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petebachant avatar petebachant commented on May 18, 2024

Also see Dyachuk and Goude (2015): http://dx.doi.org/10.3390/en8021353.

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petebachant avatar petebachant commented on May 18, 2024

This is effectively implemented, but a 0.5 chord mount is hard-coded in. We could create a list from the turbine element geometry and pass this into the actuator line dictionaries, which then pass the values into the elements.

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petebachant avatar petebachant commented on May 18, 2024

Fixed the implementation of this in df36d7e, and it looks way wrong now.

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petebachant avatar petebachant commented on May 18, 2024

May need to reevaluate which model to use. Niblick (2012) describes a correction by Mandal and Burton (1994) that seems reasonable:

image

This could be implemented by adding new members for the leading and trailing edge velocity vectors for each element.

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petebachant avatar petebachant commented on May 18, 2024

From Strickland et al.'s report on VDART3:

image

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petebachant avatar petebachant commented on May 18, 2024

And from Murray and Barone (2011) on CACTUS:

image

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petebachant avatar petebachant commented on May 18, 2024

Bjorck (2000) uses this relation for dealing with the pitch rate:

image

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petebachant avatar petebachant commented on May 18, 2024

Need to add this to the fvOptions dictionary for a turbine source, allowing for selecting different models, deactivating, etc.

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petebachant avatar petebachant commented on May 18, 2024

Going to close this for now since both the Goude and MandalBurton models are implemented. May need to open another later after thoroughly testing their accuracy.

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