Author:
Manh Vu D.,Le Duong T.,Nguyen Quan Q.,Pham Phuong X.,Nguyen Kien T.
Abstract
<div class="section abstract"><div class="htmlview paragraph">Jet impingement, one of the highly efficient heat exchange enhancement methods,
is commonly used to cool down the nozzle guide vanes (NGVs) of gas turbine
engines. This method normally generates a very high local heat transfer
coefficient (up to 1,000 ÷ 3,000 W/m<sup>2</sup>) due to the presence of a high
turbulent kinetic energy region and a laminar-to-turbulent transition zone
created by the jet. In the jet impingement system, the edge tip zone of a
turbine vane is often represented by cylindrical models, while flat plate models
are adopted for the midchord region. Due to interactions between the jet flow
and the initial cross flow at the midchord region, the local heat transfer
coefficient increases remarkably. The heat transfer coefficient can be
determined through computational fluid dynamics (CFD) simulation or experimental
approaches. Available experimental methods in the current literature include the
steady-state technique, transient liquid crystal thermography technique, and
temperature oscillation technique (TOIRT). In this article, a CFD model in
ANSYS-Fluent and a TOIRT experimental system were developed to determine the
heat transfer coefficient for a jet impingement tube with initial cross flow.
The numerical model was validated by experimental results obtained in this study
along with other data reported in the literature. The results show that the
cross flow increases the average and maximum heat transfer coefficients in the
jet impingement model. However, the cross flow also significantly changes the
direction of the jet flow and the position of the stagnation zone.</div></div>