Abstract
A computer program was written to calculate void-fraction, flow rate, system circulation time and pressure drops for SIDAS under natural circulation conditions. In this program the thermohydraulic behaviour of the loop is simulated. Taking into account for the large uncertainty in two-phase frictional pressure drops, the chimney length is calculated, together with the length of the tubes which connect the downcomer at assembly height with the assembly inlet in a roundabout way. Tube diameter is chosen such that the frictional pressure losses are negligible. Using the results, it was decided to construct the chimney `telescopically` (consisting of a fixed part and a movable part) in order to influence the driving force. Calculations of the enthalpy of the condensed vapour flow for various system conditions have shown that it is impractical to use this flow to lower the temperature of the total downcomer flow at the necessary subcooling temperature. It is therefore decided to use the condensor flow only for lowering the total downcomer flow enthalpy at saturation enthalpy and to establish the necessary subcooling separately by cooling of the flow in the connecting tubes. (orig.).
Citation Formats
Graaf, R van de.
SImulated Dodewaard ASsembly: Developments in loop-design.
Netherlands: N. p.,
1992.
Web.
Graaf, R van de.
SImulated Dodewaard ASsembly: Developments in loop-design.
Netherlands.
Graaf, R van de.
1992.
"SImulated Dodewaard ASsembly: Developments in loop-design."
Netherlands.
@misc{etde_217559,
title = {SImulated Dodewaard ASsembly: Developments in loop-design}
author = {Graaf, R van de}
abstractNote = {A computer program was written to calculate void-fraction, flow rate, system circulation time and pressure drops for SIDAS under natural circulation conditions. In this program the thermohydraulic behaviour of the loop is simulated. Taking into account for the large uncertainty in two-phase frictional pressure drops, the chimney length is calculated, together with the length of the tubes which connect the downcomer at assembly height with the assembly inlet in a roundabout way. Tube diameter is chosen such that the frictional pressure losses are negligible. Using the results, it was decided to construct the chimney `telescopically` (consisting of a fixed part and a movable part) in order to influence the driving force. Calculations of the enthalpy of the condensed vapour flow for various system conditions have shown that it is impractical to use this flow to lower the temperature of the total downcomer flow at the necessary subcooling temperature. It is therefore decided to use the condensor flow only for lowering the total downcomer flow enthalpy at saturation enthalpy and to establish the necessary subcooling separately by cooling of the flow in the connecting tubes. (orig.).}
place = {Netherlands}
year = {1992}
month = {Mar}
}
title = {SImulated Dodewaard ASsembly: Developments in loop-design}
author = {Graaf, R van de}
abstractNote = {A computer program was written to calculate void-fraction, flow rate, system circulation time and pressure drops for SIDAS under natural circulation conditions. In this program the thermohydraulic behaviour of the loop is simulated. Taking into account for the large uncertainty in two-phase frictional pressure drops, the chimney length is calculated, together with the length of the tubes which connect the downcomer at assembly height with the assembly inlet in a roundabout way. Tube diameter is chosen such that the frictional pressure losses are negligible. Using the results, it was decided to construct the chimney `telescopically` (consisting of a fixed part and a movable part) in order to influence the driving force. Calculations of the enthalpy of the condensed vapour flow for various system conditions have shown that it is impractical to use this flow to lower the temperature of the total downcomer flow at the necessary subcooling temperature. It is therefore decided to use the condensor flow only for lowering the total downcomer flow enthalpy at saturation enthalpy and to establish the necessary subcooling separately by cooling of the flow in the connecting tubes. (orig.).}
place = {Netherlands}
year = {1992}
month = {Mar}
}