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Teledyne HFM-300 User's Manual

1. cccccccecccecceecceeceecceecceeeeseceseeeeeeeees September 2008 Revision Document Number 151 082009 August 2009 Revision L Document Number 151 102009 October 2009 Revision M Document Number 151 082010 August 2010 pos Visit www teledyne hi com for WEEE disposal guidance The instruments described in this manual are available with multiple pin outs CAUTION Ensure that all electrical connections are correct CAUTION The instruments described in this manual are designed for INDOOR use only The instruments described in this manual are designed for Class 2 installations CAUTION in accordance with IAW IPC standards Hastings Instruments reserves the right to change or modify the design of its equipment without any obligation to provide notification of change or intent to change Manual 151 082010 300 302 Series Page 2 of 31 Table of Contents 1 GENERAL INFORMATION 4 1 1 EEATURESnecrBeteetesmeueemeaueseieser debi dede aee a QE 4 1 2 Iaa EE ILEAN LOIN E E 5 1 3 OPTIONAL 4 20 MA CURRENT OUTPUT e e a e a een as a i e ee ian Ee iaa 5 1 4 OTHER ACCESSORIES 5 5 A E E ede e eee ette AE etti EE EERS 6 LI Hastings Power supplies iu esena ae a E E A ttp ete EE a rN 6 1 4 2 Interconnecting Cables ae e e
2. DESDE Ab yet with passages thin enough to create the differential pressures required for the sensor An Fig 3 4 annular passage meets these requirements The basic operation is similar to the operation of the tubular shunt but the equations for the entry length and pressure drop will be different If we assume that the annular region is very small Ar r Then it be shown that the pressure drop is 120Lu 3 7 5e The shunt must generate a pressure drop at the desired full scale flow which drives the proper flow through the sensor tube to generate a full scale output from the sensor Since the full scale flow of the sensor is the same for all of the different full scale flows that may pass through the shunt the geometry must vary for the different full scale flows in order to generate the same pressured drop for all of them From Equation 3 7 it can be seen that if the width of the annular ring is varied slightly it can correct for very large changes in the full scale flow rate Q Below is a graph showing how the thickness of the annular ring must be changed to create a passage that will properly divide the flow for various full scale flows This graph is based on the 75 Pa pressure drop required to push full scale flow through a particular sensor that has 2 cm spacing between the inlet and outlet taps The flow divider has an outside diameter of 0 95 cm Manual 151 0
3. rae 13 2 11 GAIN POTENTIOMETER Na ave E EN E TURN CURVA TE TEE Big 13 2 12 TEMPERATURE COBFFICIENT Sis erac ee av EATEN CE QW TP ERE TI NEL TE 14 3 THEORY OF OPERATION siso 15 3 1 OVERALI EUNGTIONAL DESCRIPTION erreien rtt Hee eet a He NE te RC Dre Oed 15 3 2 SENSOR DESCRIPTION iioc itecto beu ie be td ete bee esee berti ee bre voe iesu ee e eH e EE vue dd 15 33 SENSOR THEORY eiecti et eene b t eb ueber eb ete 15 3 4 betae E bil dg Rt ad het duin nl ces d guber 17 3 5 SHUNEDESGRIPTION toan oa abito nile TE wees 17 3 6 SHUNTEHEORY rea Eee onto aee 17 3 7 Moe esu d OE eec Esset A d OE Aere 21 3 8 BEECTRONIC CIRGUEITRY E 21 4 reaS E Sa M 22 4 1 TROUBLESHOOTING ate ee rete tante ie o eie taa ct 22 4 2 ADJUSTMENTS e eie oc eiie ite enti ct aid itenudnta nena anii 23 Adel Calibration Brocedure d as aa ded ada eive dte eee ect dau teehee 23 4 3 END CAB REMOVAL ee re
4. P 1 776 107 P 1 929 107 P 0 014 Sensor Where P is the pressure in psig and Error is the fraction of the reading in error The flow reading can be corrected as follows Corrected Indication Indication Error Where the Indication is the indicated flow and Error is the result of the previous formula or read from charts above 2 6 4 Blending of Gases This section describes two methods by which to achieve a controlled blending of different gasses Both methods use the flow signal Output from one flow instrument as the Master to control the Command signal Input to a second unit Manual 151 082010 300 302 Series Page 11 of 31 The first method requires that the two controllers use the same signal range 0 to 5 VDC or 4 to 20 mA and that they be sized and calibrated to provide the correct ratio of gasses Then by routing the actual flow Output signal from the primary meter controller through the secondary controller s External Input pin See Tables 2 1 amp 2 2 the ratio of flows can be maintained over the entire range of gas flows EXAMPLE Flow controller A has 0 100 slpm range with a 5 00 volt output at full scale Flow controller B has 0 10 slpm range with a 5 00 volt output at full scale If flow controller A is set at 80 slpm its output voltage would be 4 00 volts 80 slpm 100 slpm x 5 00 volts 4 00 volts If the output signal from flow controller A is connected to the command Set Point of flow controller B
5. The end effect for a typical laminar flow element in air account for approximately 4 of the total pressure drop For hydrogen however which has a density that is about 14 times less than air and has a viscosity that is much greater than air the second term is completely negligible For the heavier gasses such as sulfur hexafluoride which has a density 5 times that of air the end effects will become 10 of the total This fundamental property makes it a difficult to maintain accuracy specifications when calibrating an instrument using one gas for use with another gas The pressure drop is linear with respect to the volumetric flow rate between a point that is downstream of the entrance area and another point further downstream but upstream of the exit region From Kays amp Crawford that entrance length L of a capillary tube in laminar flow is a function of the Reynolds number and the tube diameter It can be shown that Manual 151 082010 300 302 Series Page 18 of 31 3 5 c For a typical flow divider tube the entry length is approximately 0 16 cm From this it can be seen that if the sensor inlet pickup point is inside of the flow divider tube but downstream of the entrance length and if the sensor outlet point is inside the flow divider tube but upstream of the exit point then the pressure drop that drives the flow through the sensor would be linear with respect to volumetric flow rate Since the pressure drop across the
6. Gain Potentiometer x On the top left of inlet side of the flow controller there is a hole through which the gain potentiometer is accessible Fig 2 3 This gain potentiometer affects the gain of the closed loop controller Normally this potentiometer will be set at the factory for good stable control It may be necessary to adjust this potentiometer in the field if the system varies widely from the conditions under which the controller was setup Turning this gain potentiometer clockwise will improve stability Turning the potentiometer counter clockwise will speed up the valve reaction time to changes in the command signal Control Loop Jumper Manual 151 082010 300 302 Series Page 13 of 31 2 12 Temperature Coefficients As the ambient temperature of Fig 2 8 the instrument changes from the original calibration temperature errors will be Span error vs Temperature introduced into the output of 1 496 the instrument The Temperature Coefficient of Zero describes the change in the output that is seen at zero y 5 06 9E 05x 0 0007 flow This error is added to the 1 0 overall output signal regardless of flow but can be eliminated by merely adjusting the zero potentiometer of the flow meter controller to read zero volts at zero flow conditions The Temperature Coefficient of Span describes the change in output after the zero error is eliminated This error cannot 0 2 be eliminated but can be compensated
7. then flow controller B becomes a slave to the flow signal of controller A The resultant flow of controller B will be the same proportion as the ratio of the flow ranges of the two flow controllers If the set point of flow controller A is set at 50 of full scale and the reference voltage from flow controller A is 2 50 then the command signal going to flow controller B would be 2 50 volts The flow of gas through flow controller B is then controlled at 5 slpm 2 50 volts 5 00 volts x 10 slpm 5 slpm The ratio of the two gases is 10 1 50 slpm 5slpm The mixture of gas A is 90 9090 50slpm 55 slpm and the mixture of gas B is 0 09091 5 slpm 55 slpm Should the flow of flow controller A drop to 78 slpm flow controller B would drop to 3 9 slpm hence maintaining the same ratio of the mixture 78 slpm 100slpm x 5v 3 90v x 50 1 95v 1 95v 5 00v x 10 3 9 slpm 78 slpm 3 9 slpm 20 1 In the blending of two gases it is possible to maintain a fixed ratio of one gas to another In this case the output of one flow controller is used as the reference voltage for the set point potentiometer of a second flow controller The set point potentiometer then provides a control signal that is proportional to the output signal of the first flow controller and hence controls the flow rate of the second gas as a percentage of the flow rate of the first gas 2 7 Output Filter The output signal may have noise superimposed on the mean
8. DER Ete AAEE IARE qe RE ET RR NEO E Aiea 6 2 INSTALLATION AND OPERATION csccssscosssssssssessecsssestasssvectoosessssesestecsesvssesseeessovinseasesesiosseonssesiubessosdestessssessoessvestoosss 7 2 1 RECEIVING INSPECTION BES oe ena Soa F 2 2 POWER REQUIBBEMENIES secte Bok cab d tanita ben Siti re F 2 3 OUTPUT TA ch adhe Pto AE E ATA 7 2 4 MECHANICAL CONNECTIONS fice eon TO OO nO RE EOS 8 2d JFit ting cuissesutea e a rt P GE E a E E d rte rc aee s 8 8 24 3 Plumbing iie d eec e aie dea dpa deca e e 8 2 5 ELECTRICAL CONNECTIONS aon iS 8 2 6 OPERATION er 9 2 6 7 Operating Conditions a pP ee e ba ei bac aep d at 9 VITE TTE 10 2 6 3 High Pressure Operation iei iiia aena idt akea ia Sere eR teet e RE cutee ees ERR ERE abd che ke 10 2 6 4 Blending of Gases iste ande Aa aN EE Oaea AE AET TAE EN aaa Tiaa 11 2 1 OUTPUT EIETER 5 ode OIN UE RIOT 12 2 8 CONTROLLING OTHER PROCESS VARIABLES e ese ese EEE 12 2 9 COMMAND INPUT exero eed ee eyed ab 13 2 10 MALVE OVERRIDE CONTROL dec
9. an outlet plenum See Figure 3 3 Since stability of the flow multiplier is desired to ensure a stable instrument there must be some matching between the linear volumetric flow versus pressure drop of the sensor and the shape of the volumetric flow versus pressure drop of Manual 151 082010 300 302 Series Page 17 of 31 the shunt Most instruments employ Poiseuille s law and use some sort of multi passage device that creates Ca d VA WZ laminar flow between the upstream Cs 04 Vy sensor inlet and the downstream outlet SRLS This makes the volumetric flow versus INLET ESXESAXEVXETA pressure drop curve primarily linear but PLENUM eee VAS PLENU there are other effects which introduce pt higher order terms Most flow transducers are designed such that the outlet plenum has a smaller yy diameter than the inlet plenum This LE LLLL ZY 7 22 eases the insertion and containment of the shunt between the sensor inlet point and the sensor outlet point If the shunt Fig 43 is removed the energy of the gas must be conserved when passing from the inlet ad plenum to the outlet plenum From Bernoulli s equation the sum of the kinetic energy and the pressure at each point must be a constant Since all of the pressure drops are small it can be assumed that the flow is incompressible The
10. and 600 ohm If it is returned to the 15VDC the load must be between 600 and 1200 ohm Failure to meet these conditions will cause failure of the loop transmitter Manual 151 082010 300 302 Series Page 5 of 31 The 4 20 mA I O option can accept a current input The 0 5 VDC command signal on pin 14 can be replaced by a 4 20mA command signal The loop presets an impedance of 75 ohms and is returned to the power supply through the valve common POWER SUPPLY HASTINGS FLOW CONTROLLER PIN OUT H PLC OR ANALOG VO CARD POWER IN 9 ANALOG OUT SETPOINT INPUT PIN 14 uma 77 OHMS ge a i ii ALOG IN 3 ANALOG RETURN ANALOG OUTPUT PIN 6 SWHO 009 0 1 4 Other Accessories 1 4 1 Hastings Power supplies Hastings Power Pod power supply display units are available in one and four channel versions They convert 100 115 or 230VAC to the 15 VDC required to operate the flow meter and provide a digital indication of the flow rate Interface terminals for the retransmission of the flow meter analog output signal are located on the rear of the panel The Power Pod 100 and 400 models are built with controllers in mind but will work with meters as well The Model 40 is for flow meters only Throughout this manual when reference is made to a power supply it is assumed the customer is using a Hastings power supply Hastings PowerPod 100 and PowerPod 400 power supplies are CE marked but the Model 40 does not me
11. but as the complexity of the gas increases its behavior departs from that of an ideal gas Hence the inaccuracy of the GCF increases Hastings Instruments continually searches for better estimates of the GCF s of the more complex gases and regularly updates the list Most Hastings flow meters and controllers are calibrated using nitrogen The conversion factors published by Hastings are meant to be applied to these meters To apply the GCF s simply multiply the gas flow reading and the GCF for the process gas in use For example to calculate the actual flow of argon passing through a nitrogen calibrated meter that reads 20 sccm multiply the reading and the GCF for argon 20 x 1 4047 28 094 Conversely to determine what reading to set a nitrogen calibrated meter in order to get a desired flow rate of a process gas other than nitrogen you divide the desired rate by the GCF For example to get a desired flow of 20 sccm of argon flowing through the meter divide 20 sccm by 1 4047 20 1 4047 14 238 That is you set the meter to read 14 238 sccm Some meters specifically the high flow meters are calibrated in air The flow readings must be corrected for the case where a gas other than air is flowing through the meter In addition there must be a correction for the difference in the GCF from nitrogen to air In this case multiply the reading and the ratio of the process gas GCF to the GCF of the calibration gas For example a meter calibr
12. meter As a result the Hastings 300 flow meter calibration is more stable when changing between measured gases For the 5 sccm 10 sccm and 20 sccm flow rates a solid stainless steel shunt is used The shunt uses a close tolerance fit to block the main flow passage thereby directing all flow through the sensor tube The 50 sccm flow range uses a stainless steel shunt which has been machined flat on an edge The gap between the main flow passage and the flat machined on the shunt creates an alternate laminar flow passage such that the overall gas flow is split precisely between the sensor and the shunt By increasing the number of flats and the size of the laminar shunt passageway flow rates up to 200 sccm are accommodated For flow rates above 200 sccm the shunts are made so that an annular flow passage is formed between the shunt cylinder and the main flow passage A stainless steel plug with an annular spacing of 0 006 0 15 mm accommodates the 500 sccm flow range Increased flow rates require larger gap dimensions Eventually a maximum annular gap dimension for laminar flow is obtained 0 020 0 5 mm This patented shunt technology also includes inboard sensor ports which ensure laminar flow without the turbulence associated with end effects This unique flow geometry provides an exceedingly linear shunt 3 6 Shunt Theory A flow divider for a thermal mass flow transducer usually consists of an inlet plenum a flow restriction shunt and
13. of this aluminum block Aluminum has a very high thermal conductivity which ensures that both ends of the sensor tube and the two coils wound around the ambient block will all be at the same temperature This block is in good thermal contact with the stainless steel base to ensure that the ambient block is at the same temperature as the main instrument block and therefore the same temperature as the incoming gas stream This allows the coils wound on the aluminum block to sense the ambient gas temperature Two identical Wheatstone bridges are employed as shown in Figure 3 2 Each bridge utilizes an ambient temperature sensing coil and a heater coil The heater coil and a constant value series resistor comprise the first leg of the bridges The second leg of each bridge contains the ambient sensing coil and two constant value series resistors These Wheatstone bridges keep each heater temperature at a fixed value of dT 48 C above the ambient sensor temperature through the application of closed loop control and the proper selection of the constant value bridge resistors 3 3 Sensor Theory Consider the sensor design shown in Figure 3 1 The heat convected to or from a fluid is proportional to the mass flow of that fluid Since the constant differential temperature sensor has 2 heater coils symmetrically spaced on the sensor tube it is convenient to consider the upstream and downstream heat transfer modes separately The electrical power suppl
14. referenced to a common ground One of the common pins must be connected to the common terminal of the power supply Case ground should be connected to the AC ground locally The cable shield if available should be connected to AC ground at the either the power supply end or the instrument end of the cable not at both Pin 6 is the output signal from the flow meter The standard output will be 0 to 5 VDC where 5 VDC is 100 of the rated or full scale flow The command set point input should be a 0 5 VDC signal or 4 20mA if configured as such and must be free of spikes or other electrical noise as these would generate false flow commands that the controller would attempt to follow The command signal should be referenced to signal common A valve override command is available to the flow controller Connect the center pin of a single pole three position switch center off to the override pin Connect 15 VDC to one end of the three position switch and 15 VDC to the other end The valve will be forced full open when 15 VDC is supplied to the override pin and full closed when 15 VDC is applied When there is no connection to the pin the three position switch is centered the valve will be in auto control and will obey the 0 5 VDC commands supplied to command set point input Manual 151 082010 300 502 Series Page 8 of 31 SET POINT IN 0 5 VDC POWER SUPPLY PIN 15 PIN 11 PIN FLOW CONTROLLER OUTPUT FLOW CONT
15. replaceable sensor module Field repairs to units can be achieved with a minimum of production line downtime LARGE DIAMETER SENSOR TUBE The Hastings 300 sensor is less likely to be clogged due to its large internal diameter 0 026 0 66mm Clogging is the most common cause of failure in the industry e LOW AP The Hastings 300 sensor requires a pressure of approximately 0 25 inches of water 62 at a flow rate of 10 sccm The low pressure drop across this instrument is ideal for leak detection applications since the pneumatic settling times are proportional to the differential pressure e FAST SETTLING TIME Changes in flow rate are detected in less than 250 milliseconds when using the standard factory PC board settings e LOW TEMPERATURE DRIFT The temperature coefficient of span for the Hastings 300 series is less than 0 03 of full scale from 15 50 The temperature coefficient of zero is less than 0 1 of reading from 0 60 C e FIELD RANGEABLE The Hastings 300 series is available in ranges from 0 5 sccm to 0 25 slpm Each flow meter has a shunt which can be quickly and easily exchanged in the field to select different ranges Calibration however is required e METAL SEALS The Hastings 300 series is constructed of Stainless Steel All internal seals are made with Ni 200 gaskets eliminating the permeation degradation and outgassing problems of elastomer O rings e LOW SURFACE AREA The shunt is designed to h
16. 82010 300 302 Series Page 19 of 31 Fig 3 5 Thickness of the annular ring as a function of flow rate for a sensor with a 75 Pa drop and a 2 cm spacing 2 e nm Passage Thickness cm o o 0 04 0 5 10 15 20 25 30 35 Flow liter min Each shunt must have a section of the annular region upstream of the upstream sensor tap to allow the flow to become fully developed before reaching the first tap The entry length for the annular passage is then 40zzu Below is a graph that demonstrates the entry length that would be required to design a flow divider for various full scale flows The parameters on the sensor that the flow divider must match are the same as the ones on the previous graph Entrance length as a function of flow rate Fig 3 6 for an annular ring of the size specified in figure 3 5 45 Entrance Length cm 0 5 10 15 20 25 30 35 Flow liter min Manual 151 082010 300 302 Series Page 20 of 31 3 7 Control Valve ALVE COIL COVE Fig 3 7 The control valve is an automatic metering solenoid valve see Figure 3 7 While most solenoid valves operate in either the fully open or closed positions the automatic metering solenoid valve is designed to control flow A spring is used to hold a magnetic plunger assembly tightly against an orifice thereby shutting off the flow The magnetic plunger assembly is surrounded by a coil of magnet wire When the coil is ener
17. DC output adjust the zero potentiometer located on the lower inlet side of the flow meter until the meter indicates zero For the optional 4 20 mA output adjust the zero potentiometer so that the meter indicates slightly more than 4 mA i e 4 03 to 4 05 mA This slight positive adjustment ensures that the 4 20 mA transmitter is not in its cut off region The error induced by this adjustment is approximately 0 3 of full scale 4 Turn on gas supply to inlet of instrument and adjust the flow rate to the desired full scale flow as indicated by a reference flow meter controller 5 Adjust Span pot until the indicated flow reads full scale 5 00VDC or 20 mA Perform this step only if a calibrated reference flow meter is available 6 Record flow meter controller and flow reference outputs for flow rates of 20 40 60 80 and 100 and make sure data are within 0 75 3o of full scale 4 3 End Cap Removal The end cap on the inlet side must be removed to gain access to shunt assembly First remove power and shut off the supply of gas to the instrument Disconnect the fittings on the inlet and outlet sides of the transducer and remove it from the system plumbing Remove the four Allen head screws holding the end cap to the instrument Carefully remove the end cap nickel gasket spacer and shunt noting their order and proper orientation The shunt can be severely damaged if dropped Examine the shunt If damaged dirty or blocked clean
18. ROLLER PIN 9 PINS GND VALVE CONTROL OVER RIDE U PIN OUT CONNECTIONS Fig 2 1 SET POINT IN 0 5 VDC POWER SUPPLY FLOW CONTROLLER PINS PIN7 GND H PIN OUT CONNECTIONS VALVE 1 CONTROL Fig 2 2 OVER RIDE Figures 2 1 2 2 and Tables 2 1 2 2 show the 300 302 pin out Table 2 1 U Pin Out ignal Common Do not use Output 0 5 VDC 4 20mA ignal Common Case Ground Valve Override N epe os Se OG 15VDC 2 External Input 6 EA 8 9 2 6 Operation Table 2 2 H Pin Out Do not use Do not use Do not use Do not use Signal Common Output 0 5 VDC 4 20mA Case Ground Valve Override 15VDC Do not use 5 FLOW CONTROLLER OUTPUT The standard instrument output is a 0 5 VDC out and the signal is proportional to the flow i e 0 volts zero flow and 5 volts 100 of rated flow The 4 20 mA option is also proportional to flow 4 mA zero flow and 20 mA 100 of rated flow 2 6 1 Operating Conditions For proper operation the combination of ambient temperature and gas temperature must be such that the flow meter temperature remains between 0 and 60 C Most accurate measurement of flow will be obtained if the flow meter is zeroed at operating temperature as temperature shifts result in some zero offset The Hastings 300 series instrument is intended for use in non condensing environments only Conden
19. TELEDYNE HASTINGS INSTRUMENTS INSTRUCTION MANUAL HFM 300 FLOW METER HFC 302 FLOW CONTROLLER HASTINGS ASA TELEDYNE dh HASTINGS INSTRUMENTS C 150 9001 Teledyne Technologies Company CERTIFIED Manual Print History The print history shown below lists the printing dates of all revisions and addenda created for this manual The revision level letter increases alphabetically as the manual undergoes subsequent updates Addenda which are released between revisions contain important change information that the user should incorporate immediately into the manual Addenda are numbered sequentially When a new revision is created all addenda associated with the previous revision of the manual are incorporated into the new revision of the manual Each new revision includes a revised copy of this print history page Revision C Document Number 151 032000 cesses eene March 2000 Revision D Document Number 151 072000 July 2000 Revision E Document Number 151 092002 September 2002 Revision Document Number 151 082005 August 2005 Revision Document Number 151 032007 March 2007 Revision Document Number 151 062008 ccccseccsseceeceeceeceecaeeceeeceeeeeeceeeeeeaeeeees June 2008 Revision J Document Number 151 092008
20. ailable at the terminals on the rear panel If a Hastings supply is not used the output is available on pin 6 of the D connector It is recommended that the load resistance be no less that 2kQ If the optional 4 20 mA output is used the load impedance must be selected in accordance with Section 1 3 Manual 151 082010 300 302 Series Page 7 of 31 2 4 Mechanical Connections 2 4 1 Filtering The smallest of the internal passageways in the Hastings 300 is the diameter of the sensor tube which is 0 026 0 66 mm and the annular clearance for the 500 sccm shunt which is 0 006 0 15 mm all other flow ranges have larger passages so the instrument requires adequate filtering of the eas supply to prevent blockage or clogging of the tube 2 4 2 Mounting There are two mounting holes 48 32 thread in the bottom of the transducer that can be used to secure it to a mounting bracket if desired The flow meter may be mounted in any position as long as the direction of gas flow through the instrument follows the arrow marked on the bottom of the flow meter case label The preferred orientation is with the inlet and outlet fittings in a horizontal plane As explained in the section on operating at high pressures pressure can have a significant affect on readings and accuracy When considering mounting a flow meter in anything other than a horizontal attitude consideration must be given to the fact that the heater coil can now set up a circu
21. and replace as applicable Reassemble in the Manual 151 082010 300 302 Series Page 23 of 31 reverse order of disassembly A new nickel gasket will be required Secure the endcap with 65 in lb 7 3 N m to 85 in lb 9 6 N m of torque on each stainless steel socket head cap screw Use of a fastener other than the one mentioned here may result in leakage at the seal Recalibration of the Hastings 300 is necessary 4 4 Printed Circuit Board Replacement NOTE This instrument contains static sensitive PC boards Maintain static protection when handling the PC boards In the event that any of the PC boards fail they are easily removed from the instrument and replaced with a spare This ease in disassembly and replacement substantially reduces instrument downtime 1 Replacement of the 4 20 mA option PC board Unplug the power cable from the instruments D connector Remove the fasteners and steel can The 4 20 mA board is the PC board mounted by a single screw Remove the screw and lift off the 4 20 mA board Be careful not to damage the main board and 4 20 mA board connectors 2 Replacement of the main PC board Unplug the power cable from the instruments D connector Remove the fasteners and steel can Remove the 2 screws which fasten the main PC board to the sensor module Gently unplug the main board from the sensor and from the 4 20 mA board if present 4 5 Sensor Replacement Follow instructions for removing the PC boar
22. ated in air is Manual 151 082010 300 302 Series Page 25 of 31 being used to measure the flow of propane The reading from the meter is multiplied by the GCF for propane divided by the GCF of air 20 0 3499 1 0015 6 9875 To calculate a target setting 20 sccm to achieve a desired flow rate of propane using a meter calibrated to air invert the ratio above and multiply 20 1 0015 0 3499 57 2449 Gas conversion factors can be found at the Hastings Instruments web site http www teledyne hi com Follow the link to Mass Flow Products and then to Gas Conversion Factors Manual 151 082010 300 302 Series Page 26 of 31 6 Volumetric Vs Mass Flow Mass flow measures just what it says the mass or number of molecules of the gas flowing through the instrument Mass flow or weight per unit time units are given in pounds per hour lb hour kilograms per sec kg sec etc When your specifications state units of flow to be in mass units there is no reason to reference a temperature or pressure Mass does not change based on temperature or pressure However if you need to see your results of gas flow in volumetric units like liters per minute cubic feet per hour etc you must consider the fact that volume DOES change with temperature and pressure To do this the density grams liter of the gas must be known and this value changes with temperature and pressure When you heat a gas the molecules have more energy and th
23. ave minimal wetted surface area and no un swept volumes This will minimize particle generation trapping and retention CURRENT LOOP The 4 20 mA option gives the user the advantages of a current loop output to minimize environmental noise pickup Manual 151 082010 300 302 Series Page 4 of 31 1 2 Specifications eerte rte eter te Ter Puts lt 0 75 full scale F S at 1 0 F S for gt 10 slm versions Repeatability ire EE tee EU 0 05 of reading 0 02 5 Maximum cedo er ee eru dedere viuum 500 psi 3 45 MPa With high pressure option 1000 psi 6 9 MPa Pressure Coefficient 0 0196 of reading psi 0 0015 kPa N2 See pressure section for higher pressure errors Operating Temperature 0 60 C in non condensing environment Temperature Coefficient zero Maximum 0 1 F S C from 0 to 60 C Temperature Coefficient span Maximum 300 ppm C from 15 to 50 C Maximum 450 ppm C from 0 to 60 C Leak Integrity eri Tto aa ee bw ts lt 1x10 9 std cc s Flow Ranges oo Ain ed EHE ERE MD 0 5 sccm to 0 25 slpm N2 Equivalent Standard Output EAR E NER ERR awake PRAG 0 5 VDC load min 2k Ohms Optional Output c dla eee tue eu
24. d s as described in Section 4 5 Remove the 4 Allen head cap screws that fasten the sensor to the main instrument base Remove the sensor module from the base discarding the used nickel gaskets New nickel gaskets are required for re assembly To place an order or to obtain information concerning replacement parts contact the factory representative in your area See the last page in this manual for the address or phone number When ordering include the following information Instrument model number part description and Hastings part number Manual 151 082010 300 502 Series Page 24 of 31 5 Gas Conversion Factors Gas conversion factors GCF s for gasses metered using Hastings Instruments products can be found by visiting the Hastings Instruments web site The web address can be found at the end of this document The gas conversion factors GCF s provided by Hastings Instruments HT fall into five basic accuracy domains that to a large extent are dependent on the method by which they are found The following table summarizes the different methods used to determine the GCF s The table lists the methods in decreasing order of the degree of accuracy that may be achieved when applying a conversion factor Methods Used to Determine Gas Conversion Factors 1 Determined empirically at Hastings Instruments 2 Calculated From NIST tables 3 Calculated using the virial coefficients of independent investigators empirical data using both
25. e 2 heater coils is easily obtained by measuring the voltage across the heater shown as V on Figure 3 2 and the voltage across the fixed resistor R Since R is in series with the heater R they have the same current flowing through them The electrical power supplied to a given heater is then calculated P V V y 3 2 With constant differential temperature applied to each heater coil and no mass flow through the sensor the difference in heater power will be zero As the mass flow rate through the sensor tube is increased heat is transferred from the upstream heater to the gas stream This heat loss from the heater to the gas stream will force the upstream bridge control loop to apply more power to the upstream heater so that the 48 C constant differential temperature is maintained Manual 151 082010 300 502 Series Page 16 of 31 The gas stream will increase in temperature due to the heat it gains from the upstream heater This elevated gas stream temperature causes the heat transfer at the downstream heater to gain heat from the gas stream The heat gained from the gas stream forces the downstream bridge control loop to apply less power to the downstream heater coil in order to maintain a constant differential temperature of 48 C The power difference at the RTD s is a function of the mass flow rate and the specific heat of the gas Since the heat capacity of many gases is relatively constant over wide ranges of
26. e 28 of 31 Sensor and Main PC Board TRANSDUCER TRANSDUCER HFM 300 Sectional View L SHUNT ENDCAP ENDCAP Manual 151 082010 300 302 Series Page 29 of 31 TRANSDUCER VALVE ASSEMBLY CONTROLLER CARD Wes t SHUNT ENDCAP ENDCAP HFC 302 Sectional View Manual 151 082010 300 302 Series Page 30 of 31 8 WARRANTY 8 1 Warranty Repair Policy Hastings Instruments warrants this product for a period of one year from the date of shipment to be free from defects in material and workmanship This warranty does not apply to defects or failures resulting from unauthorized modification misuse or mishandling of the product This warranty does not apply to batteries or other expendable parts or to damage caused by leaking batteries or any similar occurrence This warranty does not apply to any instrument which has had a tamper seal removed or broken This warranty is in lieu of all other warranties expressed or implied including any implied warranty as to fitness for a particular use Hastings Instruments shall not be liable for any indirect or consequential damages Hastings Instruments will at its option repair replace or refund the selling price of the product if Hastings Instruments determines in good faith that it is defective in materials or workmanship during the warranty period Defective instruments should be returned to Hastings Instruments shipment prepaid together with a w
27. et CE standards at this time The Model 40 and PowerPod 100 are not compatible with 4 20 mA analog signals With the PowerPod 400 individual channels input signals as well as their commands become 4 20 mA compatible when selected The PowerPod 400 also sports a Totalizer feature More information about the Power Pods can be found on the Hastings web site http www teledyne hi com products powerpod series htm 1 4 2 Interconnecting Cables Cables are available from Hastings in various lengths to connect from the 15 pin D connector on the back of the Power Pod directly to any of the 200 series and 300 series flow instruments including digital versions More information about the available cables can be found in the Power Pod 400 bulletin on the Hastings web site http www teledyne hi com pdfs bulletins htm Manual 151 082010 300 302 Series Page 6 of 31 2 Installation and Operation This section contains the steps necessary to assist in getting a new flow meter controller into operation as quickly and easily as possible Please read the following thoroughly before attempting to install the instrument 2 1 Receiving Inspection Carefully unpack the Hastings unit and any accessories that have also been ordered Inspect for any obvious signs of damage to the shipment Immediately advise the carrier who delivered the shipment if any damage is suspected Check each component shipped with the packing list Insure that all parts are
28. ey move around faster so when they bounce off each other they become more spread out therefore the volume is different for the same number of molecules Think about this The density of Air at 0 is 1 29 g liter The density of Air at 25 C is 1 19 g liter The difference is 0 1 g liter If you are measuring flows of 100 liters per minute and you don t use the correct density factor then you will have an error of 10 g minute Volume also changes with pressure Think about a helium balloon with a volume of 1 liter If you could scuba dive with this balloon and the pressure on it increases What do you think happens to the weight of the helium It stays the same What would happen to the volume 1 liter It would shrink Why is the word standard included with the volume terms liters and cubic feet in mass flow applications A mass flow meter measures mass and we know we can convert to volume To use density we must pick one or standard temperature and pressure to use in our calculation When this calculation is done the units are called standard liters per minute SLM or standard cubic feet per minute SCFM for instance because they are referenced to a standard temperature and pressure when the volume is calculated Using the example to the left we can see a standard liter can be defined differently The first balloon contains 0 179 grams of Helium at 0 C and 760 Torr density of 0 179 grams liter Heat up that balloo
29. for 0 0 mathematically if necessary The curve pictured in Figure 2 8 shows the span error in percent 0 2 of point as a function of Temperature C temperature assuming 23 C is 1 2 0 8 0 6 0 4 Span Error of Point the calibration temperature Manual 151 082010 300 302 Series Page 14 of 31 3 Theory of Operation This section contains an overall functional description of the Hastings 300 series of flow instruments In this section and other sections throughout this manual it is assumed that the customer is using a Hastings power supply 3 1 Overall Functional Description The Hastings 300 meter consists of a sensor base and a shunt In addition to the components in a meter The 300 controller includes a control valve and extra electronic circuitry The sensor is configured to measure gas flow rate from 0 to 5 sccm 0 to 10 sccm or 0 to 20 sccm depending on the customer s desired overall flow rate The shunt divides the overall gas flow such that the flow through the sensor is a precise percentage of the flow through the shunt The flow through both the sensor and shunt is laminar The control valve adjusts the flow so that the sensor s flow measurement matches the set point input The circuit board amplifies the sensor output from the two RTD s Resistive Temperature Detectors and provides an analog output of either 0 5 VDC or 4 20 mA 3 2 Sensor Description A cros
30. fter referred to as the Hastings 300 series are intrinsically linear and are designed to accurately measure and control mass flow over the range of 0 5 sccm to 0 10 slm with an accuracy of better than 0 75 F S at 3o from the mean versions gt 10 slm are 1 0 F S Hastings mass flow instruments do not require any periodic maintenance under normal operating conditions with clean gases No damage will occur from the use of moderate overpressures 500 psi 3 45MPa or overflows Instruments are normally calibrated with the appropriate standard calibration gas nitrogen then a correction factor is used to adjust the output for the intended gas Calibrations for other gases such as oxygen helium and argon are available upon special order 1 1 Features LINEAR BY DESIGN The Hastings 300 series is intrinsically linear no linearization circuitry is employed Should recalibration a calibration standard is required in the field be desired the customer needs to simply set the zero and span points There will be no appreciable linearity change of the instrument when the flowing gas is changed NO FOLDOVER The output signal is linear for very large over flows and is monotonically increasing thereafter The output signal will not come back on scale when flows an order of magnitude over the full scale flow rate are measured This means no false acceptable readings during leak testing MODULAR SENSOR The Hastings 300 series incorporates a removable
31. gized the electric current passing through the wire coil produces a magnetic field which attracts the plunger The plunger assembly moves away from the orifice allowing the gas flow to pass between the orifice and the plunger seat The distance between the orifice and the plunger seat and thus the flow through the valve is controlled by the amount of current supplied to the coil The valve seat is made of Kalrez or equivalent per fluoroelastomer The valve orifice is made from Stainless Steel The valve plunger and pole piece are made of nickel plated magnetic alloy Hi perm 49 and the control springs are made of 302 stainless steel Nickel gaskets seal all interfaces between the process gas and the outside environment as described in section 3 4 3 8 Electronic Circuitry The Hastings 300 employs a thermal transfer principle capillary tube described in section 3 2 to measure the flow through the sensor which is proportional to the total flow through the instrument The sensor develops a differential voltage output signal proportional to flow which is amplified to produce 5 VDC at full scale flow The amplified output can be measured on the external D connector If a Hastings power supply is employed the 5 volt output is also sent to the terminals on the back and to the decoding circuitry in the display the optional 4 20 mA analog output is available in lieu of an output voltage The addition of a 4 20 mA current loop transmitter on a seco
32. he zero potentiometer located on the upper right inlet side of the flow meter until the meter indicates zero For the optional 4 20 mA output adjust the zero potentiometer so that the meter indicates slightly more than 4 mA i e 4 03 to 4 05 mA This slight positive adjustment ensures that the 4 20 mA transmitter is not in its cut off region The error induced by this adjustment is approximately 0 3 of full scale Symptom Flow meter is out of calibration and non linear Cause Leaks in the gas inlet or outlet fittings Action Check all fittings for leaks by placing soap solution on all fittings between gas supply and final destination of gas Check flow meter for leaks Replace if required or recalibrate as necessary Symptom Little or no flow even when the valve is in over ride OPEN Cause Blocked orifice or incorrect pressure across the Flowcontroller Action Verify that the pressure drop originally specified on the instrument is across the instrument If the differential pressure across the instrument is correct the orifice may be obstructed Remove all gas pressure and shut off power supply Remove the valve 4 2 Adjustments 4 2 1 Calibration Procedure 1 Calibration must take place with cover firmly in place 2 Connect power to D connector as specified in Section 2 5 Allow the instrument to warm up for 60 minutes with 10 of full scale flow 3 Completely shut off the flow and wait for 2 minutes For the standard 0 5V
33. ied to either of the heater coils will be converted to heat which can be dissipated by radiation conduction or convection The radiation term is negligible due to the Manual 151 082010 300 302 Series Page 15 of 31 low temperatures used by the sensor and because the sensor construction preferentially favors the conductive and convective heat transfer modes The thermal energy of each heater will then be dissipated by conduction down the stainless steel sensor tube conduction to the insulating foam plus the convection due to the mass flow of the sensed gas Because great care is taken to wind the resistive heater coils symmetrically about the midpoint of the tube it is assumed that the heat conducted along the sensor tube from the upstream heater will be equal to the heat conducted through the tube from the downstream heater Similarly the heat conducted from the upstream and downstream coils to the foam insulation surrounding them is assumed to be equal based on the symmetry of the sensor construction Since the sensor tube inlet and outlet are linked by an aluminum ambient bar the high thermal conductivity of the bar provides a thermal short constraining the ends of the sensor tube to be at equal surface temperature Moreover the tube ends and the aluminum ambient bar have intimate thermal communication with the main flow passageway prescribed by the main stainless steel flow meter body This further constrains each end of the sensor t
34. ionally gas is being added or removed from a system to control some other process variable This could be the system pressure oxygen concentration vacuum level or any other parameter which is important to the process If this process variable has a sensor that can supply an analog output signal proportional to its value then the flow controller may be able to control this Manual 151 082010 300 302 Series Page 12 of 31 variable directly This analog output signal could be 0 5 volts 0 10 volts or 4 20 ma for units with 4 20 ma boards or any value in between On the controller card there is a jumper that sets whether the control loop controls mass flow or an external process variable See Figure 2 7 If the jumper is over the top two pins the loop controls mass flow If the jumper is over the bottom two pins the loop controls an external process variable This process variable signal must be supplied on pin 12 of the D connector for U pin out units of the measurement card When the controller is set for external variable control it will open or close the valve as necessary to make the external process variable signal match the command signal The command signal may be 0 5 volts 0 10 volts 4 20 ma for 4 20 ma input output cards or any value in between If the process variable has a response time that is much faster or slower than the flow meter signal it may be necessary to adjust the gain potentiometer 2 9 Command Input The flow contro
35. lating flow through the sensor tube thereby throwing the zero off This condition worsens with denser gases or with higher pressures Whenever possible install the instrument horizontally Always re zero the instrument with zero flow at its normal operating temperature and purged with its intended gas at its normal operating pressure 2 4 3 Plumbing The standard inlet and outlet fittings for the Hastings 300 Series are VCR 4 VCO 4 or 1 4 Swagelok It is suggested that all connections be checked for leaks after installation This can be done by pressurizing the instrument do not exceed 500 psig unless the flow meter is specifically rated for higher pressures and applying a diluted soap solution to the flow connections 2 5 Electrical Connections If a power supply from Hastings Instruments is used installation consists of connecting the HFM 300 302 series cable from the D connector on the rear of the power supply to the D connector on the top of the flow meter controller The H pin out requires cable AF 8 AM grey molded backshell The pin out requires cable 65 791 black molded backshell If a different power supply is used follow the instructions below when connecting the flow meter and refer to either table 2 1 or 2 2 for the applicable pin out The power supply used must be bipolar and capable of providing 15 VDC at 55 mA for flow meter applications and 15 VDC at 150 mA for controllers These voltages must be
36. ller will operate normally with any command input signal between 0 5 volts 4 20 ma for units with 4 20 ma input output cards If the command signal exceeds 14 volts it may damage the circuit cards During normal operation the control loop will open or close the valve to bring the output of the flow meter signal to within 0 001 volts of the command signal The command signal will not match the flow signal if there is insufficient gas pressure to generate the desired flow If the command signal exceeds 5 volts the controller will continue to increase the flow until the output matches the command signal However the flow output does not have any guaranteed accuracy values under these conditions If the command signal is less than 2 of full scale 0 1 volts or 4 32 ma the valve override control circuit will activate in the closed position This will force the valve completely closed regardless of the flow signal 2 10 Valve Override Control The valve override control line provides a method to override the loop controller and open or close the valve regardless of the flow or command signals During normal operation this line must be allowed to float freely This will allow the loop control to open and close the valve as it requires If the valve override line is forced high gt 5 volts the valve will be forced full open If the valve override line is forced negative 5 volts the valve will be forced closed 2 11 Gain Potentiometer Fig 2 7
37. mptom Hastings 300 output continues to indicate flow with no flow present or indicates 14 volts Power supply inputs are correct see the above troubleshooting tip and zero pot has no effect Cause Faulty IC chip s on the main PC board Action Replace main PC board See sections 4 5 and 6 1 Symptom Output of flow meter is proportional to flow but extremely small and not correctable by span pot Cause Sensor is not being heated Action Shut off gas supply and disconnect the power to the flow meter Remove cover and PC board from unit Check the resistance from pins 1 to 2 and 3 to 4 refer to figures in section 6 of the sensor module These pins should read 1650 nominal resistance Also check that the resistance from pins 5 to 6 and 7 to 8 are 400 O nominal value Incorrect resistance values indicate that the sensor unit needs to be replaced Symptom Sensor has proper resistance readings but little or no output with flow Cause Plugged sensor Action Shut off gas supply and disconnect the power to the flow meter Remove cover and PC board from unit Remove and inspect sensor If sensor has evidence of clogging clean or replace as applicable Symptom flow meter reads other than 0 00 VDC with no flow or there is a small flow when the flow meter reads 0 00 VDC Cause Zero pot is out of adjustment Manual 151 082010 300 302 Series Page 22 of 31 Action Shut off all flow For the standard 0 5VDC output adjust t
38. n to room temperature and the volume increases but the mass has not changed The volume is not 1 liter anymore it is 1 08 liters So to define a standard liter of Helium at 25 C we must extract only one liter from the second balloon and that liter weighs only 0 175 grams If a mass flow meter is set up for STP at 0 C and Liter 1 08 Liter Liter 760 Torr when it measures 0 179 grams of He it 0 C 25 25 will give you results of 1 SLM If a second meter is 0 179 grams 1 0 179 g 1 08 0 164 grams set up for STP at 25 C and 760 Torr when it liter liters measures 0 164 grams it will give results of 1 SLM Manual 151 082010 300 302 Series Page 27 of 31 T Drawings and References 5 15 1 BEEN 15 PIN D CONNECTOR 7 302 68 62 2540 P Y 1 Y Y 19 05 92 98 1 50 DAT sl 810 9 5317 X I FITTING TYPE DIM A 18 FEMALE i 8 W NUT 8 BARE 4 W NUT BARE o E 1 4 19 05 FACE 1 4 87 22 10 HFM 300 HFC 302 Outline Drawing All dim Are approximate Manual 151 082010 300 302 Series Pag
39. ndary PC board mounted parallel to the main pc board is required to provide this current loop A jumper change is made on the secondary PC board to establish the selected output mode Manual 151 082010 300 302 Series Page 21 of 31 4 Maintenance This section contains service and calibration information Some portions of the instrument are delicate Use extreme care when servicing the instrument Authorized Maintenance With proper care in installation and use the instrument will require little or no maintenance If maintenance does become necessary most of the instrument can be cleaned or repaired in the field Most procedures may require recalibration Do not attempt these procedures unless calibration references are available Entry into the sensor or tampering with the printed circuit board will void warranty Do not perform repairs on these assemblies while the unit is still under warranty 4 1 Troubleshooting Symptom Output reads strong indication of flow with no flow present Zero pot has no effect Cause Power shorted out Action Turn power supply off for a few seconds and then turn it on again If this is ineffective disconnect the power supply from the unit Check that the power supply voltages are correct Incorrect voltages most likely signify a faulty regulator chip inside the supply If the power supply display returns to zero after the instrument has been disconnected there may be a short from the unit to ground Sy
40. o flow output that is directly proportional to the system pressure Fig 2 4 2 096 4 Span Error vs Pressure 0 026 Sensor Tube 0 0 2 0 4 0 6 0 8 0 10 0 12 0 Span Error reading 14 0 16 0 18 0 20 0 0 100 Manual 151 082010 300 302 Series 300 400 500 600 700 800 900 1000 Pressure psig Page 10 of 31 Fig 2 5 Span Error Vs Pressure 0 017 Sensor 196 Span Error 6 reading 0 1 2 0 100 200 300 400 500 600 700 800 900 1000 Pressure psig If the system pressure is higher than 250 psig 1 7 MPa the pressure induced error in the span reading becomes significant The charts above show the mean error enveloped by the minimum maximum expected span errors induced by high pressures This error will approach 16 at 1000 psig For accurate high pressure measurements this error must be corrected The formulae for predicting mean error expressed as a fraction of the reading are Error 9 887 10 P 3 4154 10 7 P 8 3288 10 P 0 026 Sensor Error 1 533 1077 P 3 304 107 P 1 8313 10 P 0 017 Sensor Error 1 692 10
41. present i e flow meter power supply cables etc Optional equipment or accessories will be listed separately on the packing list There may also be one or more OPT options on the packing list These normally refer to special ranges or special gas calibrations They may also refer to special helium leak tests or high pressure tests In most cases these are not separate parts rather they are special options or modifications built into the flow meter Quick Start Insure flow circuit mechanical connections are leak free Insure electrical connections are correct see label Allow 30 min to 1 hour for warm up Note the flow signal decays toward zero Run 20 flow through instrument for 5 minutes Insure zero flow wait 2 minutes then zero the instrument Instrument is ready for operation 2 2 Power Requirements The HFM 300 meter requires 15 VDC 55 mA 15 VDC 50 mA for proper operation The HFC 302 controller requires 15 VDC 150mA The supply voltage should be sufficiently regulated to no more than 50 mV ripple The supply voltage can vary from 14 0 to 16 0 VDC Surge suppressors are recommended to prevent power spikes reaching the instrument The Hastings power supply described in Section 1 4 2 satisfies these power requirements 2 3 Output Signal The standard output of the flow meter is a 0 5 VDC signal proportional to the flow rate In the Hastings power supply the output is routed to the display and is also av
42. pressure drop over the shunt can be shown to be 4 3 3 AP lpv 2 l 2 D We can see that even with no effect from the shunt there will be a pressure drop between the sensor inlet and outlet points This pressure drop will be a strong function of the ratio of the two diameters Since the drop is a square function of the flow velocity the differential pressure will be non linear with respect to flow rate Note also that the pressure drop is a function of density The density will vary as a function of system pressure and it will also vary when the gas composition changes This will cause the magnitude of the pressure drop due to the area change to be a function of system pressure and gas composition Most of the shunts used contain or can be approximated by many short capillary tubes in parallel From Rimberg we know that the equation for the pressure drop across a capillary tube contains terms that are proportional to the square of the volumetric flow rate These terms come from the pressure drops associated with the sudden compression at the entrance and the sudden expansion at the exit of the capillary tube The end effect terms are a function of density which will cause the quadratic term to vary with system pressure and gas composition The absence of viscosity in the second term will cause a change in the relative magnitudes of the two terms whenever the viscosity of the flowing gas changes 4j apa 200202080 K K 4 2
43. ren Salen tire ee 4 20 mA load 600 Ohms Power Requirements sssssssssseseeme nee nnn 15 VDC 55 mA meters 15 VDC 150 mA controller Class 2 power 150VA max Wetted Materials oi na itched ane data cu ad stainless steel nickel 200 Attitude Sensitivity of zero eee lt 0 7 F S for 90 without re zeroing N2 at 19 7 psia 135 KPa ae oe a Gea ies eae 1 93 Ib 0 88 kg Electrical Connector oi REGERE ERE RRRER ese EERRAM nage ORAE dS 15 pin subminiature D Fitting Options Swagelok 1 8 Swagelok VCR VCO 9 16 18 Female thread Face Seal to Face Seal 1 88 47 75 mm VCR amp Specifications may vary for instruments with ranges greater than 10 slpm 1 3 Optional 4 20 mA Current Output An option to the standard 0 5 VDC output is the 4 20 mA current output that is proportional to flow The 4 20 mA signal is produced from the 0 5 VDC output of the flow meter The current loop output is useful for remote applications where pickup noise could substantially affect the stability of the voltage output The current loop signal replaces the voltage output on pin 6 of the D connector The current loop may be returned to either the signal common or the 15 VDC connection on the power supply If the current loop is returned to the signal common the load must be between 0
44. ritten statement of the problem and a Return Material Authorization RMA number Please consult the factory for your RMA number before returning any product for repair Collect freight will not be accepted 8 2 Non Warranty Repair Policy Any product returned for a non warranty repair must be accompanied by a purchase order RMA form and a written description of the problem with the instrument If the repair cost is higher you will be contacted for authorization before we proceed with any repairs If you then choose not to have the product repaired a minimum will be charged to cover the processing and inspection Please consult the factory for your RMA number before returning any product repair TELEDYNE HASTINGS INSTRUMENTS 804 NEWCOMBE AVENUE HAMPTON VIRGINIA 23669 U S A ATTENTION REPAIR DEPARTMENT TELEPHONE 757 723 6531 TOLL FREE 1 800 950 2468 FAX 757 723 3925 E MAIL hastings instruments teledyne com INTERNET ADDRESS http www teledyne hi com Repair Forms may be obtained from the Information Request section of the Hastings Instruments web site Manual 151 082010 300 302 Series Page 31 of 31
45. s section of the sensor is shown in Figure 3 1 The sensor consists of two coils of resistance wire with a high temperature coefficient of resistance 3500 ppm C wound around a stainless steel tube with internal diameter of 0 6604 mm and 7 62 cm length Each coil is 1 372 cm in length and they are separated by 1 27 mm distance These two identical resistance wire coils are used to heat the gas stream and are symmetrically located upstream and downstream on the sensor tube Insulation surrounds the sensor tube and heater coils with no voids around the tube to prevent any convection losses The ends of this sensor tube pass through an aluminum block and into the stainless steel sensor base This aluminum block thermally shorts the ends of the sensor tube and maintains them at ambient temperature There are two coils of resistance wire that are wound around the aluminum block The coils are identical to each other and are symmetrically spaced on the aluminum ambient block These coils are wound from the same spool of wire that is used for the sensor heater coils so they have the same resistivity and the same temperature coefficient of resistance as the sensor heater coils The number of turns is controlled to have a resistance that is 10 times larger than the resistance of the heater coils Thermal grease fills any voids between the ambient temperature block and the sensor tube to ensure that the ends of the sensor tube are thermally tied to the temperature
46. sate or any other liquids which enter the flow meter may destroy its electronic components Manual 151 082010 300 302 Series Page 9 of 31 2 6 2 Zero Check Fig 2 3 Turn the power supply on if not already energized Allow for a 1 hour warm up Stop all flow through the instrument and wait 2 minutes Caution Do not assume that all metering valves completely shut off the flow Even a slight leakage will cause an indication on the meter and an apparent zero shift For the standard 0 5 VDC output adjust the zero potentiometer located on the inlet side of the flow meter until the meter indicates zero Fig 2 3 For the optional 4 20 mA output adjust the zero potentiometer so that the meter indicates slightly more than 4 mA i e 4 03 to 4 05 mA This slight positive adjustment ensures that the 4 20 mA current loop transmitter is not in the cut off region The error induced by this adjustment is approximately 0 3 of full scale This zero should be checked periodically during normal operation Zero adjustment is required if there is a change in ambient temperature or vertical orientation of the flow meter controller 2 6 3 High Pressure Operation When operating at high pressure the increased density of gas will cause natural convection to flow through the sensor tube if the instrument is not mounted in a level position This natural convection flow will be proportional to the system pressure This will be seen as a shift in the zer
47. sensor now increases linearly with the main flow rate and the sensor has a linearly increasing flow with respect to pressure drop there is now a flow through the sensor which is directly proportional to the main flow through the flow divider without the flow division errors that are present when the sensor samples the flow completely upstream and downstream of the flow divider Unfortunately a typical shunt has an internal diameter on the order of 0 3 mm This is too small to insert tap points into the tube Also the sample flow through the sensor is approximately 10 sccm while the flow through a shunt is approximately 25 sccm This means the sample flow would be affecting the flow it was trying to measure If the sensor tube is made large enough and with enough flow through it to insert WILL VA Lh J JA SAL A the sensor taps at these m XS positions then the pressure drop LE 2 d x RKF would be too small to push the e ee 24 E A necessary flow through the sensor KK OK 2 SIR RE 34 K REX 2 tube INLET __ SOROS SSRI KR OY KR OUTLET PLENUM SIRI OUT PLENUM PX XS A 29 The solution is to use a different CR eae geometry for the flow tube It OK 2 s ERE 7 LK f X must be large enough to allow B A 6 2 ve MRL SOILS xX the sample points in the middle M
48. te OWN re D E EE HEINE oie SERRE ev weeds 23 4 4 PRINTED CIRCUIT BOARD REPLACEMENT eee ere e e enenennn ener nnns nsns uses is ese uses e se ese ese ses ss esas esee ases ue 24 4 5 SENSOR REPLACEMENT ceo diti eet e e neret e Ee ee e NE EL e e TRIER Eun 24 5 GAS CONVERSION FACTORS 5 eres eei twee to sees cadechossadecncnsaseedsouscesssbucdesvesvaseavcouesevesusssavesosinavessssesucsteusexessbdeeesess 25 6 VOLUMETRIC VS MASS FLOW icisssscscsecssscoicssscccsessecsosectecssvessocssvciosssbecsesusbecsooessesesbsesosusbecsesestesdeenssosdevdaccoseviecsteessess 27 7 DRAWINGS AND REFERENCES isssscccsscssscsisvsncsosectecsosestecssvecdoosevesdosesbecsesussensesvssesseesssssdusossosdeseadsebecsosecdeccosestacsdbessess 28 8 UE SIS WW eae 31 8 1 WARRANTY REPAIR POLICY ve ccccrccvseiencceavscuecpacaceedesvacdecDavsucccparseuedpucadesdeavandespecauacep anuvuedpavededepansedesdeegescevaresieaperseaceberse 31 8 2 NON W ARRANTY REPAIR POLICY eeeeeeeeeeeeenene e e e emen nnnnnn nnns nn ese nsi e ese sane uses e ese ese ese s ases EEEE ases e sese esee 31 Manual 151 082010 300 302 Series Page 3 of 31 1 General Information The Teledyne Hastings HFM 300 is used to measure mass flow rates in gases In addition to flow rate measurement the HFC 302 includes a proportional valve to accurately control gas flow The Hastings mass flow meter HFM 300 and controller HFC 302 herea
49. temperature and pressure the flow meter may be calibrated directly in mass units for those gases Changes in gas composition require application of a multiplication factor to the nitrogen calibration to account for the difference in heat capacity The sensor measures up to 20 sccm full scale flow rate at less than 0 75 F S error The pressure drop required for a flow of 20 sccm through the sensor is approximately 0 5 inches of H O 125 Pa 3 4 Base The stainless steel base has 1 5 by 1 0 38 1 mm by 25 4 mm cross section and is 3 64 92 5 mm long The length from face seal fitting to face seal fitting is 4 88 124 0 mm The base has an internal flow channel that is 0 75 19 1 mm diameter Metal to metal seals are used between the base and endcaps as well as the base and sensor module Gaskets made of nickel 200 are swaged between mating face seals machined into the stainless steel parts All metal seals are tested at the factory and have leak rates of less than 1x10 std cc s Because of this corrosion resistant all metal sealed design the Hastings 300 can measure corrosive gases which would damage elastomer sealed flow meters 3 5 Shunt description The flow rate of interest determines the size of the shunt required As previously indicated 9 separate shunts are required for the range of flow spanning 5 sccm to 10 slpm full scale These shunts employ a patented method of flow division which results in a more linear flow
50. temperature and pressure as variables 4 Calculated from virial coefficients using temperature only 5 Calculated from specific heat data at 0 C and 1 atmosphere 1 most accurate method is by direct measurement Gases that can be handled safely inert gases gases common in the atmosphere etc can be run through a standard flow meter and the GCF determined empirically 2 The National Institute of Standards and Technology NIST maintains tables of thermodynamic properties of certain fluids Using these tables one may look up the necessary thermophysical property and calculate the GCF with the same degree of accuracy as going directly to the referenced investigator 3 and 4 Many gases that have been investigated sufficiently by other researchers can have their molar specific heat calculated The gas conversion factor is then calculated using the following ratio pN2 GCF pGasX GCF s calculated in this manner have been found to agree with the empirically determined GCF s within a few tenths of a percent Data from investigations that factor in pressure as well as temperature usually supply a higher degree of accuracy in their predictions 5 For rare expensive gases or gases requiring special handling due to safety concerns one may look up specific heat properties in a variety of texts on the subject Usually data found in this manner applies only in the ideal gas case This method yields GCF s for ideal gases
51. ube to be equal to the ambient gas temperature Further since the length of each heater section is nearly 21 times greater than the inside tube diameter the mean gas temperature at the tubes axial midpoint is approximately equal to the tube surface temperature at that point Recall that the outside of the sensor tube is well insulated from the surroundings therefore the tube surface temperature at the axial midpoint is very close to the operating temperature of the heater coils The mean temperature of the gas stream is then approximately the same as the heater temperature Assuming the mean gas temperature is equal to the heater temperature it can be shown that the differential pressure is 3 1 P P 2mC heater T mibien The value of the constant pressure specific heat of a gas is virtually constant over small changes in temperature By maintaining both heaters at the same constant temperature difference above the ambient gas stream temperature the difference in heater power is a function only of the mass flow rate Fluctuations in ambient gas temperature which cause errors in conventional mass flow sensors are avoided the resistance of the ambient sensing coil changes proportionally with the ambient temperature fluctuations causing the closed loop control to vary the bridge voltage such that the heater resistance changes proportionally to the ambient temperature fluctuation The power supplied to each of th
52. voltage levels This noise may be due to high turbulence in the flow stream that the fast sensor is measuring or it could be electrical noise when the flow meter has a high internal gain i e 5 sccm full scale meter Varying levels of radio frequency noise or varying airflow over the electronics cover can also induce noise Noise can be most pronounced when measuring the flow output with a sampling analog digital A D converter When possible program the system to take multiple samples and average the readings to determine the flow rate If less overall system noise is desired a jumper may be installed over the pins of JP 1 on the flow measurement card See Figure 2 6 Covering the pins closest to the D connector will activate a resistor capacitor RC filter that has a time constant of one second This will increase the x settling time of the indicated flow rate to approximately 4 seconds Covering the other two pins will lower the response time to approx 1 second This adjustment will not affect the calibration of the flow meter circuit or the actual flow response to change in command signal flow controllers This will only slow down the indicated response output voltage current 2 8 Controlling Other Process Variables Normally a flow controller is setup to control the mass flow The control loop will open and close the valve as necessary to make the output from the flow measurement match the input on the command line Occas

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