loss in fluid dynamics in a
number- pipe
𝐿𝑎 = ⋅ ; where
𝑙 Δ𝑝
𝐿𝑔 = ; where
𝜂 𝑣
is the Reynolds number (item 11-4.1) and is the
𝑙 is length (ISO 80000-3:2006, item 3-1.1) of a pipe,
Euler number (item 11-4.2)
Δ𝑝 is drop of pressure (ISO 80000-4:2006, item 4-15.1) along a pipe,
𝜂 is dynamic viscosity (ISO 80000-4:2006, item 4-23), and
© ISO 2017 – All rights reserved
𝐸𝑢 𝑅𝑒
𝐸𝑢 𝑅𝑒
𝐷𝑛
𝑣𝑟
𝐷𝑛
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oSIST prEN ISO 80000-11:2017
ISO/DIS 80000-11:2017(E)
No. Name Symbol Definition Remarks
𝑣 is speed (ISO 80000-3:2006, item 3-8.1)
11-4.17 Bingham ratio of yield stress to viscous stress in a viscous material for flow of
𝐵𝑚 , 𝐵𝑛number;
- viscoplastic material in channels
𝜏 𝑑
𝐵𝑚 = ; where
plasticity
𝜂 𝑣
number
𝜏 is shear stress (ISO 80000-4:2006, item 4-15.3),
𝑑 is characteristic diameter (ISO 80000-3:2006, item 3-1.7), e.g.
effective channel width,
𝜂 is dynamic viscosity (ISO 80000-4:2006, item 4-23), and
𝑣 is speed (ISO 80000-3:2006, item 3-8.1)
11-4.18 Hedström ratio of yield stress to viscous stress of a viscous material at flow
- number limit.for visco-plastic material in channels at flow limit𝜏 𝑑 𝜌
= ; where
𝜏 is shear stress (ISO 80000-4:2006, item 4-15.3) at flow limit,
𝑑 is characteristic diameter (ISO 80000-3:2006, item 3-1.7), e.g.
effective channel width,
𝜌 is mass density (ISO 80000-4:2006, item 4-2), and
𝜂 is dynamic viscosity (ISO 80000-4:2006, item 4-23)
11-4.19 Bodenstein representation of the transfer of matter by convection in reactors with The Bodenstein number is also given by
𝐵𝑑number ∗
- respect to diffusion
𝐵𝑑 = = ⋅ 𝑆𝑐 ; where
𝐵𝑑 = 𝑣 𝑙 /𝐷 ; where
is Péclet number for mass transfer (11-6.2),
𝑣 is speed (ISO 80000-3:2006, item 3-8.1),
is Reynolds number (11-4.1), and
𝑙 is length (ISO 80000-3:2006, item 3-1.1) of reactor, and
⁄( ) ⁄
𝑆𝑐 = 𝜂 = 𝜈 𝐷 is Schmidt number (11-7.2).
𝐷 is diffusion coefficient (ISO 80000-9:2009, item 9-45)
11-4.20 Rossby ratio of inertial forces to Coriolis forces in the context of transfer of The Rossby number represents the effect of earth's
- number; matter for the flow of a rotating fluid rotation on flow in pipes, rivers, ocean currents,
⁄( )tornadoes, etc.
Kiebel = 𝑣 2 𝑙 𝜔 sin𝜙 ; where
number
𝑣 is speed (ISO 80000-3:2006, item 3-8.1) of motion,
The quantity 𝜔 sin𝜙 is called Coriolis frequency.
𝑙 is a characteristic length (ISO 80000-3:2006, item 3-1.1), the scale
of the phenomenon;
𝜔 is angular velocity (ISO 80000-3:2006, item 3-10) of earth's
© ISO 2017 – All rights reserved
𝑅𝑜
𝑅𝑜
𝜌𝐷
𝑅𝑒
𝑃𝑒
𝑅𝑒 𝑃𝑒
𝐻𝑒
𝐻𝑑 𝐻𝑒
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oSIST prEN ISO 80000-11:2017
ISO/DIS 80000-11:2017(E)
No. Name Symbol Definition Remarks
rotation, and
𝜙 is angel (ISO 80000-3:2006, item 3-5) of latitude
11-4.21 Ekman ratio of viscous forces to Coriolis forces in the context of transfer of In plasma physics the square root of this number is used.
- number matter for the flow of a rotating fluidThe Ekman number is also given by
⁄( )
= 𝜈 2 𝑙 𝜔 sin𝜙 ; where
= ; where
𝜈 is kinematic viscosity (ISO 80000-4:2006, item 4-24),
𝑅 𝑜 is the Rossby number and is the Reynolds number.
𝑙 is a characteristic length (ISO 80000-3:2006, item 3-1.1), the scale
of the phenomenon,
𝜔 is angular frequency 𝜔 (ISO 80000-3:2006, item 3-10) of earth’s
rotation, and
𝜙 is angel (ISO 80000-3:2006, item 3-5) of latitude
See also Deborah Number (item 11-7.8).
11-4.22 Elasticity ratio of relaxation time to diffusion time in viscoelastic flows
number- = 𝑡 𝜈 𝑟 ; where
𝑡 is relaxation time (ISO 80000-12:2009, item 12-33.1),
𝜈 is kinematic viscosity (ISO 80000-4:2006, item 4-24), and
𝑟 is radius (ISO 80000-3:2006, item 3-1.5) of pipe
𝑓 = 4𝑓 (Fanning friction factor)
11-4.23 Darcy friction representation of pressure loss in a pipe due to friction within the fluid
𝐷 𝑓- factor; in a laminar or turbulent flow of a fluid in a pipe
2Δ𝑝 𝑑
Moody
𝑓 = ; where
𝜌 𝑣 𝑙
friction factor
Δ𝑝 is drop of pressure (ISO 80000-4:2006, item 4-15.1) due to friction,
𝑙 is length (ISO 80000-3:2006, item 3-1.1) of the pipe,
𝑑 is diameter (ISO 80000-3:2006, item 3-1.7) of the pipe,
𝜌 is mass density (ISO 80000-4:2006, item 4-2) of the fluid, and
𝑣 is (average) speed (ISO 80000-3:2006, item 3-8.1) of the fluid in
the pipe
11-4.25 Fanning ratio of shear stress to dynamic pressure in the flow of a fluid in a The Fanning number describes the flow of fluids in a pipe
𝑓 𝑓- number , containment with friction at the walls represented by its shear stress.
2𝜏𝑓 = ; where
n Symbol 𝑓 can be used where no conflicts are possible.
𝜌 𝑣
𝜏 is shear stress (ISO 80000-4:2006, item 4-15.3) at the wall,
© ISO 2017 – All rights reserved
𝐸𝑙
𝐸𝑙
𝑅𝑒
𝑅𝑒 𝑅𝑜 𝐸𝑘
𝐸𝑘
𝐸𝑘
---------------------- Page: 16 ----------------------
oSIST prEN ISO 80000-11:2017
ISO/DIS 80000-11:2017(E)
No. Name Symbol Definition Remarks
𝜌 is mass density (ISO 80000-4:2006, item 4-2) of the fluid, and
𝑣 is speed (ISO 80000-3:2006, item 3-8.1) of the fluid in the pipe
11-4.26 Goertler characterization of the stability of laminar boundary layer flows in The Goertler parameter represents the ratio of centrifugal
effects to viscous effects.- parameter transfer of matter in a boundary layer on a curved surface
1⁄2
𝑣 𝑙 𝑙
𝑏 𝑏
( )
= ; where
𝜈 𝑟
𝑣 is speed (ISO 80000-3:2006, item 3-8.1) m/s
𝑙 is boundary layer thickness (ISO 80000-3:2006, item 3-1.4),
𝜈 is kinematic viscosity (ISO 80000-4:2006, item 4-24), and
𝑟 is radius of curvature (ISO 80000-3:2006, item 3-1.13)
𝑑𝑝
11-4.27 Hagen generalization of Grashof number (11.-4.4) for forced or free convection
For free thermal convection with = 𝜌 𝑔 𝛼 𝛥𝑇 the Hagen𝑑𝑥
- number in laminar flow
number then coincides with the Grashof number (11-4.4).
1 𝑑𝑝 𝑙
= − ; where
See also Poisseuille number (item 11-4.29).
𝜌 𝑑𝑥 𝜈
𝜌 is mass density (ISO 80000-4:2006, item 4-2) of fluid kg/m³,
𝑙 is a characteristic length (ISO 80000-3:2006, item 3-1.1),
𝜈 is kinematic viscosity (ISO 80000-4:2006, item 4-24), and
𝑑𝑝
is gradient of pressure (ISO 80000-4:2006, item 4-15.1)
𝑑𝑥
11-4.28 Laval number ratio of speed to the (critical) sound speed in the throat of the nozzle The Laval number is a specific kind of Mach number (item
𝐿𝑎11-4.6).
- ⁄ ( )⁄( )
𝐿𝑎 = 𝑣 √ 𝑅 𝑇 2𝛾 𝛾 + 1 ; where
𝑣 is speed (ISO 80000-3:2006, item 3-8.1),
𝛾 is ratio of the specific heat capacities (ISO 80000-5:2007, item 5-
17.1),
𝑇 thermodynamic temperature (ISO 80000-5:2007, item 5-1),
𝑅 = is specific gas constant; with
𝑅 = molar gas constant (ISO 80000-9:2009, item 9-42), and
𝑀 = molar mass (ISO 80000-9:2009, item 9-5)
𝑜𝑖𝑃 = 32 for laminar flow in a round pipe.
11-4.29 Poiseuille ratio of propulsive force by pressure to viscous force for a flow of fluids
𝑜𝑖𝑃- number in a pipe
See also Hagen number (item 11-4.27).
© ISO 2017 – All rights reserved
𝐻𝑔
𝐻𝑎 𝐻𝑔
𝐺𝑜
𝐺𝑜
---------------------- Page: 17 ----------------------
oSIST prEN ISO 80000-11:2017
ISO/DIS 80000-11:2017(E)
No. Name Symbol Definition Remarks
Δ𝑝 𝑑
𝑜𝑖𝑃 = − where
𝑙 𝜂 𝑣
Δ𝑝 is drop of pressure (ISO 80000-4:2006, item 4-15.1)
Pa = N/m² = kg/ms²
𝑙 is length (ISO 80000-3:2006, item 3-1.1),
𝑑 is diameter (ISO 80000-3:2006, item 3-1.7),
𝜂 is dynamic viscosity (ISO 80000-4: 2006, item 4-23), and
𝑣 is speed (ISO 80000-3:2006, item 3-8.1)
11-4.30 power ratio of power consumption by agitators due to drag (on agitator,
- number impeller) to rotational inertial power in fluids
3 5
⁄( )
= 𝑃 𝜌 𝑛 𝑑 ; where
𝑃 is active power (IEC 80000-6:2008, item 6-56) consumed by a
stirrer,
𝜌 is mass density (ISO 80000-4:2006, item 4-2) of fluid,
𝑛 is rotational frequency (ISO 80000-3:2006, item 3-15.2), and
𝑑 is diameter (ISO 80000-3:2006, item 3-1.7) of stirrer
11-4.31 Richardson ratio of potential energy to kinetic energy for a falling body In geophysics differences of these quantities are of
- number = 𝑔 ℎ 𝑣 ; where interest.𝑔 is acceleration of free fall (ISO 80000-3:2006, item 3-9.2),
ℎ is a representative height (ISO 80000-3:2006, item 3-1.3), and
𝑣 is a representative speed (ISO 80000-3:2006, item 3-8.1)
11-4.32 Reech ratio of a speed of an object submerged in water to water wave The Reech number can be u
...
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