חידושים במדידת לחות, טמפרטורה ונקודת הטל. Humidity Theory ? מה זה לחות יחסית Humidity= לחות Water vapor content in a gas (air) If you can see the water it is not in the gas phase anymore! כמות של אדי מים בגז Page 3 / 10-2011 / LES / ©Vaisala Dalton’s Law “The total pressure of a gas is the sum of different gases’ partial pressures” Pt = P1 + P2 + ... E.g. air pressure is the sum of the partial pressures of nitrogen, oxygen, water vapor, carbon dioxide etc... In simple terms, ambient air consists of water vapor and other gases -> water vapor has a partial pressure Pw which is a part of the total pressure Pt = Pw + Pdry Pdry is the sum of the partial pressures of all other gases Page 4 / 10-2011 / LES / ©Vaisala John Dalton 6.9.1766 - 27.7.1844 Water Vapor Saturation Pressure Maximum amount of water vapor that can be present in a gas is water vapor saturation pressure Pws Pws depends on the temperature of the gas: warmer air can contain MUCH more water vapor אוויר חם יכול להכליל הרבה יותר אדי מים מאוויר קר Water vapour’s saturation pressure as a function of temperature Amount at 20°C Amount at 100°C Page 5 / 10-2011 / LES / ©Vaisala Relative Humidity %RH = 100 x Pw / Pws (t) Relative humidity is the ratio of water vapor pressure present in a gas (Pw) to the maximum pressure of water vapor that could be present in the gas in that temperature [Pws(t)] יחס אדי מים באוויר מול כמות מקסימלית של אדי מים שהאוויר יכול להכליל : Ta = 60 °C Pws = 200 hPa Pw = 100 hPa RH = 100 x 100/200 = 50 %RH Page 6 / 10-2011 / LES / ©Vaisala Ta = 100 °C Pws = 1013 hPa Pw = 100 hPa RH = 100 x 100/1013 = 10 %RH Relative humidity is strongly proportional to temperature and its Dewpoint נקודת הטל Dewpoint is the temperature to which a gas must be cooled for the water vapor to condense into water At dewpoint, the relative humidity is 100 %RH The gas is saturated: contains its full capacity of water vapor . הטמפרטורה שצריך לקרר הגז כדי שהאדי מים הִ תְ עַ ּבו Page 7 / 10-2011 / LES / ©Vaisala Dewpoint (continued) Changing the Pressure changes the dew point as the vapor pressure also changes The vapor pressure is directly proportional to total pressure Ta = 60 °C Td = 47 °C Pws = 200 hPa Pw = 100 hPa Ptot =1 bar RH = 100 x 100/200 = 50 %RH Page 8 / 10-2011 / LES / ©Vaisala Ta = 60 °C Td = 60 °C Pws = 200 hPa Pw = 200 hPa Ptot =2 bar RH = 100 x 200/200 = 100 %RH Dewpoint (continued) Changing the temperature doesn´t change the dewpoint, it depends only on the vapor pressure Ta = 60 °C Td = 47 °C Pws = 200 hPa Pw = 100 hPa RH = 100 x 100/200 = 50 %RH Page 9 / 10-2011 / LES / ©Vaisala Ta = 100 °C Td = 47 °C Pws = 1013 hPa Pw = 100 hPa RH = 100 x 100/1013 = 10 %RH When RH and when Td? Td is the preferred parameter in low humidities (~below 10%RH, Tf -10°C) Humidity low i.e. Td << T Humidity high i.e. Td close to T Td RH Also in some high humidity cases when the interest is in avoiding condensation Page 10 / 10-2011 / LES / ©Vaisala Different Measures for Humidity - RH Uses: How much water is there compared to the maximum possible AT THIS TEMPERATURE? Usually the best parameter to use when comfort of humans or in "life sciences" Also traditional measure in meteorology Relative Humidity [%RH] Properties: Range 0…100% VERY strong temperature dependence Also directly proportional to pressure if a gas sample is compressed Page 12 / 10-2011 / LES / ©Vaisala Key Takeaways: Relative humidity depends strongly on temperature If you know temperature and one humidity parameter the others can be calculated Dewpoint does not depend on temperature Page 13 / 10-2011 / LES / ©Vaisala Capacitive HUMIDITY Sensors Structure of the Capacitive Humidity Sensor Only the area where the electrodes overlap matter Page 15 / 10-2011 / LES / ©Vaisala Structure of the Capacitive Humidity Sensor (continued) Upper electrode Conductive material, corrosion resistant. Protects the active material of the sensor from dust, dirt and conductive particles Lets through water vapour Functions as one of the two electrodes in a capacitor Active material A polymer film absorbs water vapour: amount is a function of ambient relative humidity Lower electrode Made of conductive material,corrosion resistant Functions as one of the two electrodes in a capacitor Glass substrate Base that supports the sensor structure Page 16 / 10-2011 / LES / ©Vaisala Operation of the Capacitive Humidity Sensor Water vapour penetrates the upper electrode and reaches the active polymer film. How much water vapour is absorbed into the film depends on the ambient relative humidity. Because the sensor is small and the polymer film thin, the sensor responds quickly to changes in ambient humidity. The water vapour absorbed in the film changes the dielectric properties of the sensor: the capacitance of the sensor changes. The change in the sensor’s capacitance is measured with measurement electronics. Page 17 / 10-2011 / LES / ©Vaisala The solution Page 18 / 10-2011 / LES / ©Vaisala Where to Use Vaisala HUMICAP® Sensors Most normal relative humidity measurements In temperatures of -70 ...+180 °C In humidities 0...100 %RH (with some exceptions in high humidities) In processes without any high concentrations of corrosive gases and/or solvents Page 19 / 10-2011 / LES / ©Vaisala Difficult applications In combined high temperature/high humidity (e.g. +100 °C/95 %RH); more frequent calibration required. When the process contains high concentrations of corrosive gases and/or solvents. In low humidity/high temperature (e.g. +160 °C/ +20 °C dewpoint temperature); in low humidities the measurement accuracy of a RH transmitter may not be good enough DRYCAP ® instruments are more suitable here. Consider Drycap instruments if RH is always <10%RH Page 20 / 10-2011 / LES / ©Vaisala Response Time INTERCAP® T90 with filters/slow moving air: open grid 8s steel netting 20 s sintered filter 40 s Typical time constant of bare chip at 20°C: 2s HUMICAP®180R T90 with filters/slow moving air: open grid 17 s steel netting 50 s sintered filter 60 s Typical time constant of bare chip at 20°C: 10s The response time varies exponentially with the temperature, at -40°C 100x longer than at 20°C (H180): Page 21 / 10-2011 / LES / ©Vaisala Stability – the Key to Good Measurements The graphs below show the excellent stability of the Humicap180R sensor during a 4 years test at the Vaisala outdoor test site Page 22 / 10-2011 / LES / ©Vaisala Application Tests – Wood Dryer Samples: HUMICAP®180R with and without chemical purge Conditions: -30 ... 100°C, 10 ... 100%RH, various chemicals Page 23 / 10-2011 / LES / ©Vaisala A Source for Drift - Chemicals Some chemicals (mainly hydrocarbons) can slowly penetrate the sensor and cause changes in its behaviour. As the time scales involved are many times long this is perceived as drift by the customer instead of cross sensitivity Chemicals usually cause a decrease of sensitivity (gain) of the sensors. If our instruments are found to show too low values at high humidity chemicals are usually to blame if the errors are large. dC0% dC0%, d75% } => Drift in RH-reading Page 24 / 10-2011 / LES / ©Vaisala Capacitance dC75% Chemical Tests – Drift, Saturated Isopropanol Vapor Isopropanol vapor exposure, sensor drift at 0% and 75%RH: Humicap180R can tolerate even large concentrations in many cases Some drift is still seen after long exposures Page 25 / 10-2011 / LES / ©Vaisala Chemical Purge – Principle HUMICAP®180R is briefly heated with an attached PT-100 element. Diffused chemicals are removed from the sensor’s active polymer. Polymer sensor PT-100 Page 26 / 10-2011 / LES / ©Vaisala Chemical Purge – Example, Isopropanol (saturated) Chemical purge after 35 days exposure to Isopropanol (saturated) A chemical purge corrects the error caused by diffused chemicals Page 27 / 10-2011 / LES / ©Vaisala Vaisala’s Patented Warmed Probe Technology Vaisala HUMICAP® sensor Heating element inside the probe Ambient: RHa, Ta , Tda Conditions inside the probe: RHs , Ts , Tda Ambient: Ta = 14 °C Humidity sensor: Ts = 16 °C RHa = 97 %RH RHs = 83 %RH Tda = 13 °C Tda = 13 °C (calculated) NOTE! The heating does not effect in dewpoint! The ambient temperature is measured with separate T-probe! Page 28 / 10-2011 / LES / ©Vaisala Comparison of Warmed and Non-Warmed Sensor Heads in High Humidity Weather Page 29 / 10-2011 / LES / ©Vaisala Key Takeaways HUMICAP®180R is the best sensor on the market with excellent stability and good chemical tolerance Chemical purge can improve stability in applications where chemicals are constantly present. Heated probe technology improves perfomance in condensing conditions Page 30 / 10-2011 / LES / ©Vaisala 5 Things to Remember Relative humidity depends strongly on temperature If you know temperature and one humidity parameter the others can be calculated HUMICAP®180R is the best sensor on the market with excellent stability and good chemical tolerance Heated probe technology improves perfomance in condensing conditions Chemical purge can improve stability in applications where chemicals are constantly present. Page 31 / 10-2011 / LES / ©Vaisala Vaisala Technologies for Humidity/ Dewpoint Measurement Dewpoint is mostly used as a parameter in dry applications, but can be used all over the humidity range Vaisala instruments: DRYCAP® technology for low humidity (below 10%RH) HUMICAP® technology for high humidity (over 10 %RH) Both DRYCAP® and HUMICAP® instruments may have RH and Td/f outputs available. The choice of technology is not about parameter but humidity range of the application Humidity low i.e. Td << T Humidity high i.e. Td close to T DRYCAP Page 32 / 10-2011 / LES / ©Vaisala HUMICAP Vaisala DRYCAP® Sensor Polymer sensor - capacitance signal Measures the ambient water vapor Relative to the number of absorbed water molecules (RH= Pw/Pws ) Temperature sensor resistance signal (Pt-100) Measures the sensor temperature Td is the calculated result of measured RH and T Page 33 / 10-2011 / LES / ©Vaisala Polymer sensor PT-100 Vaisala Autocalibration Vaisala DRYCAP® technology utilize autocalibration procedure for accurate dewpoint measurement Autocalibration warms up the sensor automatically and makes the offset (= zero point) correction: 1) guarantees the very good accuracy in low dewpoints 2) offers excellent long term stability Page 34 / 10-2011 / LES / ©Vaisala Auto-calibration in detail 3. RH and T values logged during cooling phase 4. When drawing a straight line through the collected RH&T points the offset correction value is got as a result 5. Auto-calibration ends: Sensor is cooled and normal measurement mode gets active again using the correction value 6. After set interval (once/hour) auto-calibration repeated Page 35 / 10-2011 / LES / ©Vaisala Sensor temperature Sensor humidity 1. 2. 3. humidity increases 5. 6. time RH/T point before warming 1. RH/T points during the cooling phase Humidity 1. Auto-calibration start: Sensor warmed RH value decreases when T increases 2. Sensor starts to cool down after short warming. RH reading starts to increase. 3. RH/T point right after the warming 2. = Humidity values after offset correction low humidity 0 T increases 4. offset correction value (RH is this much off, e.g. 0.01 %RH) Temperature low T DRYCAP® instruments equipped with intelligent functions Auto-calibration typically once an hour and when the instrument switched on offset correction (zero point correction) Sensor purge once a day and when the instrument switched on gain correction (wet point correction) Sensor head warming Long term stability 2 years recommended calibration interval in case of humidity > 70 %RH to avoid sensor wetting Page 36 / 10-2011 / LES / ©Vaisala DRYCAP® sensor long term stability 55 months Long term stability of VAISALA DRYCAP®180M Dewpoint output reading of three randomly selected units against reference dewpoint at -10, -40 and -60 °C Td test results at +20 °C room temperature, no adjustments done for test units during the test Dewpoint value Reference Thunder humidity generator 0 -10 unit #1 -20 unit #2 2 years 4 years unit #3 -30 Unit # 1 - DMT242 Stored in N2 gas -40 Unit # 2 - DMT242 Stored on room table -50 Unit # 3 - DMT242 Stored on room table -60 accuracy specification ±2°C Td / 2 yrs -70 0 5 10 15 20 25 30 35 time units tested / months Page 37 / 10-2011 / LES / ©Vaisala 40 45 50 55 Drycap recovery from liquid water exposure Dew point reading, -40 Tfp --> immersed in water 1 hour -- > -40 Tfp -10 -15 immersed -20 ['C] -25 -30 -35 -40 -45 0 0.5 1 1.5 2 time [h] Page 38 / 10-2011 / LES / ©Vaisala 2.5 3 3.5 4 DRYCAP® vs. AlOx sensor DRYCAP® sensor AlOx sensor Excellent long term stability Tendency to drift Fast Response time - Necessary especially in dewpoint dependent switching First reaction quick, but slow to stabilize Durable against high humidity and liquid water - no need to protect sensor from ambient humidity or water spikes Loss of calibration when exposed to high humidity Selection of transmitters and sensors available - Optimum sensors for all dryers One old sensor technology available Easy field checks - Compatibility with the hand-held DM70 for easy field checks Typically no field check possibility Low cost of ownership - Long calibration interval High lifetime cost - service costs high vs. purchase price Page 39 / 10-2011 / LES / ©Vaisala Adventages Excellent long term stability: Accuracy specification includes 2 year drift. Fast Response time: Essential especially in dewpoint dependent switching. Durable against high humidity and liquid water: no need to protect sensor from ambient humidity or water spikes. Due to the sensor purge function, durable against typical chemical contaminants & air pollutants often present at industrial sites. Selection of transmitters and sensors available: Optimum sensors for all dryers/ systems. Easy verification on-site: Compatibility with the hand-held DM70 for easy field checks Low cost of ownership: Long calibration interval Page 40 / 10-2011 / LES / ©Vaisala Sampling cells DMT242SC • G3/8”, G1/4” ISO (inlet, outlet) • G1/2” for probe DMT242SC2 • Like above, but with 1/4” swagelok fittings DSC74C • For pressurized air, quick connector and leak screw • Pressurized measurement DSC74C • • For measurement in atmospheric pressure Fixed leak screw 3 ..1 0 bar DMCOIL Page 41 / 10-2011 / LES / ©Vaisala • For venting the sample out in low dew point DMT348 - For Pressurized Pipelines • Durability up to 40 bar (580 psi) • Also long 400 mm probe available • 2 m, 5, 10 and 15 m probe cable • Quick and easy installation in pressurized pipelines • A selection of installation accessories: • Sampling cells • one with thread connection • one with Swagelok connectors • Ball valve • Duct installation flange Page 42 42 / 10-2011 / LES / ©Vaisala Page / 12/1/2014 / name / Internal use / ©Vaisala filter options: DMT342 - With Small Size Flanged Probe for use with sampling cell • Durability with specified accuracy up to 50 bar (725 psia) • Mechanical durability up to 250 bar (3625 psi) • 2 m, 5 m and 10 m probe cable • Excellent for high pressure processes that require small size probe • Direct installation to process or using sampling cell (HMP302SC) filter options: Page 43 43 / 10-2011 / LES / ©Vaisala Page / 12/1/2014 / name / Internal use / ©Vaisala Hand-Held Devices as Spot Check and Field Reference Instruments Page 44 / 10-2011 / LES / ©Vaisala 4 12/1 [Name] Calibration Page 45 / 10-2011 / LES / ©Vaisala HM70 as Field Reference Instrument MI70 indicator has two probe ports: One for reference probe (e.g. HMP75) Other can be simultaneously used for the fixed transmitter to be checked – depending on the transmitter, the adjustment can be done with the MI70 interface, transmitters push buttons or trimmers – transmitter settings (e.g. pressure) Page 46 / 10-2011 / LES / ©Vaisala 4 12/1 [Name] Transmitter not working? Clipping to min / max Frozen value Fluctuating too rapidly Impossible values (sub-zero with refrigerant etc) Td Td1 --43,5°C 43,5°C MI70 Td2- 43,3°C DMT152 dewpoint transmitt er Easy checking with DM70 Display and datalogger Data link verification Reference measurement Powers the ref unit Page 47 / 10-2011 / LES / ©Vaisala Dryer control hand-held meter Referenc e DMT152 dewpoint transmitt er SEE YOU IN THE NEXT APPLICATION .
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