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Development of Heat Pipe Reactor Modeling in SAM

Guojun Hu, +2 more
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The article was published on 2019-06-01 and is currently open access. It has received 13 citations till now. The article focuses on the topics: Heat pipe.

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ANL/NSE-19/9
Development of Heat Pipe Reactor Modeling in SAM
Nuclear Science and Engineering Division

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prepared by
G. Hu, R. Hu, and L. Zou
Nuclear Science and Engineering Division, Argonne National Laboratory
June 2019
ANL-NSE-19/9
Development of Heat Pipe Reactor Modeling in SAM


Development of Heat Pipe Reactor Modeling in SAM
June 2019
i ANL-NSE-19/9
EXECUTIVE SUMMARY
System Analysis Module (SAM) is under development at Argonne National Laboratory as
a modern system-level modeling and simulation tool for advanced non-light water reactor safety
analyses. It utilizes the object-oriented application framework MOOSE to leverage the modern
software environment and advanced numerical methods available in PETSc. The capabilities
of SAM are being extended to enable the transient modeling, analysis, and design of various
advanced nuclear reactor systems. This report presents the development of new capabilities for
modeling the heat pipe type reactor systems.
The need for power at remote locations away from a reliable electrical grid is an important
niche for nuclear energy. Heat pipe-cooled fast-spectrum nuclear reactors are well suited for
these applications. The key feature of the heat pipe reactors is the use of heat pipes for heat
removal from the reactor core. The heat pipe makes use of the phase change of the working
fluid and transports a large amount of heat from the evaporator to the condensation end with
very small temperature drops. In contrast to the traditional nuclear reactor system that makes
use of pumped loop for extracting the thermal power, the heat pipe reactors make use of
hundreds of heat pipes for removing the thermal power (including the decay heat) passively.
This could potentially significantly improve the reliability and safety of the reactor systems.
The essential part in the analysis of a heat pipe type reactor is the modeling of heat transport
inside the heat pipe. The capability of SAM is extended in this work to enable the modeling of
the conventional heat pipe. Two alternative modeling options, 2D-RZ Heat conduction and 3D-
1D coupling, are developed, which are both based on the assumption that the heat pipe vapor
core can be modeled as a superconductor of extremely high thermal conductivity. Both
modeling options are verified with a simplified thermal resistance model. The heat pipes are
also coupled with the fuel region of a prototype micro reactor under both normal and off-normal
conditions. It is confirmed that both modeling options can correctly model the heat transport in
the heat-pipe reactors.

Citations
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Journal ArticleDOI

3D-2D coupling multi-dimension simulation for the heat pipe micro-reactor by MOOSE&SAM

TL;DR: A simulation is performed for the prototypical 37-heat-pipes test article to predict the thermal performance of the MAGNET facility under steady-state operation and several sensitivity parameters are analyzed to investigate their impact on facility thermal performance.
Journal ArticleDOI

Heat transfer analysis of heat pipe cooled device with thermoelectric generator for nuclear power application

TL;DR: In this paper , the ANSYS Fluent is used to perform thermal calculations on the heat pipe thermoelectric generator (HPTEG) prototype for both normal and accident conditions which include heat pipe failure and loss of heat sink accident conditions.
Journal ArticleDOI

A two-phase three-field modeling framework for heat pipe application in nuclear reactors

- 01 JanΒ 2022Β -Β 
TL;DR: In this article , a comprehensive one-dimensional two-phase three-field flow model has been developed for the analysis of heat pipes in normal operation conditions and transients, which is used in nuclear microreactors to remove fission power from the primary system.
Journal ArticleDOI

A two-phase three-field modeling framework for heat pipe application in nuclear reactors

TL;DR: In this article, a comprehensive one-dimensional three-field flow model has been developed for the analysis of heat pipes in normal operation conditions and transients for the liquid film, vapor, and droplet.
Journal ArticleDOI

Conceptualization of the Micro Research Reactor Cooled by Heat Pipes (MRR-HP), Part-I: neutronics analyses

TL;DR: The Micro Research Reactor cooled by Heat Pipes (MRR-HP) as mentioned in this paper is a 3D-detailed neutronics model using the Monte-Carlo Serpent-2.1.31 code.
References
More filters
Book

Heat Pipe Science And Technology

Amir Faghri
TL;DR: In this article, the authors present a detailed analysis of non-conventional heat pipe properties, including variable conductance heat pipes, and their properties in terms of heat transfer and mass transfer.
Journal ArticleDOI

MOOSE: A parallel computational framework for coupled systems of nonlinear equations

TL;DR: MOOSE as mentioned in this paper is a parallel computational framework targeted at solving coupled, nonlinear partial di?erential equations often arise in sim- ulation of nuclear processes, which is based on mathematics based on Jacobian-free Newton Krylov (JFNK).
ReportDOI

Thermodynamic and transport properties of sodium liquid and vapor

TL;DR: In this article, the authors present Russian recommendations and results of equation of state calculations on thermophysical properties of sodium have been included in this critical assessment, and their uncertainties are graphed and tabulated as functions of temperature.
Frequently Asked Questions (15)
Q1. What are the contributions mentioned in the paper "Development of heat pipe reactor modeling in sam" ?

In this paper, the authors presented the new heat pipe modeling capabilities of SAM in the analysis of a made-up heat pipe reactor.Β 

Since the vapor volume is fixed and the vapor density is usually small, the stability condition requires that the specific heat capacity is large enough.Β 

The thermal fluid phenomena in a heat pipe can be divided into four basic categories: 1) heat conduction in the heat pipe wall; 2) liquid flow and heat transfer in the wick structure; 3) interfacial mass, momentum, and energy transfer in the liquid vapor interface; and 4) vapor flow in the heat pipe core.Β 

The main approximation for modeling the heat pipe in SAM is that the vapor core can be modeled as a superconductor with a very large thermal conductivity.Β 

The advantages of using a heat pipe over other conventional methods include for example exceptional flexibility, simple construction, easy maintenance, and easy control with no external pumping power.Β 

Because of the increasing interests in heat-pipe type micro-reactors, the capability of SAM has been extended in this work to enable the modeling of the conventional heat pipe and the heat pipe type reactor.Β 

The boundary condition between the wick and the vapor core isπ‘žQ = β„Žn β‹… (𝑇Q βˆ’ 𝑇n) (2-10)where 𝑇Q and π‘žQ are the wall temperature and wall heat flux at the wick-vapor boundary, respectively.Β 

At the bottom and top end, the temperature gradient is zero, which represents that there is no heat loss from the bottom and top of the heat pipe.Β 

In general, the effective thermal conductivity of the vapor core has to be very large, e.g. 107 W/(m-K) is used in the verification tests.Β 

The overall condenser heat transfer capability is variable and thus provide a variable total conductance, which will control the operating temperature.Β 

The prediction shows that the failure of a single heat pipe causes a local peak in the fuel temperature, where the peaking factor is mainly determined by the inter-assembly heat transfer characteristic of the reactor.Β 

It should also be noted that the primary goal of the developed heat pipe modeling capability is to enable the transient safety analyses of the heat-pipe-type reactor systems, not to design a heat pipe.Β 

This process will continue as long as the capillary pressure is enough to drive the condensed working fluid back to the condenser region.Β 

The solution of the heat conduction equation in the 3D structure requires the vapor temperature while the solution of the vapor temperature equation requires the wall heat flux at the wick and vapor core boundaries.Β 

It is observed that the main parameters that governs stability condition is the total heat capacity of the vapor core, i.e. πœŒπ‘‰πΆo.Β