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Title: StingRAY H1 Humboldt Cost Breakdown Structure

Abstract

Columbia Power LCOE (levelized cost of energy) Model for the Stingray H1 at the DOE Reference Site of Humboldt, CA. The model is integrated with and reports LCOE from DOE Cost Breakdown Structure

Authors:
Publication Date:
Other Number(s):
194
DOE Contract Number:  
EE0007347
Research Org.:
Marine and Hydrokinetic Data Repository (MHKDR); Columbia Power Technologies, Inc.
Sponsoring Org.:
USDOE Office of Energy Efficiency and Renewable Energy (EERE), Wind and Water Technologies Office (EE-4W)
Collaborations:
Columbia Power Technologies, Inc.
Subject:
16 Tidal and Wave Power
Keywords:
MHK; Marine; Hydrokinetic; energy; power; Humboldt; CA; USA; LCOE; WEC; wave energy; Wave Energy Converter; stingray; H1; cwpr; wave; levelized cost of energy; Columbia Power Technologies; point; absorber; economics; cost
Geolocation:
41.14288548653,-124.07680874023|40.493126959856,-124.07680874023|40.493126959856,-124.91441508789|41.14288548653,-124.91441508789|41.14288548653,-124.07680874023
OSTI Identifier:
1415571
DOI:
https://doi.org/10.15473/1415571
Project Location:


Citation Formats

Rhinefrank, Ken. StingRAY H1 Humboldt Cost Breakdown Structure. United States: N. p., 2017. Web. doi:10.15473/1415571.
Rhinefrank, Ken. StingRAY H1 Humboldt Cost Breakdown Structure. United States. doi:https://doi.org/10.15473/1415571
Rhinefrank, Ken. 2017. "StingRAY H1 Humboldt Cost Breakdown Structure". United States. doi:https://doi.org/10.15473/1415571. https://www.osti.gov/servlets/purl/1415571. Pub date:Mon Mar 06 00:00:00 EST 2017
@article{osti_1415571,
title = {StingRAY H1 Humboldt Cost Breakdown Structure},
author = {Rhinefrank, Ken},
abstractNote = {Columbia Power LCOE (levelized cost of energy) Model for the Stingray H1 at the DOE Reference Site of Humboldt, CA. The model is integrated with and reports LCOE from DOE Cost Breakdown Structure},
doi = {10.15473/1415571},
journal = {},
number = ,
volume = ,
place = {United States},
year = {Mon Mar 06 00:00:00 EST 2017},
month = {Mon Mar 06 00:00:00 EST 2017}
}