9
ISO 3105-1976 (E) ANNEX8 SUSPENDED-LF:VEL VISCOMETERS B.3.3.2 Charge the BS/IP/SL. BS/IP/SL(SI. BS/IP!MSL. and F itzSimons viscometer~ through tube L with sufficient sample to fill bulb A, butnot bulb B. The viscometer may be mounted verticatly in the constant.temperature bath either prior to or following charging of the sampte into the viscometer. B.1 GENERAL The suspended-level viscometers Include the BS/IP/SL. BS/IP/SL(S). BS/IP/MSL. Ubbelohde. FitzSimons. Atlantic. Cannon-Ubbelohde. and Cannon-Ubbelohde semi-mlcro designs. The distinctive feature of suspended-level viscometers às that the liquid is suspended in the capillary which it fills completely. This suspension ensures a uniform driving head of liquid independent of the quantity of sample charged into the viscometer. making the viscometer constant independent of temperature. By making the diameter of the lower meniscus approximately equal to the average diameter of the upper meniscus. the surface tensàon correction is greatly reduced. Suspended-level viscometers are used for the measurement of the kinematic viscosities of transparent. Newtonian liquids up to 100000 mm2ís. 8.3.3.3 Permanently mount lhe Atlantic viscometer in lhe constant.temperature bath wlth lhe enlargement S resting on lhe top-split collar, and the lower end of capillary tube R, 25 mm from lhe bottom of lhe bath. Pour lhe sample into a clean 50 ml beaker. Charge lhe viscometer by positioning lhe beaker and sample under tube L so that it will be immersed in lhe sample. Slowly apply vacuum to tube N by turning the three-way stopcock O to vacuum. Draw lhe sample into the viscometer filling capillary R, timing bulb C, and partially filling upper bulb D. Glose stopcock O, holding the sample in the viscometer. If only a small sample is available, a short length of rubber-tipped glass tubing can be placed in the beaker with lhe rubber against the bottom of capillary tube R, and lhe sample drawn up asabove. 8.2 APPARATUS For the suspended-level viscometers, detailed dra\"!ings. size designations, nominal viscometer constants, kinematic viscosity range, capillary diameter and bulb volumes for each visco meter are shown in figures 8 to 15. 8.3.4 Allow the viscometer to remaln in the constant-temperature bath a sufficient time to ensure that the sample reaches temperature equilibrium (for liquids of low kinematic viscosity, 10 min at 40 °C, 15 min at 100 °C, or 20 min at 135 °C; highly viscous liquids may require double this time). 8.3 OPERATING INSTRUCTIONS 8.3.1 A standard operating procedure, applicable to ali glass capillary kinematic viscometers, is contained in ISO 3104. Operating instructions for the suspended-level types are outlined in 8.3.2 to B.3.8 wlth emphasis on procedures that are specific to this group of viscometers. B.3.5 Except for the Atlõntic viscometer which already has the sample in position, close tube M with the finger and use vacuum (or pressure, if the sample contains volatile constitutes) to draw the sample slowly through bulb C to about 8 mm above the upper timing mark E. Release the vacuum from tube N and immediately place a finger from tube M to tube N holding the meniscus above timing mark E until the lower meniscus hõs dropped below the end of capillary R in bulb B. Release the finger and allow the sample to flow by gravity. 8.3.2 Select a clean, dry calibrated viscometer whlch wlll give a flow time greater than 200 s or the minimum shown in the table of dimensions, whichever is the greater. 8.3.3 Charge the viscometer in the manner dictated by the design of the instrumento this operation being in conformity with that employed when the instrument was calibrated. If the sample is thought to contain fibres or solid particles. filter through a 75 .um screen during charging. 8.3.6 Measure to the nearest 0,2 s the time requíred for lhe leading edge of the meniscus to pass from timing mark E to timing mark F. If the flow time is less than 200 s. select a smaller capillary viscometer and repeat steps 8.3.3 to 8.3.6. 8.3.3.1 Charge the Ubbelohde and Cannon-Ubbelohde viscometers by tilting the instrument about 30" from the vertical and pouring sufficient sample through tube L into bulb A so that when the viscometer is returned to the vertical the meniscus is between filling marks G and H, and tube P completely fills without entrapping air. Mount the viscometer in the constant-temperature bath. keeping tube L vertical. To facilitate charging very viscou.. liquids, the viscometer may be inverted with tube L placed in the sample. Apply vacuum to tube N, closlng tube M by a finger or rubber stopper; draw sufficient sample into tube L such that after wiping L clean and placing the viscometer in the constant.temperature bath, bulb A will fill as described Clbove. 8.3.7 Repeat steps 8.3.5 and 8.3.6. maklng a dupllcate measurement of flow time. I f the two measurements agree within 0,2 ~'o. use the average for calculating kinematic viscosity- B.3.8 Clean lhe viscometer thoroughly by several rlnslngs with an appropriate solvent complete/y miscible with lhe sample. followed by rinsinq with a completely volatil~ solvem. Dry lhe viscometer by passing a slow stream of filtered, dry air through lhe viscometer for 2 mino or umil lhe last trace of solvem is removed. 14

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Page 1: ISO 3105-1976 (E) - webpages.ciencias.ulisboa.pt

ISO 3105-1976 (E)

ANNEX8

SUSPENDED-LF:VEL VISCOMETERS

B.3.3.2 Charge the BS/IP/SL. BS/IP/SL(SI. BS/IP!MSL.and F itzSimons viscometer~ through tube L with sufficientsample to fill bulb A, butnot bulb B. The viscometer maybe mounted verticatly in the constant.temperature batheither prior to or following charging of the sampte into the

viscometer.

B.1 GENERAL

The suspended-level viscometers Include the BS/IP/SL.BS/IP/SL(S). BS/IP/MSL. Ubbelohde. FitzSimons. Atlantic.Cannon-Ubbelohde. and Cannon-Ubbelohde semi-mlcrodesigns. The distinctive feature of suspended-levelviscometers às that the liquid is suspended in the capillarywhich it fills completely. This suspension ensures a uniformdriving head of liquid independent of the quantity ofsample charged into the viscometer. making the viscometerconstant independent of temperature. By making thediameter of the lower meniscus approximately equal to theaverage diameter of the upper meniscus. the surface tensàoncorrection is greatly reduced. Suspended-level viscometersare used for the measurement of the kinematic viscosities oftransparent. Newtonian liquids up to 100000 mm2ís.

8.3.3.3 Permanently mount lhe Atlantic viscometer in lheconstant.temperature bath wlth lhe enlargement S restingon lhe top-split collar, and the lower end of capillarytube R, 25 mm from lhe bottom of lhe bath. Pour lhesample into a clean 50 ml beaker. Charge lhe viscometer bypositioning lhe beaker and sample under tube L so that itwill be immersed in lhe sample. Slowly apply vacuum totube N by turning the three-way stopcock O to vacuum.Draw lhe sample into the viscometer filling capillary R,timing bulb C, and partially filling upper bulb D. Glosestopcock O, holding the sample in the viscometer. If only asmall sample is available, a short length of rubber-tippedglass tubing can be placed in the beaker with lhe rubberagainst the bottom of capillary tube R, and lhe sample

drawn up as above.

8.2 APPARATUS

For the suspended-level viscometers, detailed dra\"!ings. sizedesignations, nominal viscometer constants, kinematicviscosity range, capillary diameter and bulb volumes for

each visco meter are shown in figures 8 to 15. 8.3.4 Allow the viscometer to remaln in theconstant-temperature bath a sufficient time to ensure thatthe sample reaches temperature equilibrium (for liquids oflow kinematic viscosity, 10 min at 40 °C, 15 min at 100 °C,or 20 min at 135 °C; highly viscous liquids may requiredouble this time).

8.3 OPERATING INSTRUCTIONS

8.3.1 A standard operating procedure, applicable to aliglass capillary kinematic viscometers, is contained in

ISO 3104. Operating instructions for the suspended-leveltypes are outlined in 8.3.2 to B.3.8 wlth emphasis onprocedures that are specific to this group of viscometers.

B.3.5 Except for the Atlõntic viscometer which alreadyhas the sample in position, close tube M with the finger anduse vacuum (or pressure, if the sample contains volatileconstitutes) to draw the sample slowly through bulb C toabout 8 mm above the upper timing mark E. Release thevacuum from tube N and immediately place a finger fromtube M to tube N holding the meniscus above timingmark E until the lower meniscus hõs dropped below the endof capillary R in bulb B. Release the finger and allow the

sample to flow by gravity.

8.3.2 Select a clean, dry calibrated viscometer whlch wlllgive a flow time greater than 200 s or the minimum shownin the table of dimensions, whichever is the greater.

8.3.3 Charge the viscometer in the manner dictated by the

design of the instrumento this operation being in conformitywith that employed when the instrument was calibrated. If

the sample is thought to contain fibres or solid particles.filter through a 75 .um screen during charging.

8.3.6 Measure to the nearest 0,2 s the time requíred forlhe leading edge of the meniscus to pass from timingmark E to timing mark F. If the flow time is less than200 s. select a smaller capillary viscometer and repeat steps

8.3.3 to 8.3.6.8.3.3.1 Charge the Ubbelohde and Cannon-Ubbelohdeviscometers by tilting the instrument about 30" from thevertical and pouring sufficient sample through tube L intobulb A so that when the viscometer is returned to thevertical the meniscus is between filling marks G and H, andtube P completely fills without entrapping air. Mount theviscometer in the constant-temperature bath. keepingtube L vertical. To facilitate charging very viscou.. liquids,the viscometer may be inverted with tube L placed in thesample. Apply vacuum to tube N, closlng tube M by afinger or rubber stopper; draw sufficient sample into tube Lsuch that after wiping L clean and placing the viscometer inthe constant.temperature bath, bulb A will fill as described

Clbove.

8.3.7 Repeat steps 8.3.5 and 8.3.6. maklng a dupllcatemeasurement of flow time. I f the two measurements agreewithin 0,2 ~'o. use the average for calculating kinematic

viscosity-

B.3.8 Clean lhe viscometer thoroughly by several rlnslngswith an appropriate solvent complete/y miscible with lhesample. followed by rinsinq with a completely volatil~solvem. Dry lhe viscometer by passing a slow stream offiltered, dry air through lhe viscometer for 2 mino or umil

lhe last trace of solvem is removed.

14

Page 2: ISO 3105-1976 (E) - webpages.ciencias.ulisboa.pt

ISO 3105-1976 (E)

Dimensions in millimetres

FIGURE 8 -BS/IP/SL viscometer

T ABLE 10- Oimensions and kinematic viscosity ranges

350 s minlmum flow time: 200 s mlnlmum flow time for ali othe,

15

Page 3: ISO 3105-1976 (E) - webpages.ciencias.ulisboa.pt

ISO 3105-1976 (E)

Dimensions in millimetre$

~

T ABLE 11 -Dimensions and kinematic viscosity ranges

1 320 s mlnlmum flow tIme;600 s minimum flow time;380 s minlmum flow tIme;200 s mlnlmum flow tIme for ali other slzes.

16

Page 4: ISO 3105-1976 (E) - webpages.ciencias.ulisboa.pt

ISO 3105-1976 (E)

Dimensions in mi11imetres

FIGURE 10 -BS/IP/MSL viscometer

I AtjLt: 1 ~ -Ulmenslons and klnematlc VISCOSlty ranges

LUU 5 mrnlmum IIOW tIme lor ali sIzes.

11

Page 5: ISO 3105-1976 (E) - webpages.ciencias.ulisboa.pt

18---ISO 3105-1976 (E)

16.5

~

Oimensions in mitlimetres

O-N

I/''"\

L -11

TAS L E 13 -Oimensions and kinematlc VISCOSlty ranges~

NomInalviscometer

constant

(mm2/sl/s

VolumebulbC

Inslde dlameterof tube P

Kinematic

\iiscosity range

Insíde díameterof tube R

Slze NO.

mm;t/s mm (t 2 %1

0.240.360.460.580.730.881.031.361.551.832,432.753.274.325.206.25

mllt !)~,

1,0

2.0

3.0

4,0

4,0

4,0

4,0

4,0

4,0

4,0

4.0

4,0

4,0

4,0

5,0

5.0

mm I~ ~,,\)I

6.06.06.06.06.06.06.06.06.06.06.06.57.08.08.5

10.0

uOC06

11C

16

2

2C

26

3

3C36

4

4C46

5

U,UUl-0,003

0,005

0,01

0,03

0,05

0,1

0.30,51.03.05,0

10

3050

100

0,3" to 1

0.6 to 3

1 t05

2 to 10

6 to 30

10 to 50

20 to 100

60 to 300

100 to 500

200 to 1 000

600 to 3 000

1 000 to 5 000

2 000 to 10 000

6000 to 30000

10000 to 50000

20000 to 100 000

300 s mlnlmUm tlOW tIme: ~uu s monlmum "OW (.me 'o' alI o{n", SIL"S

lH

Page 6: ISO 3105-1976 (E) - webpages.ciencias.ulisboa.pt

I:>U 31U5.1976 (tI

Ulmensions in mitlimetres

L

~III.

N-b

M-I

J7=-~

{ ,

~I (; l,;1.. "'2to

-

II

~II

II

I

,i

CSIn

Nr

D

/1

(- 'A -~O

~irur 'UI"rd"""~ ur,

lengths. see 3.2

VI'" "~pll,~ry I VVO I;~plllary

FIGURE 12 -FitzSimons visco meter

I,",OLC I q -ulmenSlons ano Klnematlc VISCOSlty ranges

,~~. "..",.,.u,.. .,~.. .',.,~ .~. U', .,~~..

1:7

Page 7: ISO 3105-1976 (E) - webpages.ciencias.ulisboa.pt

ISO 3105-1976 (E)

Dimensions in millimetres

T ABLE 15 -Dimensions and kinematic viscosity ranges

2505 mlnimum flow time; 2005 minimum flow time for ali othel

20

Page 8: ISO 3105-1976 (E) - webpages.ciencias.ulisboa.pt

ISO 3105-1976 (E), 22 ,:---,

I

l O NÓ-Ia..-,

MO--

Dimensions in millimetres

FIGURE 14 -Cannon-Ubbelohde (A) and Cannon-Ubbelohde dilution (81 viscometer

T ABLE 16 -Oimensions õnd kinematic viscosity ranges

21

Page 9: ISO 3105-1976 (E) - webpages.ciencias.ulisboa.pt

1503105-1976 (E)

Dimensions in millimetres

22~

LO:~

, ,

~FIGURE 15 -Cannon-Ubbelohde semi-micro viscometer

T ABLE 17 -Oimensions and kinematic viscosity ranges

200 s mlnlmUm flOW tIme tor ali 5lzes.

22