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The accuracy of length measurement limited by unknown

temperature

Citation for published version (APA):

Koning, J. (1970). The accuracy of length measurement limited by unknown temperature. (TH Eindhoven. Afd. Werktuigbouwkunde, Laboratorium voor mechanische technologie en werkplaatstechniek : WT rapporten; Vol. WT0239). Technische Hogeschool Eindhoven.

Document status and date: Published: 01/01/1970 Document Version:

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. .

,

THE ACCORACY' OF LENGTH ME'ASUREMENT

LIMITED

BY UN.KNJWN

TEMPERATURE •

by

J. Koning

Eindhoven, University of Technology, the Netherlands

Paper to be presented to the General. Assembly of the C.I.R.P.~ Po'Plno~ 19'10

(3)

A short discussion on the definition of tenperature and its

consequence for accurate length rreasurement.

Dn vorliegenden Beitrag wird der Tenperatw:begriff hinsichtlich

seiner Konsequenzen

rUr

genaue, LangenI'OOSsung kurz

erOrtert.

I . .

I .

Une discussion de 1a conception de teIrperature et ses oonsequences

i

(4)

Although the subject of this note may be well knCM.rl, the author should like to enlarge on it, because of its technical iIr{x:>rtance in rretrology.

The knCMledge of tenperature is essential to precise length treasurement At present, the best accuracy realised on industrial standards may be about 10-7 • If it is acceptable that half of this value is caused

by inaccuracy of tercperature rreasurement, terrperature must be knOtm to 5 rnK or better !Sf) •

. ' - 0

As a rule length rreasurenents are stated to be 'corrected to 20 C, but often it is not made clear what is rreant by 20oC.

Ten:parature is defined in physics by thenrodynarnic relations I together

with the value 273.16 K == 0.01

°c

for the tenperature of the tr:j..ple ];X)int of water. In' practice I hCMever I tenperature is treasured follCMing

the routine of the international practical terrperature scale (IPl'S).

Therefore it can be taken for granted that 200C nonnally stands for

20°C IPl'S. .

It is well k.n.cMn that the IPl'S in the region of 20°C is defined by interpolation between certain fixp:>ints by rreans of a platinum resistance therm.::m:rte:t;:', using a quadratio equation.

Recent rreasurerrents (1) have shown this scale to differ 8 rnK fran true ('¢enrodynamic) tenperature at 20°C.' The latest version of the IPl'S (IPl'S

19~8)

(2)

takeSthisdifferencein~'account.ThiS

means,

hCWever,

'that-'

there exists a difference of 10-7 in length measurements performed before

filld

after october 1968.

IPl'S cannot be nore than an approximation to true (therm:x:1ynam:i.c)

tenperature. The accuracy of the fixp:>ints, as stated (ref. 2, table 7), limits the accuracy of this approximation at 20°C to 2 mK.

It seems advisable to state explicitely that 20°C is neant _ to be true tenperature. IPl'S 1's used, of course, as a practical apprOxmation.

In that case the symbol, t68 is to be used.

~)

note: Kelvin for a ten:p'=>...raturedifference of 1 degree Celsius == 1 (Iegree Kelvin; thus 5 mK == 0.005 degree).

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'lhe properties of platinum resistance thenn:.::m=ters being well knCMIl, it seems advisable to use such thenrareters for the rrore

.

exacting work. TheJ::1lO1lE!ters are available with dimensions dc::1tm

to 2 nm of diarreter and 50 nm of length and maybe smaller. If such a thenrorreter, having Ro == 100 0, is supplied with a current of 2,5 mA., a potential difference of 1 mV per K results, which can be neasured and· registrated oonvenently.

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(2)

PrestonjThanas, H •. and C.G.M. Kirby

Metrologia

! -

30 - (1967). Metrologia 5 - 36 - (1969).

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