2. Benchmark solution#

2.1. Calculation method#

Air mass conservation calculation

The conservation of the mass of gas is written as:

_images/Object_14.svg

eq 2.1.1-1

We write that the total mass of water and the total mass of air are preserved (because there is no water or gas flow at the edge) and we get:

_images/Object_15.svg

therefore

_images/Object_16.svg

Eq 2.1.1-2

_images/Object_17.svg

and

_images/Object_18.svg _images/Object_19.svg

Speed calculation:

_images/Object_20.svg

Eq 2.1.1-3

since

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and

_images/Object_22.svg

and

_images/Object_23.svg

with

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Like

_images/Object_25.svg _images/Object_26.svg

[éq 2.1.1-1] can then be simplified to the following form:

_images/Object_27.svg

with

_images/Object_28.svg

Heat equation that is treated by an Aster thermal calculation.

2.2. Benchmark results#

With the previous numerical values, we find:

_images/Object_29.svg _images/Object_30.svg

and

_images/Object_31.svg _images/Object_32.svg

The constants of the heat equation are then:

_images/Object_33.svg

2.3. Uncertainty about the solution#

The uncertainties are quite large since the quasi-analytical solution (the result of a thermal calculation) is an approximate solution due to the linearization of the equations.