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Annual Report

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port (RST) or Large Eddy Simulation (LES) models<br />

- have to be used to predict these corner<br />

zones where recirculation and corner vortices<br />

occur. In order to improve the degree of confidence<br />

with which these models can be used, it<br />

is essential to conduct experimental measurements<br />

in order to ensure that the assumptions<br />

inherent in these models are well-founded.<br />

It is possible to carry out very accurate measurements<br />

within experimental ducts by using<br />

transparent panels through which lasers can<br />

penetrate. Particle Tracking Velocimetry (PTV)<br />

or Particle Image Velocimetry (PIV) are modern<br />

measurement techniques that present considerable<br />

advantages over the more invasive Pitot<br />

Tube and Hot-wire Anemometry methods used<br />

in the past. The resolution in space and time<br />

that can be achieved is more than sufficient to<br />

capture the degree of detail needed to validate<br />

numerical simulations.<br />

Hybrid Methods for Thermal Hydraulic Analysis<br />

of Natural Circulation Environments<br />

Researcher: Morgan Cowper<br />

Supervisor: Dr Michael Bluck<br />

Sponsor: Rolls-Royce<br />

Thermal hydraulic analysis of nuclear reactors<br />

is largely performed with software known as<br />

“system codes”. As a crude but reasonably accurate<br />

shorthand, nuclear engineering systems<br />

codes model the desired scenario in the form<br />

of a series of 1D pipes , in which conservation<br />

equations for mass, momentum and energy are<br />

solved. For circumstances when this is a reasonable<br />

approximation, systems codes are remarkably<br />

effective, reflecting the very extensive<br />

development to which they have been subject<br />

over the past half-century. However, there are<br />

many circumstances in which the environment<br />

cannot adequately be represented as a piece of<br />

pipe and the detail cannot be covered by a 1D<br />

representation. CFD packages are capable of<br />

providing a detailed three-dimensional model<br />

of flow yet this comes at a great expense in the<br />

form of computational time.<br />

Therefore there is a growing interest in the<br />

technique of coupling of the two modelling systems;<br />

where a systems code can be used where<br />

it is adequate with the more detailed CFD being<br />

used where necessary. Although work has<br />

been done on this subject for a number of years<br />

it is still an embryonic aspect of computational<br />

physics and there is vast room for improvement<br />

and refining.<br />

Advanced Component-scale CFD Modelling of<br />

Nucleate Boiling<br />

Researcher: Ronak Thakrar<br />

Supervisor: Dr Simon Walker<br />

Sponsor: Rolls-Royce<br />

In a nuclear reactor, uncontrolled boiling can<br />

lead to the hazardous condition often referred<br />

to as the “critical heat flux” (or CHF) which can<br />

result in the fuel clad no longer being wetted<br />

and the integrity of the fuel being compromised;<br />

this condition defines the upper limit<br />

for safe reactor operation and therefore there<br />

is an essential requirement for the engineering<br />

capability to predict the onset of this condition<br />

(and hence to accurately predict the behaviour<br />

of boiling flows). Today’s state-of-the-art<br />

in boiling modelling in CFD embodies a significant<br />

degree of empiricism by way of using<br />

correlations to define the overwhelming majority<br />

of closure terms in the modelling formulation.<br />

In addition to this, the formulation is itself<br />

unrepresentative of the many interacting heat<br />

transfer mechanisms at work during the boiling<br />

process. These factors impose an upper<br />

bound on the predictive capability (and range<br />

of application) of the CFD code, which limits its<br />

Centre for Nuclear Engineering <strong>Annual</strong> <strong>Report</strong> 2014-2016 44

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