Gemini 550S Evaluation Report

    Data issued: 12 February 1998

    Gemini 550s Evaluation Report

    AN EVALUATION REPORT OF THE GEMINI 550S (SERIAL NUMBER 550/1) METAL BLOCK BATH MANUFACTURED BY ISOTHERMAL TECHNOLOGY LTD.

    INTRODUCTION

    The Gemini 550S is the latest version of Isotech's most popular metal block bath. It works over the temperature range 35° C to 550° C.

    At Isotech it is our earnest desire to present for our customers consideration as much useful information as possible and to this end we have spent a substantial amount of time evaluating our products.

    The results of the evaluation of a metal block bath can be presented in many formats some of which will give an optimistic or indeed a pessimistic view of how the product operates.

    For the first time to our knowledge in 1996 a discussion document was written by Germany's Laboratory Accreditation body DKD with the view of standardising the test and certification of metal block baths.

    We have used this document as the basis of the evaluation that follows.

    The evaluation based on the DKD document presents almost the worse case error that may occur within the bath.

    With some care and proper procedures it is possible to improve considerably upon these uncertainties. We have therefore presented a second evaluation based on the best practice as an Appendix to the evaluation.

    SUMMARY

    The Gemini 550S Metal Block Bath Serial Number 550/1 was fully evaluated in two ways.

    Firstly it was evaluated using the guidelines of DKD-R5-4 (Draft) document for the calibration of temperature "block calibrators".

    In document DKD-R5-4 (Draft) Annex 2 a table appears in which an uncertainty is introduced entitled, "Heat Conduction from the Thermometer to be Measured". The uncertainty of this component is quoted as 0.25% of (Tmeas-Tenv).

    At higher temperatures this component becomes the largest source of error and has no relevance to the metal block bath itself, nor is it within the control of the manufacturer of the block bath.

    For this reason we have calculated the bath uncertainties with and without this influence.

    The largest total uncertainties using DKD-R5-4 (Draft) were found to be 0.6° C at 550° C without the measured thermometer error and 1.6° C with the measured thermometer immersion error,

    Secondly it has been evaluated using "good practice and procedures".

    The second evaluation takes an sprt and an industrial resistance thermometer both with UKAS calibrations. Using procedures which are normal in a good quality laboratory, the errors fall below 0.1° C over the whole temperature range.

    It therefore seems that 3 uncertainties can be ascribed to a metal block bath.

    A. That, using "good practice and procedures" with the Gemini 550S gives less than 0.1° C uncertainties.

    B. That, worst case, ignoring the uncertainties of the thermometer to be measured, gives uncertainties of 0.2° C at 35° C, 0.2° C at 275° C and 0.6° C at 550° C.

    C. That, worst case, including an arbitrary test thermometer with heat loss uncertainties of 0.25% (Tmeas-Tenv) gives uncertainties of 0.2° C at 35° C, 0.7° C at 250° C and 1.6° C at 550° C.

    Having carefully considered the work performed in this evaluation of the Gemini 550S metal block bath we can summarise the uncertainties as follows:

    A shows the capabilities of the Gemini 550S when used to Isotech's recommendations.

    B provides a useful evaluation of the profile and stability of the metal block bath. It shows its limitations but not its capabilities.

    C Shows how the errors of the measured thermometer mask the true performance of the bath at the higher temperatures. The thermometer to be measured is a separate item, whose stem conduction should be evaluated in the traditional way of withdrawing the thermometer in 1cm steps.

     

    METHOD OF USE

     

    ERROR VARIATIONS WITH OPERATING PRACTICE

      OPERATING TEMPERATURE
      35° C 275°C 550° C
    A. Good practice and procedures as stated by Isotech 0.1° C 0.1° C 0.1° C
    B. Worst case ignoring stem conduction from the thermometer to be calibrated. 0.2° C 0.2° C 0.6° C
    C. Worst case including stem conduction from thermometer to be calibrated. 0.2° C 0.7° C 1.6° C

    Whenever possible this report follows the recommendations of the Guideline of the Deutscher Kalibriererdienst (DKD, German Calibration Service) for the calibration of temperature block calibrators. DKD-R5-4-(DRAFT) In particular section 2.2 Measurements to Ascertain Calibration Capability.

    Summary of Performance.

    TEMPERATURE

    ° C

    STABILITY

    ±° C

    RADIAL

    HOMOGENEITY

    AXIAL

    HOMOGENEITY

    LOADING

    EFFECT

    35

    275

    550

    0.05

    0.05

    0.05

    0.0005

    0.001

    0.035

    0.013

    0.06

    1.00

    0

    0

    0

    HEAT UP TIME

    50 to 550° C, 60 minutes.

    COOL DOWN TIME AT 23° C AMBIENT

    550° C to 330° C 85 minutes.

    550° C to 135° C 345 minutes.

    (Faster times can be achieved with the fast cool down accessory)

    From DKD-R5-4-(DRAFT)

    2.2.1 Axial Temperature Homogeneity: The axial temperature distribution is to be measured at three different temperatures representative of the field of application and covering the extreme temperatures that may occur. One of several suitable thermometers (e.g. a differential thermocouple) are to be used, and the sensor length must not exceed 5mm. At least six different measurements per bore are to be carried out in the calibration zone and adjoining parts of the bore, the recommended distance between measurement points being about 1cm. If there are several symmetrically arranged bores of equal diameter, the measurement must be carried out in only one representative bore.

    TEST METHOD

    For 50° C two 935-14-61 probes (designed for small stem conduction) were placed in each hole A and E One probe was raised in 1cm steps (Pocket A) and the temperature difference between it and the static probe at the bottom of pocket E was recorded. Alumina powder was placed in the pocket.


    We specify the homogenous zone to be the lower 40mm of the pocket

    AXIAL TEMPERATURE HOMOGENEITY: 35° C

    DISTANCE FROM BOTTOM

    OF INSERT POCKET, CM

    POCKET E

    TEMPERATURE DIFFERENCE

    D T=TA-TE ° C

    0

    1

    2

    3

    4

    5

    6

    0.0105

    0.0165

    0.0165

    0.0055

    0.0035

    -0.0005

    -0.0165

    At 35° C the Maximum Variation over 40mm Zone was 0.013° C

    (This includes the measurement error)

    AXIAL TEMPERATURE HOMOGENEITY: 275° C

    Using a differential type N thermocouple, the lower section is 7.5mm diameter, over all length 300mm. The two "positive" conductors connected to Fluke 45 DVM serial number 45/1.

    DISTANCE FROM BOTTOM OF

    INSERT POCKET, CM

    POCKET E

    TEMPERATURE DIFFERENCE

    D T=TA-TE uV (35uV/° C)

    0

    1

    2

    3

    4

    5

    6

    0

    0

    -2

    -2

    0

    5

    7

    At 275° C the Maximum Variation over 40mm Zone was 0.06° C

    (This includes the measurement error)

    AXIAL TEMPERATURE HOMOGENEITY: 550° C

    Using a differential type N thermocouple in hole E the two junctions are formed with MI type N thermocouples. The two "positive" conductors connected to Fluke 45 DVM serial number 45/1.

    DISTANCE FROM BOTTOM OF INSERT POCKET, CM POCKET E TEMPERATURE DIFFERENCE

    D T = TA-TEm V (39m V/° C)

    0

    1

    2

    3

    4

    5

    6

    0

    21

    33

    37

    39

    32

    -18

    At 550° C the Maximum Variation over 40mm Zone was 1.00° C

    (This includes the measurement error)

    From DKD-R5-4-(DRAFT)

    2.2.2 Radial Temperature Homogeneity: The temperature differences between the zones in the individual bores provided for the measurements are measured with one or several suitable thermometers at three different temperatures respresentative of the field of application and covering the extreme temperatures which may occur. The conditions stated under points 2.1.9 and 2.1.10 must be complied with. If there is only one bore, no measurement is to be carried out.

    TEST METHOD

    Two 935-14-17 thermometers were placed in two 8mm holes (A + E]. Measurements were recorded and then the probes were moved between the two pockets and repeat measurements made. The temperature, D t, was calculated to remove the small offsets between the two probes.

    RADIAL TEMPERATURE HOMOGENEITY, 35° C

    PROBE POCKET A POCKET E
    TA-C

    TA-F

    35.070° C

    35.114° C

    35.075° C

    35.110° C

     

    D t = ? [(tATA-C - tETA-C) + [(tATA-F- tETA-F)]

    Radial Temperature Homogeneity 35°C = 0.0005°C

    RADIAL TEMPERATURE HOMOGENEITY, 275° C

    PROBE POCKET A POCKET E
    TA-C

    TA-F

    276.067° C

    276.091° C

    276.065° C

    276.095° C

    D t = ? [(tATA-C - tETA-C) + [(tATA-F- tETA-F)]

    Radial Temperature Homogeneity 275° C = 0.001° C

    RADIAL TEMPERATURE HOMOGENEITY, 550° C

    PROBE POCKET A POCKET E
    TA-C

    TA-F

    550.120° C

    550.026° C

    550.110° C

    550.106° C

    D t = ? [(tATA-C - tETA-C) + [(tATA-F- tETA-F)]

    Radial Temperature Homogeneity 550° C = 0.035° C

    From DKD-R5-4-(DRAFT)

    2.2.3 Influence upon radial temperature homogeneity due to different loading: A suitable thermometer is placed into the bore located next to the largest bore, with due regard to points 2.1.9 and 2.1.10. The change in temperature is measured which results when a solid metal rod is introduced into the largest bore, in compliance with point 2.1.9, which protrudes from the bore by at least 200mm. The measurement is to be carried out at three different temperatures representative of the field of application and covering the extreme temperatures that may occur. If there is only one bore, no measurement is to be carried out.

    TEST METHOD

    Isothermal Technology recommends an external probe is used to determine the insert temperature. For this test the recommended probe model 935-14-72 is connected to the built in indicator of the site model. A second thermometer is introduced to measure the insert temperature independently - 909 and TTI 2/2 record the temperature measured in pocket A, Probe 935-14-72-550/1 is placed in pocket G. A solid metal rod 360mm long and 19mm diameter is placed in pocket H.

    Insert Temperature, 35° C

      NO ROD ROD ADDED CHANGE DUE

    TO LOADING

    909/885 +TTI 2

    935-14-72+Site

    Indicator (In Built)

    35.25° C

    35.1° C

    35.23° C

    35.1° C

    0.02° C

    As Actual Insert T

     

    The Gemini's separate PRT and in built indicator detected the temperature change due to loading hence

    No additional error due to loading at 35° C

    Insert Temperature, 275° C

      NO ROD ROD ADDED CHANGE DUE

    TO LOADING

    909/885 + TTI 2

    935-14-72+Site

    Indicator (In Built)

    275.189° C

    275.1° C

    275.235° C

    275.1° C

    0.046° C

    As Actual Insert T

    The Gemini's separate PRT and in built indicator detected the temperature change due to loading hence

    No additional error due to loading at 250° C

    Insert Temperature, 550° C

      NO ROD ROD ADDED CHANGE DUE

    TO LOADING

    935-14-72-ZZ+TTI 2

    935-14-72+Site

    Indicator (In Built)

    549.961° C

    550.0° C

    550.034° C

    550.0° C

    0.073° C

    As Actual Insert T

    The Gemini's separate PRT and in built indicator detected the temperature change due to loading hence

    No additional error due to loading at 550° C

    STABILITY WITH TIME

    From DKD-R5-4-(DRAFT)

    2.1.4 Stability with time: The variation of temperature with time in the zones in the individual bores provided for measurements must be sufficiently small. The temperature variations are considered to be sufficiently small when the greatest temperature difference occurring within 30 minutes is smaller than or, equal to, half the uncertainty of the measurement stated.

    Stability at 50° C, 30 minute period, ±0.05° C

    Stability at 250° C, 30 minute period, ±0.05° C

    Stability at 550° C, 30 minute period, ±0.05° C

    TEST METHOD

    A s.p.r.t serial number 909/887 was placed in hole A. The probe was connected to a TTI 2 precision temperature indicator [5] and the variation in temperature was recorded for a 30 minute period at three different temperatures. The ambient temperature was within 23° C ± 3° C.

    HEAT UP TIME

    35° C to 550° C 35 Min.

    Cool Down

    550 to 275° C 85 Min

    550 to 65° C 345 Min

    PROBE AGEING

    A s.p.r.t. (909/887) was placed in a Jupiter along with the reference probe (935-14-17-550/1). The Jupiter 650 was set to the maximum operating temperature of 650° C and the difference between the two probes was recorded at two periods ten hours apart. The probe changed in value by 0.008° C, 8 mK.

    HYSTERESIS (REPEATABILITY)

    The Gemini was set to 110° C and the actual temperature along with the value for the in-built

    temperature indicator was recorded, then the temperature was raised to 550° C for two hours. The temperature was then reset to 110° C and repeat measurements made.

      FROM COLD AFTER 550° C
    Actual 110.052 109.883
    External 110.1 109.8

     

    Change in actual temperature and hence the hysteresis 0.169° C, change in external indicated value 0.1° C, NOTE: Resolution of indicator is 0.1° C

     

    CALCULATION OF THE UNCERTAINTY, DKD METHOD

    CALIBRATION TEMPERATURE, 35° C

    Ambient Temperature 23° C. Using 909/885 with TTI 2 and in built "external" indicator of Gemini 550 with reference probe 935-14-17-550/1.

    SOURCE OF UCT DETERMINATION

    OF UCT

    PROBABILITY

    DISTRIBUTION

    UNCERTAINTY

    ° C

    DIVISOR ui(t),

    ° C

    Standard Thermometer including measurement with standard thermometer UKAS Schedule Normal 0.05 2 0.025
    Axial Temperature distribution This evaluation report Rectangular 0.013 ? 12 0.0038
    Radial Temperature distribution This evaluation report Rectangular 0.0005 ? 3 0.0003
    Loading of block This evaluation report Rectangular 0 ? 3 0
    Stability with time This evaluation report Rectangular 0.05 ? 12 0.014
    Ageing of reference thermometer This evaluation report Rectangular 0.04 ? 3 0.023
    Repeatability (Hysteresis) This evaluation report Rectangular 0.1* ? 3 0.058
    Heat Conduction from thermometer 0.25% of (Tmeas-Tenv) Rectangular 0.03 ? 3 0.017
     
    Combined Uct   k=1 0.083    
    Expanded Uct   k=2 0.166    

     

    *Hysteresis figure is resolution of in built indicator.

    CALIBRATION TEMPERATURE 275° C

    Ambient Temperature 23° C. Using 909/885 with TTI 2 and in built "external" indicator of Gemini 550 with reference probe 935-14-17-550/1.

     

    SOURCE OF UCT DETERMINATION

    OF UCT

    PROBABILITY

    DISTRIBUTION

    UNCERTAINTY

    ° C

    DIVISOR ui(t),

    ° C

    Standard Thermometer including measurement with standard thermometer UKAS Schedule Normal 0.05 2 0.025
    Axial Temperature distribution This evaluation report Rectangular 0.06 ? 12 0.017
    Radial Temperature distribution This evaluation report Rectangular 0.001 ? 3 0.00058
    Loading of block This evaluation report Rectangular 0 ? 3 0
    Stability with time This evaluation report Rectangular 0.05 ? 12 0.014
    Ageing of reference thermometer This evaluation report Rectangular 0.04 ? 3 0.023
    Repeatability (Hysteresis) This evaluation report Rectangular 0.1* ? 3 0.058
    Heat Conduction from thermometer 0.25% of (Tmeas-Tenv) Rectangular 0.63 ? 3 0.36
     
    Combined Uct   k=1 0.37    
    Expanded Uct   k=2 0.74    

     

    *Hysteresis figure is resolution of in built indicator.

    CALIBRATION TEMPERATURE, 550° C

    Ambient Temperature 23° C. Using 909/885 with TTI 2 and in built "external" indicator of Gemini 550 with reference probe 935-14-17-550/1.

     

    SOURCE OF UCT DETERMINATION

    OF UCT

    PROBABILITY

    DISTRIBUTION

    UNCERTAINTY

    ° C

    DIVISOR ui(t),

    ° C

    Standard Thermometer including measurement with standard thermometer UKAS Schedule Normal 0.05 2 0.025
    Axial Temperature distribution This evaluation report Rectangular 1.00 ? 12 0.29
    Radial Temperature distribution This evaluation report Rectangular 0.035 ? 3 0.020
    Loading of block This evaluation report Rectangular 0 ? 3 0
    Stability with time This evaluation report Rectangular 0.05 ? 12 0.014
    Ageing of reference thermometer This evaluation report Rectangular 0.04 ? 3 0.023
    Repeatability (Hysteresis) This evaluation report Rectangular 0.1* ? 3 0.058
    Heat Conduction from thermometer 0.25% of (Tmeas-Tenv) Rectangular 1.32 ? 3 0.76
     
    Combined Uct   k=1 0.82    
    Expanded Uct   k=2 1.64    

    *Hysteresis figure is resolution of in build indicator

    SUMMARY TABLE

    Including the UCT ignoring heat conduction allowance for thermometer under test.

     

    TEMPERATURE UCT OF BLOCK BATH UCT including a theoretical sensor with stem conduction 0.25% Tmeas-Tenv
    35° C

    275° C

    550° C

    0.2

    0.2

    0.6

    0.2

    0.7

    1.6

    GEMINI 550S - AUDIT CALIBRATION

    Appendix 1 of Gemini 550S Evaluation Report

    The evaluation report represents almost the worst uncertainties of use.

    It is normal to recommend that the standard and test thermometer are immersed to a similar depth, which all but eliminates the axial homogeneity assuming the probes are similar. An additional recommendation is to exchange the standard and test thermometer to obtain 2 comparison results which all but eliminates radial inhomogeneity.

    Thirdly, comparing the standard to the test thermometer calibration is made quickly or simultaneously then the absolute stability of the metal block bath is of little importance.

    Here an audit probe was calibrated in the UKAS calibrated Gemini 550S, the audit probe was calibrated by comparison to the supplied external probe and in built indicator arrangement of the Gemini 550S. The audit probe has previously been calibrated in the UKAS Laboratory. The results from the calibration in the Gemini 550S can then be compared to the UKAS calibration.

    The audit probe is an Isotech Model 935-14-95 thermometer which has a 100 ohm resistance element 25mm long. The thermometer is 6mm diameter, 450mm long and has a metal alloy sheath. The serial number is 51196[8]. The thermometer was calibrated in fixed point cells, gallium, tin, zinc and aluminium. The calibration uncertainty of the thermometer is better than ±0.05° C.

    In addition a 25.5 ohm standard platinum resistance thermometer 909/885 was placed in pocket F. This allows the audit probes to be compared directly to the s.p.r.t. and shows the very best results that might be expected from using the Gemini as a comparison bath. The uncertainty of 909/885 and the TTI 2 indicator is ±0.05° C.

    SET POINT ACTUAL TEMPERATURE

    909/885

    TEMPERATURE MEASURED WITH THE Gemini 550S (CORRECTED, from CAL CERT) AUDIT PRT

    51196

    110

    220

    330

    440

    550

    110.052

    220.195

    330.209

    439.945

    549.428

    110.1

    220.2

    330.2

    440.0

    549.4

    110.016

    220.153

    330.163

    439.887

    549.349

     

    CONSIDERING THE DIFFERENCES BETWEEN PROBES

     

    DIFFERENCE FROM

    SPRT

    DIFFERENCE FROM IN-BUILT STANDARD

    UCT FROM DKD

    R5-4-DRAFT

    TEMPERATURE AUDIT PRT 51196 AUDIT PRT 51196  
    110° C

    220° C

    330° C

    440° C

    550° C

    0.036

    0.042

    0.046

    0.058

    0.079

    <0.1° C

    <0.1° C

    <0.1° C

    0.1° C

    <0.1° C

    All less than indicator res.

    0.2 at 35

     

    0.7 at 275

     

    1.6 at 550

    The Audit calibration shows the largest error between the metal sheathed PRT 100 ohm thermometer and either the 25.5 ohm sprt or the in-built standard probe/indicator of the Gemini 550S was 0.1° C over the range of the bath, 35 to 550° C.

     


航空航天军工 | 公司简介 | 客户服务|
联系我们 | 合作伙伴 |返回首页

北京  上海  武汉 香港