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Experimental Study on the Effect of Initial Temperature on CHF in a Vertical Annulus Narrow Channel with Bilateral Heated

Atom Indonesia · Vol. 37 No. 2 (2011) · hlm. 45–51

DOI
10.17146/aij.2011.61
ISSN
2356-5322, 0126-1568
Terbit
2011-12-22
Penerbit
National Research and Innovation Agency
Bahasa
eng
Lisensi
creativecommons.org/licenses/by-nc-sa/4.0

Abstrak

Study on understanding of the complexities of boiling in the narrow channel which was occured in a severe accident on nuclear power plant has been carried out in experimentally using simulation apparatus in order to achieve the safety management capability. Critical Heat Flux (CHF) is one important parameter to control heat during transient accident. The methodology of research is an experiment using experiment apparatus called HeaTiNG-01 test section with modifications in the outside pipe using stainless steel material as the reactor vessel wall simulation. Experiments were conducted by heating the heated rod as a simulation of debris until the desired initial temperature by bilateral heated. Then water with a saturation temperature in atmospheric was poured gravitationally into the narrow channel. Data acquisition system recorded temperature changes in transient during the cooling process. The transient temperature profile in double heating surface and rewetting point (rewet fronts) was characterized. Experiment was conducted at three initial temperature variations i.e. 650oC, 750oC and 850oC and using channel width 1 mm. Experiment data was used to calculate heat flux then to fitting CHF form boiling curve. The results showed that CHF in outer pipe is higher than heated rod, these conditions explain that more heat is released through the outer pipe, so that the heat control can be done from outside the system to reduce the temperature quickly. The average value of CHF for each vertical position 100 mm and 400 mm at outer pipe are 380 kW/m2 and 733 kW/m2, and then at the heated rod are 250 kW/m2 and 497 kW/m2. Received: 20 November 2010; Revised: 25 July 2011; Accepted: 08 August 2011

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  • National Nuclear Energy Agency of Indonesia
  • Universitas Gadjah Mada
  • National Research and Innovation Agency
  • University of Indonesia
  • University of Technology Sydney
  • Udayana University
  • Research Organization for Nuclear Energy
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Rekan penulisOrganisasiArtikel bersama
Anhar Riza AntariksawanNational Nuclear Energy Agency of Indonesia4
Putut Hery SetiawanNational Research and Innovation Agency3
Sri IsmarwantiNational Nuclear Energy Agency of Indonesia3
Mukhsinun Hadi KusumaNational Nuclear Energy Agency of Indonesia3
Tanti ArdiyatiNational Nuclear Energy Agency of Indonesia3
T.M.I. MahliaUniversity of Technology Sydney3
Deendarlianto DeendarliantoUniversitas Gadjah Mada3
Julwan Hendry PurbaNational Nuclear Energy Agency of Indonesia2
Surip WidodoNational Nuclear Energy Agency of Indonesia2
Arif Adtyas BudimanNational Research and Innovation Agency2
Ainur RosidiNational Nuclear Energy Agency of Indonesia2
Wayan Nata SeptiadiUdayana University2
Irwin Pratama PutraUniversity of Indonesia2
Ranggi SahmuraUniversity of Indonesia2
P W JokoNational Nuclear Energy Agency of Indonesia1
H IsmuNational Nuclear Energy Agency of Indonesia1
Edy SNational Nuclear Energy Agency of Indonesia1
Kiswanta KiswantaNational Nuclear Energy Agency of Indonesia1
D. HaryantoNational Nuclear Energy Agency of Indonesia1
J.P. WitokoNational Nuclear Energy Agency of Indonesia1
GI GiarnoNational Nuclear Energy Agency of Indonesia1
E. P. AristaUniversitas Gadjah Mada1
A. S. Al-aminUniversitas Gadjah Mada1
Hyundianto Arif GunawanNational Research and Innovation Agency1
Dewanto SaptoadiUniversity of Indonesia1
S. A. MariyadiAfiliasi tidak diketahui1
Nur Rochman BudiyantoUniversitas Gadjah Mada1
Dwi YuliajiUniversitas Gadjah Mada1
Ryan OktaviandiUniversitas Gadjah Mada1
Esa Putra Ariesta RaharjoUniversitas Gadjah Mada1
Adhika Enggar PamungkasResearch Organization for Nuclear Energy1
Topan SetiadipuraNational Nuclear Energy Agency of Indonesia1
H.M. KusumaNational Nuclear Energy Agency of Indonesia1
Hendro TjahjonoNational Research and Innovation Agency1
Pricylia ValentinaNational Research and Innovation Agency1

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Sumber metadata: OAI-PMH (metadata jurnal) https://atomindonesia.brin.go.id/index.php/aij/oai, pertama di-harvest 8 Nov 2026, terakhir terlihat 8 Nov 2026.
Metadata asli (oai_dc)
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	<dc:title xml:lang="en-US">Experimental Study on the Effect of Initial Temperature on CHF in a Vertical Annulus Narrow Channel with Bilateral Heated</dc:title>
	<dc:creator>Juarsa, M.</dc:creator>
	<dc:creator>Koestoer, RA.</dc:creator>
	<dc:creator>Putra, N.</dc:creator>
	<dc:creator>Indarto, Indarto</dc:creator>
	<dc:creator>Habsari, S.</dc:creator>
	<dc:subject xml:lang="en-US">Bilateral; Boiling curve; CHF; Temperature</dc:subject>
	<dc:description xml:lang="en-US">Study on understanding of the complexities of boiling in the narrow channel which was occured in a severe accident on nuclear power plant has been carried out in experimentally using simulation apparatus in order to achieve the safety management capability. Critical Heat Flux (CHF) is one important parameter to control heat during transient accident. The methodology of research is an experiment using experiment apparatus called HeaTiNG-01 test section with modifications in the outside pipe using stainless steel material as the reactor vessel wall simulation. Experiments were conducted by heating the heated rod as a simulation of debris until the desired initial temperature by bilateral heated. Then water with a saturation temperature in atmospheric was poured gravitationally into the narrow channel. Data acquisition system recorded temperature changes in transient during the cooling process. The transient temperature profile in double heating surface and rewetting point (rewet fronts) was characterized. Experiment was conducted at three initial temperature variations i.e. 650oC, 750oC and 850oC and using channel width 1 mm. Experiment data was used to calculate heat flux then to fitting CHF form boiling curve. The results showed that CHF in outer pipe is higher than heated rod, these conditions explain that more heat is released through the outer pipe, so that the heat control can be done from outside the system to reduce the temperature quickly. The average value of CHF for each vertical position 100 mm and 400 mm at outer pipe are 380 kW/m2 and 733 kW/m2, and then at the heated rod are 250 kW/m2 and 497 kW/m2. Received: 20 November 2010; Revised: 25 July 2011; Accepted: 08 August 2011 </dc:description>
	<dc:publisher xml:lang="en-US">National Research and Innovation Agency</dc:publisher>
	<dc:contributor xml:lang="en-US">National Nuclear Energy Agency of Indonesia</dc:contributor>
	<dc:date>2011-12-22</dc:date>
	<dc:type>info:eu-repo/semantics/article</dc:type>
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	<dc:format>application/pdf</dc:format>
	<dc:identifier>https://atomindonesia.brin.go.id/index.php/aij/article/view/61</dc:identifier>
	<dc:identifier>10.17146/aij.2011.61</dc:identifier>
	<dc:source xml:lang="en-US">Atom Indonesia; Vol 37, No 2 (2011): August 2011; 45-51</dc:source>
	<dc:source>2356-5322</dc:source>
	<dc:source>0126-1568</dc:source>
	<dc:source>10.17146/aij.2011.%x</dc:source>
	<dc:language>eng</dc:language>
	<dc:relation>https://atomindonesia.brin.go.id/index.php/aij/article/view/61/40</dc:relation>
	<dc:rights xml:lang="en-US">Copyright (c) 2016 Atom Indonesia</dc:rights>
	<dc:rights xml:lang="en-US">http://creativecommons.org/licenses/by-nc-sa/4.0</dc:rights>
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