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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 />

3.2 – ACHAB: <strong>Analysis</strong> <strong>Code</strong> <strong>for</strong> <strong>High</strong>-<strong>Altitude</strong> <strong>Balloons</strong><br />

The development of this model is essentially based on many results given in Ref. 9,<br />

Ref. 16, Ref. 17, Ref. 18, Ref. 20, Ref. 22, Ref. 26. We will start describing the<br />

dynamical model then the general geometric properties of the balloon and finally the<br />

thermal model.<br />

3.2.1 – Dynamical Model<br />

3.2.1.1 – Forces<br />

In order to write the 3D differential equations that describe the balloon dynamics, it<br />

is necessary to identify the <strong>for</strong>ces that act on the system. A rigorous analysis of all<br />

the <strong>for</strong>ces to which a balloon system is subjected during inflation, launch, and flight<br />

is beyond the scope and needs of this model; however, those of greatest importance<br />

<strong>for</strong> the description of the balloon motion are considered to be 9,16,17,20 :<br />

• net buoyancy<br />

• weight<br />

• aerodynamic drag<br />

Drag<br />

GI<br />

M gross<br />

V ˆ<br />

g<br />

Figure 3.2 – Forces acting on the balloon.<br />

Figure 3.2 shows the <strong>for</strong>ces acting on the balloon. The velocity vector is not oriented<br />

vertically because the model is 3-dimensional and takes into account wind<br />

disturbances.<br />

21

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