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Review on effect of two-phase interface morphology evolution on flow and heat transfer characteristics in confined channel

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Abstract

In this paper, the effect of two-phase interface morphology evolution on the flow and heat transfer characteristics in confined channels are reviewed in detail, which is one of the typical channel structures for the nuclear reactor core. The investigated contents mainly come from the open literature. In addition, this paper focuses on the important phenomena and methods proposed in recent decades, which simultaneously includes the closely related studies of authors published in the last several years. The primary contents of this paper mainly includes the following aspects: (1) the definition of confined channel is introduced based on the summary of various distinguishing criterions; (2) the effect of two-phase interface morphology on the flow and resistance characteristics is concluded, which are mainly related to the adiabatic flow conditions, thus the complex influence of boiling phenomenon can be neglected; (3) the effect of two-phase interface morphology on the flow boiling heat transfer characteristics is researched. Moreover, the development of flow boiling heat transfer model is reviewed, and the corresponding proposed model is introduced, which innovatively reflects the feature of confined channel and is considered worthy of further development; (4) the effect of two-phase interface morphology on the flow instability and boiling crisis characteristics are reviewed. Especially, the coupling relationship between them are introduced with the bubble dynamic behaviors dependent on the published research achievement of authors; (5) the material surface modification technology is proposed to be the enhanced heat transfer technology, which is also supposed to be the future research point for reactor thermal-hydraulics.

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Abbreviations

a :

Constant

b :

Constant

c :

Constant

c p :

Specific heat capacity (J/kgK)

d :

Constant

e :

Constant

f :

Friction coefficient

g :

Gravitational acceleration (m/s2)

h :

Heat transfer coefficient (W/m2K)

k :

Thermal conductivity (W/mK)

m :

Mass flow rate (kg/s)

n :

Constant

p :

Pressure (Pa)

Δp :

Pressure drop (Pa)

Δp sat :

Vapor pressure drop dependent on ΔTsat (Pa)

q :

Heat flux (W/m2)

r :

Radius (m)

t :

Time (s)

u :

Velocity (m/s)

x e :

Quality

A :

Cross-section area (m2)

D :

Diameter (m)

F:

Enhancement factor

G :

Mass flux (kg/m2s)

H :

Enthalpy (J/kg)

H fg :

Latent heat of vaporization (J/kg)

L :

Length (m)

M :

Molecular weight

N conf :

Confinement coefficient

N sub :

Subcooling number

N pch :

Phase change number

P:

Perimeter (m)

Q :

Volume flow rate (mL/s)

S:

Suppression factor

T :

Temperature (°C)

ΔT sat :

Superheat (K)

X tt :

Martinelli number

Bo:

Boiling number

Bond:

Bond number

Ca:

Capillary number

Fr:

Froude number

Ja:

Jacobs number

Pr:

Prandtl number

Re:

Reynolds number

We:

Weber number

α :

Constant

β :

Constant

γ :

Constant

ε :

Percentage

η :

Laplace pressure drop coefficient

λ:

Inverse Gaussian distribution parameter

μ :

Dynamic viscosity (Pa·s)

ν :

Inverse Gaussian distribution parameter

ρ :

Density (kg/m3)

σ :

Surface tension (N/m)

τ :

Shear stress (N/m2)

Γ :

Two-phase multiplication factor

Θ :

Dimensionless parameter

λ:

Inverse Gaussian distribution parameter

ν :

Inverse Gaussian distribution parameter

b:

Bubble

bulk:

Bulk flow

c:

Contact

cr:

Critical

ch:

Channel

drop:

Flow pressure drop

diff:

Total pressure drop

en:

Environment

exp:

Experiment

fc:

Forced convention

g:

Gas/Vapor

h:

Hydraulic diameter

i:

Number

in:

Inner

l :

Liquid-phase

m:

Mixture

os:

Onset of flow instability

pb:

Pool boiling

pre:

Prediction

sat:

Saturation

sub:

Subcooling

tp:

Two-phase

tot:

Total

F:

Friction pressure drop

G:

Gravity pressure drop

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The authors are grateful for the support of the National Natural Science Foundation of China (No. 11905212).

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Deng, J., Lu, Q., Liu, Y. et al. Review on effect of two-phase interface morphology evolution on flow and heat transfer characteristics in confined channel. Heat Mass Transfer 57, 13–39 (2021). https://doi.org/10.1007/s00231-020-02932-8

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