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Analysis Code for High Altitude Balloons - FedOA - Università degli ...

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ACHAB: <strong>Analysis</strong> <strong>Code</strong> <strong>for</strong> <strong>High</strong> <strong>Altitude</strong> <strong>Balloons</strong> Chapter 3<br />

For free convection between the external skin and the air the following <strong>for</strong>mulation<br />

of the Nusselt number is considered:<br />

Nu =<br />

free<br />

HC<br />

free<br />

Diameter<br />

Nusselt numbers <strong>for</strong> free convection problems are usually correlated to Rayleigh<br />

numbers. The general <strong>for</strong>m is:<br />

k<br />

air<br />

Nu a0<br />

a1Ra<br />

+ =<br />

where Rayleigh number is the product of the Grashof number and Prandtl number<br />

( Ra = GrPr ), and 0 a , a 1 and n are usually determined experimentally.<br />

The Nusselt number used in this model is taken from Ref. 9, 17, 18, 20. The Grashof<br />

number <strong>for</strong> air Gr air is defined as:<br />

Gr<br />

External Forced Convection.<br />

air<br />

2<br />

ρ air g T film − Tair<br />

Diameter<br />

=<br />

T µ<br />

This kind of convection depends on the vertical velocity of the balloon that <strong>for</strong>ces the<br />

relative movement of air with respect to the external skin.<br />

The <strong>for</strong>mulations of the Nusselt number ( Nu <strong>for</strong>ced ) <strong>for</strong> external <strong>for</strong>ced convection<br />

used in this model are those reported in Ref. 9, 18, 20.<br />

Hence, this yields to the following coefficient:<br />

air<br />

2<br />

air<br />

kair<br />

HC <strong>for</strong>ced =<br />

Nu<br />

Diameter<br />

n<br />

<strong>for</strong>ced<br />

3<br />

39

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