Troubleshooting Two Vacuum Problems. Alton Goodwin Process Engineering, Inc. Birmingham, AL 35201

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Transcription:

roubleshooting wo Vacuum Problems Alton Goodwin Process ngineering, Inc. Birmingham, A 35201 harles Almond Process ngineering, Inc. Birmingham, A 35201 INDUIN In both cases presented, problems associated with condensers and vacuum systems are examined. hese cases were chosen to illustrate how two completely separate problems can exhibit quite similar symptoms and how a formalized approach can assist in obtaining an accurate diagnosis. Accurate troubleshooting requires good data, careful analysis and attention to detail. As illustrated by these two cases, the differences in symptoms of problems may be quite subtle, and knowing what data to collect can be as important as the interpretation of the data Because troubleshooting evaporator problems can be so esoteric, a formal logic tree was developed - a troubleshooting chart. For those of us who frequently are involved in troubleshooting evaporator problems, this organized approach has become instinctive. However, we have found that the discipline of a troubleshooting chart is quite useful to operating personnel by reducing some of the blind alleys that many times bedevil a troubleshooting situation. Accurate troubleshooting requires accurate data. It is usually necessary to obtain vapor temperatures by converting vapor pressures into saturation temperatures. For this reason, the pressure readings are required to be as accurate as possible. he calculated temperatures are usually back checked with a hand held infrared temperature gun. Mill instrumentation is unusually inadequate for accuracy of data required. herefore, it has been found expedient to provide our own portable instrumentation. Pressure data is usually collected with a Fluke Model 245 portable pressure transducer that plugs directly into a common volt-hm multimeter. We have found it advisable to back-check calculated temperatures with an infrared temperature gun. We use a aytech ayngers model AS 1 ase 1 occurred at a major southern Kraft mill where the customer noted a gradual condenser vacuum loss and corresponding capacity loss. he condenser and vacuum system consisted of a single surface condenser with an integral precooler, a two stage steam jet ejector with indirect contact intercooler and aftercooler. Slide 1 he integral precooler consisted of a baffled section of the condenser shell with its entrance at the most hydraulically remote point from the vapor inlet. Non-condensable gases and residual vapor enter the precooler section from the bottom of the condenser. he residual vapors are condensed and the vapors are cooled by cooling water as they travel upward in the baffled section to the outlet near the top of the condenser shell. he precooler exits directly into the primary steam jet ejector suction. he intercooler and aftercooler perform the same function as the precooler, but are stand alone heat exchangers. Slide 2 he initial data points were: Slide 3 1) vapor pressure in the vapor duct immediately before the condenser 2) vapor pressure and temperature in NG line between integral precooler and first stage steam jet ejector 3) condenser cooling water inlet and outlet temperatures.

Data collected at those points indicated: a) he approach temperature of 33 o (60 F) greatly exceeded the expected value of approximately 11 o (20 F), indicating that the condenser heat transfer coefficient was poor. b) he gas inlet temperature of 60 o (140 F) at the first stage greatly exceeded an expected value of approximately 32 o (90 F), indicating that the internal precooler was also not functioning properly. Using the troubleshooting chart, we determined that the following additional data was required: Slide 4 a) emperature profile of the condenser shell b) ondenser condensate level It should be noted here that a temperature profile of the condenser shell can be a powerful tool in evaluating surface condenser operation. For this case, with a top vapor entry condenser, one would expect there to be a small temperature gradient vertically from top to bottom for most of the shell. For that area of the shell containing the precooler, one would expect a larger gradient to be reversed and somewhat greater. he vapor temperature at the precooler section should be at vapor saturation temperature, and the vapor temperature at the top of the precooler section to be within ~five o (ten F) of the cooling water inlet temperature. he secondary data showed a 28 o (50 F) temperature gradient on the condenser both outside the precooler section and inside the precooler section. his gradient indicated either an accumulation of non-condensable gasses or of condensate in the lower portion of the condenser. he normal condensate level observation ruled out an accumulation of condensate indicating non-condensible gas accumulation. Again, from the troubleshooting chart indications were that uncooled vapor and non-condensible gasses bypassing the cooler and were venting higher up on the condenser shell. Slide 5 In this case, apparently a hole had corroded in the vapor side pass baffle and allowed vapor from near the top of the condenser to flow directly into the precooler section without having first gone through the main condensing section. he vapor bypass allowed a large volume of vapor to enter directly into the first stage steam jet ejector and prevented non-condensible gases in the lower portion of the cooler from escaping. Slide 6 As an interim repair, the mill installed a vapor line from the bottom of the condenser directly to the first stage steam jet ejector. his line bypassed the defective precooler, but did allow increased removal of noncondensable gasses. Slide 7 With this modification, the evaporator was able to operate with a condenser vacuum of 17 kpa (2.5 psia) and a condenser vapor temperature of 57 o (135 F). As a permanent solution, the mill installed a new ejector system with an external precooler. Slide 8 he condenser is now operating at near design vacuum and capacity. AS 2 As in case 1, this customer was a major southern Kraft mill that experienced a gradual evaporation capacity loss due to reduced condenser vacuum. he configuration of the condenser and vacuum system was identical to case 1 with a surface condenser and a two stage steam jet ejector system with shell and tube intercooler and aftercooler. he condenser also had an internal precooler section. Slide 9 he first set of data collected was similar to that collected in case 1 - vapor pressure in the vapor duct immediately before the condenser, vapor pressure and temperature immediately before the first stage steam jet ejector, vapor pressure immediately before the second stage steam jet ejector and condenser cooling water inlet and outlet temperatures. It was also observed that the condensate level was normal. Slide 10 his initial set of data indicated that: a) he approach temperature of 58 o (105 F) greatly exceeded the expected value of approximately 11 o (20 F), - indicating that the condenser heat transfer coefficient was poor. b) he low temperature of gases approaching the first stage jet indicated that the internal precooler was functioning normally.

he troubleshooting chart indicated that either the ejectors were overloaded with excess NG or there was a physical problem with the steam jet ejectors. Slide 11 If an NG overload existed, it would have most likely been caused by an air leak somewhere in the vacuum effects. Finding a vacuum leak usually requires an extended outage for a hydrostatic test of some kind to find. he decision was made to try to first determine if there were problems with the ejectors. Page 3 of the troubleshooting chart indicated that additional data was required. Slide 12 he temperature of the NG line immediately adjacent to the first stage steam jet ejector body was read and found to be 71 o 160 F. his reading is in contrast to the 34 o (94 F) temperature for the majority of the line. Slide 13. he high temperature at the suction of the ejector indicated excessive steam passing through (or around) the steam nozzle. - either because of a worn nozzle or a leak around the nozzle itself. Although not listed on the troubleshooting chart, a final test was conducted to verify the preliminary conclusion that a mechanical problem existed with the ejector itself. his test determines the ejectors vacuum under deadhead conditions, i.e. with NG suction valve closed. his test indicated a maximum vacuum of 28 kpa (4.0 psia). Slide 14 Normally a two stage ejector can evacuate to an absolute pressure of 5.2 kpa (0.75 psia). At this point it had been determined that the low vacuum was due to a mechanical problem with the ejector - most likely due to a worn steam either nozzle or steam bypassing the nozzle. he evaporator was shut down and the first stage ejector was disassembled. A wormhole was observed in the ejector housing around the steam nozzle. Slide 15 he wormhole is caused by a small steam leak through the threaded portion of the housing. he flow of the high pressure steam through the leak erodes the metal and forms a path for a significant amount of steam to bypass the nozzle. After the repair, the evaporator was restarted and it was able to operate at near design vacuum and capacity. NUSIN As stated in the introduction, these examples were chosen primarily to illustrate that different problems can exhibit similar symptoms and how an organized procedure is required to efficiently determine the cause. Please note from the two examples that the only observable difference between the two sets of initial data was the temperature of the NG going to the first stage ejector. Secondarily, these examples were chosen because they were the only problems the two evaporators had at the time. he difficulty of troubleshooting an evaporator malfunction is greatly increased when there are multiple problems, especially if they show conflicting symptoms. As an example, if the condenser in case 2 had been fouled on the water side in addition to the ejector problem, the NG to the first stage would have been hot from the condenser to the first stage ejector symptoms similar to case1. his complication of case 2, would have made it much more difficult to identify the real problem.

1 1 S SAG J 2 ND SAG J VAP IN SUFA NDNS I N A F IN ING WA NG SYSM U AS 1 SUFA NDNS AND VAUUM SYSM NFIGUAIN

2 VAP IN NG IN P SIN MAIN NDNSING SIN P SIN BAFF NDNSA U ING WA PASS BAFF ING WA U ING WA IN VIA SH AND UB NDNS WIH INGA P SS SIN

3 5.4 PSIA & 165 F 4.8 PSIA & 140 F 1 S SAG J 2 ND SAG J VAP IN SUFA NDNS 165 F I N A F 115 F 80 F 105 F IN ING WA U NG SYSM AS 1 SUFA NDNS WIH J SYSM INIIA DAA

4 UBSHING HA NDNS VAUUM W, HK ING WA U MPAU, NDNS NDNSA V AND VAP PSSU DP ING WA U MPAU HIGH VAP PSSU DP M HAN 25 F BW VAP MP. DSIGN PBM WIHIN 25 F F VAP P U MPAU H P- U MPAU D HIGH NDNSA V W ING WA FW HIGH ING WA IN MPAU NDNS BM D NDNS BM H J VAD UPUD UB BAMI G SH DAIN BKD AK IN DWNG PUMPING PBM ING W PBM H IN P FUD UBS AI INAKAG XSSIV NG J PBM S HA 3 W VAUUM HA 2 AS 1 SUS FM INIIA DAA

6 VAP IN NG IN H IN P SIN MAIN NDNSING SIN P SIN BAFF NDNSA U ING WA PASS BAFF ING WA U VIA SH AND UB NDNS WIH H IN P SS SIN

5 UBSHING HA NDNS VAUUM W, HK ING WA U MPAU, NDNS NDNSA V AND VAP PSSU DP ING WA U MPAU HIGH VAP PSSU DP M HAN 25 F BW VAP MP. DSIGN PBM WIHIN 25 F F VAP P U MPAU H P- U MPAU D HIGH NDNSA V W ING WA FW HIGH ING WA IN MPAU NDNS BM D NDNS BM H J VAD UPUD UB BAMI G SH DAIN BKD AK IN DWNG PUMPING PBM ING W PBM H IN P FUD UBS AI INAKAG XSSIV NG J PBM S HA 3 W VAUUM HA 2 AS 1 SUIN

7 2.5 PSIA & 135 F 2.2 PSIA & 130 F VAP IN 135 F SUFA NDNS I N A F 130 F 86 F 115 F IN ING WA U NG SYSM SUFA NDNS WIH J SYSM INIM SUIN DAA

8 2.5 PSIA & 135 F 2.2 PSIA & 130 F 2.0 PSIA & 95 F VAP IN 135 F SUFA NDNS P - I N A F 130 F 86 F 115 F IN ING WA U NG SYSM AS 1 SUFA NDNS WIH J SYSM FINA SUIN DAA

9 1 S SAG J 2 ND SAG J VAP IN SUFA NDNS I N A F IN ING WA NG SYSM U AS 2 SUFA NDNS AND VAUUM SYSM NFIGUAIN

11 UBSHING HA NDNS VAUUM W, HK ING WA U MPAU, NDNS NDNSA V AND VAP PSSU DP ING WA U MPAU HIGH VAP PSSU DP WIHIN 25 F F VAP M HAN 25 F BW VAP MP. DSIGN PBM P U MPAU H P- U MPAU D HIGH NDNSA V W ING WA FW HIGH ING WA IN MPAU NDNS BM D NDNS BM H J VAD UPUD UB BAMI G SH DAIN BKD AK IN DWNG PUMPING PBM ING W PBM H IN P FUD UBS AI INAKAG XSSIV NG J PBM S HA 3 W VAUUM HA 2 AS 2 SUS FM INIIA DAA

10 7.0 PSIA & 177 F 6.25 PSIA & 94 F 8.75 PSIA & 145 F VAP IN SUFA NDNS I N A F 72 F 88 F IN ING WA U NG SYSM AS 2 SUFA NDNS AND VAUUM SYSM INIIA DAA

12 UBSHING HA NG J PBM HK WA U MPAUS HK NG IN PAU A J ING WA U MPAU HIGH ING WA U MPAU W NG IN NG IN H W ING WA FW ING WA IN MPAU HIGH DAINAG PBM FUD S MIV SAM PBM J NZZ PBM W PSSU DIFFNIA FW SIIN ING W PBM PUGGD DAIN UPUD UB PY DSIGND DAIN AK IN DAIN SAM PSSU W WA IN SAM SUPHAD SAM WN NZZ BYPASSD NZZ W VAUUM HA 3 AS 2 SUS FM SNDAY DAA

13 7.0 PSIA & 177 F 6.25 PSIA & 94 F 160 F 8.75 PSIA & 145 F VAP IN SUFA NDNS I N A F 72 F 88 F IN ING WA U NG SYSM AS 2 SNDAY DAA IN

14 4.0 PSIA VAP IN SUFA NDNS I N A F IN ING WA NG SYSM U AS 2 SUFA NDNS AND VAUUM SYSM DADHAD S

15 HIGH PSSU SAM IN SAM NZZ WM H NG IN U SAM J J SS SIN