ML12300A222: Difference between revisions
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100072780State Registration No. | 100072780State Registration No. | ||
Date _______________ | Date _______________ | ||
E12.5.1913 0 Rev.DOCUMENT IDENTIFICATION Task 5 - Non-Condensable Gases E12.5.1913 12x14x14.5 CVDS 1/8 TABLE OF CONTENTS 1.0PURPOSE ................................................................................................................................................................. 22.0BACKGROUND ................................................................................................................. | E12.5.1913 0 Rev.DOCUMENT IDENTIFICATION Task 5 - Non-Condensable Gases E12.5.1913 12x14x14.5 CVDS 1/8 TABLE OF CONTENTS 1.0PURPOSE ................................................................................................................................................................. | ||
==22.0BACKGROUND== | |||
................................................................................................................. | |||
..................................... 23.0SCOPE ...................................................................................................................................................................... 24.0ANALYSIS.................................................................................................................... | ..................................... 23.0SCOPE ...................................................................................................................................................................... 24.0ANALYSIS.................................................................................................................... | ||
............................................ 35.0RESULTS AND CONCLUSIONS .................................................................................................... | ............................................ 35.0RESULTS AND CONCLUSIONS .................................................................................................... | ||
...................... 76.0BIBLIOGRAPHY ............................................................................................................... | ...................... 76.0BIBLIOGRAPHY ............................................................................................................... | ||
..................................... 8 Task 5 - Non-Condensable Gases E12.5.1913 12x14x14.5 CVDS 2/8 1.0PURPOSE The purpose of this report is to evaluate the potential impact of the evolution of non-condensable gases on the mechanical seals of Monticello RHR pumps.2.0BACKGROUND Dissolved gases are present in water depending on the fluid temperature, gas solubility, pressure, and duration of contact. For extended time duration, the gas and liquid will come to an equilibrium | ..................................... 8 Task 5 - Non-Condensable Gases E12.5.1913 12x14x14.5 CVDS 2/8 1.0PURPOSE The purpose of this report is to evaluate the potential impact of the evolution of non-condensable gases on the mechanical seals of Monticello RHR pumps. | ||
==2.0BACKGROUND== | |||
Dissolved gases are present in water depending on the fluid temperature, gas solubility, pressure, and duration of contact. For extended time duration, the gas and liquid will come to an equilibrium | |||
state according to Henry's Law. As a liquid passes through a centrifugal pump, the reduced pressure | state according to Henry's Law. As a liquid passes through a centrifugal pump, the reduced pressure |
Revision as of 11:28, 8 February 2019
ML12300A222 | |
Person / Time | |
---|---|
Site: | Monticello, Boiling Water Reactor Owners Group ![]() |
Issue date: | 08/31/2012 |
From: | Kalra A Sulzer Pumps (US), PWR Owners Group |
To: | Office of Nuclear Reactor Regulation |
Shared Package | |
ML123000308 | List: |
References | |
BWROG-12051 BWROG-TP-12-013, Rev 0 | |
Download: ML12300A222 (12) | |
Text
{{#Wiki_filter:Containment Accident Pressure Committee Task 5 - Effects of Non-Condensible Gases on Seals (CVDS Pump)
Author: Ankur Kalra (Sulzer Pump) Project Manager: Kenneth Welch (GEH) Committee Chairman: John Freeman (Exelon) BWROG-TP-12-013 Revision 0 August 20 12 BWROG-TP-12-013 REV 0 INFORMATION NOTICE Recipients of this document have no authority or rights to release these products to anyone or organization outside their utility. The recipient shall not publish or otherwise disclose this document or the information therein to others without the prior written consent of the BWROG, and shall return the document at the request of BWROG. These products can, however, be shared with contractors performing related work directly for the participating utility, conditional upon appropriate proprietary agreements being in place with the contractor protecting these BWROG products. With regard to any unauthorized use, the BWROG participating Utility Members make no warranty, either express or implied, as to the accuracy, completeness, or usefulness of this guideline or the information, and assumes no liability with respect to its use. BWROG Utility Members CENG - Nine Mile Point Chubu Electric Power Company DTE - Fermi Chugoku Electric Power Company Energy Northwest - Columbia Comisión Federal de Electricidad Entergy - FitzPatrick Hokuriku Electric Power Company Entergy - Pilgrim Iberdrola Generacion, S.A. Entergy - River Bend/Grand Gulf Japan Atomic Power Company Entergy - Vermont Yankee J-Power (Electric Power Development Co.) Exelon (Clinton) Kernkraftwerk Leibstadt Exelon (D/QC/L) South Texas Project Exelon (Oyster Creek) Taiwan Power Company Exelon (PB/Limerick) Tohoku Electric Power Company FirstEnergy - Perry Tokyo Electric Power Company NPPD - Cooper NextEra - Duane Arnold PPL - Susquehanna PSEG - Hope Creek Progress Energy - Brunswick SNC - Hatch TVA - Browns Ferry Xcel - Monticello
BWROG-TP-12-013 REV 0 2 Executive Summary This BWROG Technical Product provides an evaluation of the effect of non-condensable gases which come out of solution and migrate to a pump seal purge piping. The evaluation is based on the seal purge piping arrangement of the Monticello RHR pump (model CVDS).
Implementation Recommendations This product is intended for use to address (in part) issues raised in the NRC Guidance Document for the Use of Containment Accident Pressure in Reactor Safety Analysis (ADAMS Accession No. ML102110167). Implementation will be part of the BWROG guidelines on the use of Containment Accident Pressure credit for ECCS pump NPSH analyses. Benefits to Site This product provides a technical response to the NRC concerns raised in the reference document above about the potential pump seal damage resulting from gases which come out of solution and migrate into the pump seal purge piping. QUALITY LEVEL SULZER PUMPS (US) INC. DOCUMENT ASME CODE SECTION Direct DOC. NO: E12.5.1913 Indirect ORDER NO: CLASS NO.CODE EDITION (YEAR)TITLE: Task 5 - Effect of Non-Condensable Gases on Seals Sulzer Pumps (US) Inc. SEASON YEARMonticello - 12x14x14.5 CVDS RHR Pump CUSTOMERGE-HITACHI Nuclear Energy Americas LLC PROJECT Monticello Nuclear Power Station, Monticello, MN CUSTOMER P.O. NO. 437054820CONTRACT NUMBER SPECIFICATION NO. ITEM / TAG NUMBER CUSTOMER APPROVAL NUMBER: CUSTOMER APPROVAL REQUIREMENT Yes No Information Only SPACE FOR CUSTOMER APPROVAL STAMP CERTIFIED AS A VALID SULZER PUMPS (US) INC. DOCUMENT (when applicable/available) For Outside Vendor For Manufacture at Sulzer Pumps (US) Inc. Risk Release Inspection Report # ________________ Other (specify) _______________________ APPROVALS(SIGNATURE)Date Engineering 04/23/12QualityAssurance CERTIFICATION (when applicable) Originating Advance Engineering This Document is certified to be in compliance Dept: with THE APPLICABLE PURCHASE ORDER, By: SPECIFICATIONS, PROCEDURES, AND ADDITIONAL REQUIREMENTS LISTED IN Ankur KalraTHE APPENDICES. Title: Hydraulic Design Engineer Date: 11/7/2011__________________________________________Professional Engineer APPLICABLE S.O. NUMBERS: ___________ _____________________________ 100072780State Registration No. Date _______________ E12.5.1913 0 Rev.DOCUMENT IDENTIFICATION Task 5 - Non-Condensable Gases E12.5.1913 12x14x14.5 CVDS 1/8 TABLE OF CONTENTS 1.0PURPOSE .................................................................................................................................................................
22.0BACKGROUND
.................................................................................................................
..................................... 23.0SCOPE ...................................................................................................................................................................... 24.0ANALYSIS.................................................................................................................... ............................................ 35.0RESULTS AND CONCLUSIONS .................................................................................................... ...................... 76.0BIBLIOGRAPHY ............................................................................................................... ..................................... 8 Task 5 - Non-Condensable Gases E12.5.1913 12x14x14.5 CVDS 2/8 1.0PURPOSE The purpose of this report is to evaluate the potential impact of the evolution of non-condensable gases on the mechanical seals of Monticello RHR pumps.
2.0BACKGROUND
Dissolved gases are present in water depending on the fluid temperature, gas solubility, pressure, and duration of contact. For extended time duration, the gas and liquid will come to an equilibrium
state according to Henry's Law. As a liquid passes through a centrifugal pump, the reduced pressure
at the pump inlet can result in some of the dissolved gas coming out of solution as gas bubbles. Since
the pump seals are continuously cooled using flush water from the pump discharge, the flush water
will contain small amounts of gas bubbles. In addition, it is also possible that air bubbles can migrate
within the pump casing into the pump seals. 3.0SCOPE The following are evaluated in this report. Froude number and critical flow calculation are used to determine the possibility of bubble accumulation in the discharge end and mechanical seal piping. Mechanical seal flush piping orientation, seal flush, and internal bearing flush injection system's role in permitting entrained air to accumulate in the stuffing box region of the pump. Task 5 - Non-Condensable Gases E12.5.1913 12x14x14.5 CVDS 3/8 4.0ANALYSIS This report evaluates the potential for the accumulation of the non-condensable gases at the mechanical seal faces that could cause the lack of lubrication and cooling of the seal faces leading to
damage and eventual seal failure. To predict gas accumulation it is important to understand the piping
configuration and the flow characteristics of the two-phase (liquid along with the entrained gas) fluid.
Figure 1 shows examples of two phase flows. The Froude number, a ratio of inertial force on a liquid
to gravitation force, is a useful parameter for predicting non-condensable gas dynamics in a fluid
carrying duct. Figure 1: Entrained Air in Pipes [Ref 1] 4.1According to BWROG,The suppression pool water is normally at a range of [[ ]] to [[ ]] and is at equilibrium with the suppression pool air space, which is composed of [[
]]4.2 In the case of the Monticello RHR pumps the mechanical seals are lubricated and cooled by pumpage (flush) that is tapped off from the discharge nozzle (See Fig. 2). Water at high
pressure enters the cyclone separator where any debris in the flush is separated out.
A Froude number calculation for the discharge and the seal piping can show if the bubbles
trapped in the fluid will travel through the mechanical seal flush piping and reach the internal
bearings. It is important to note that; Task 5 - Non-Condensable Gases E12.5.1913 12x14x14.5 CVDS 4/8 Froude number (Fr) > 1 Supercritical Flow Froude number (Fr) < 1 Subcritical Flow According to several studies done on bubble propagation in circular water pipes it is found that in a supercritical flow a bubble will travel with the fluid in its direction of flow [4]. In other words, bubble/entrained air will not stagnate and accumulate which may block the flow path.
Following is a calculation of the froude number for the RHR pump discharge side. D g V Fr Froude/)( Where, Equation 1 [5] V = Flow velocity, ft/sec g = Acceleration due to gravity = 32.2 ft/sec^2
D = Pipe ID, ft For RHR Pump, discharge ID is [[ ]]rea SectionalA Cross FlowRate V ty FlowVeloci)(, At the flow rate of [[
]], and cross sectional area of
[[
]], V = [[ ]] and Fr =
[[ ]].In case of RHR pump mechanical seals, pipe used is [[
]], with an ID of
[[ ]].Flow is typically [[ ]], which is [[
]]and 2 4 D rea SectionalA Cross=[[ ]]V = [[ ]] and Fr =
[[ ]].Since Fr is above 1 the flow is supercritical in both the discharge and the mechanical seal piping. This shows that bubbles will not accumulate in the piping and block the flow of flush
through the discharge end or the mechanical seal piping. In addition to the above calculation, another equation derived from experimental tests predicts the flow below which the air bubbles will accumulate in the discharge piping and the seal
piping. This flow is called the critical flow (Qc). Task 5 - Non-Condensable Gases E12.5.1913 12x14x14.5 CVDS 5/8 2 1 2 5 38.0 g D Q c Equation 2 [4] Where, D = Pipe ID, in
g = 32.2 ft^2/sec Using the above equation, critical flow for the discharge piping equals [[ ]] and for the seal piping [[ ]]. Hence, blockage of flow due to bubble accumulation is possible if flow rate in the discharge piping falls below [[ ]] or below [[ ] ]in the seal piping. The expected flow through the discharge piping is [[
]]and seal piping is
[[ ]], both of which are well above the critical flow values.
4.3 After
passing through the mechanical seal flush piping, entrained air would reach the internal bearings. However, due to the vertical orientation of the pump and the seal, the less dense entrained air entering from point A (See Fig 3) would rise up in the stuffing box outlet to
connection point B located above the seal faces and exit to the pump suction. Arrows (Fig 3)
show anticipated bubble flow path. 4.4 As long as the flush flow is above the critical flow, the possibility of air accumulation in the seal piping is not present. Also, stagnation or accumulation of air around the seal faces is unlikely due to the orientation of the seal and the location of the stuffing box outlet B. Therefore, due to
the above reasons the likelihood of the seals running dry is negligible. Task 5 - Non-Condensable Gases E12.5.1913 12x14x14.5 CVDS 6/8 [[ ]]Figure 2: Monticello - RHR Mechanical Seal Layout [[ ]]Figure 3: Mechanical Seal Connections Task 5 - Non-Condensable Gases E12.5.1913 12x14x14.5 CVDS 7/8 5.0RESULTS AND CONCLUSIONS Two methods; Froude Number and Critical Flow calculations indicate that air bubbles will not stagnate and accumulate in the seal piping. The vertical orientation of the pump and the location of the flush
inlet and outlet on the seal stuffing box significantly reduce the possibility of air accumulation in the
vicinity of the mechanical seals. Some of the concerns, regarding air entrainment in mechanical seals, raised in the NRC guidelines can be addressed through this report. a) Entrained air released due to NPSH margin reduction - As explained in this report, the vertical setup of the mechanical seal system will flush out the bubbles, and therefore, as long as a
minimum flow through the mechanical seal piping is maintained, the possibility of void fraction
accumulating at the seal faces is negligible. b) Use of Dual Mechanical Seals - For a vertical mechanical seal setup with seal flush outlet located at the top of the seal, dual mechanical seals with external flush system will not provide
an additional benefit. Vertical setup ensures constant flushing of the seal faces.c) Excessive entrained air centrifuged inward to the shaft - Forced lubricated bearings are located between the impeller inlet and the mechanical seals. This high pressure liquid will
prevent any bubbles to flow from the impeller inlet to the mechanical seal faces. Therefore, the entrained air that may be present in the suction line of the RHR pumps following a LOCA has no significant impact on the performance of the mechanical seals. Task 5 - Non-Condensable Gases E12.5.1913 12x14x14.5 CVDS 8/8 6.0 BIBLIOGRAPHY
[1]: Gas entrainment at a propagating slug front, Ruben Shulkes, Hydro Oil and Energy
[2]: Centrifugal Pumps, Johann Gulich, 2 nd Edition.
[3]: Centrifugal Pumps Book, Stepanoff.
[4]: Air in Water Pipes, A manual for designers of spring supplied gravity driven rural water delivery
system, Gilles Corcos, 2 nd Edition.
[5]: Froude Number, Wikipedia, http://en.wikipedia.org/wiki/Froude_number
[6]: Henry's Law Calculation.
http://www.engineeringtoolbox.com/air-solubility-water-d_639.html}}