A source of hydrogen is needed in the developing hydrogen economy, and many technologies are available for producing hydrogen from both conventional and alternative energy resources such as natural gas, coal, atoms, sunlight, wind, and biomass. The following paper summarizes the economics of produci
A comparison of hydrogen with alternate energy forms from coal and nuclear energy
โ Scribed by Kenneth E. Cox
- Publisher
- Elsevier Science
- Year
- 1976
- Weight
- 529 KB
- Volume
- 16
- Category
- Article
- ISSN
- 0013-7480
No coin nor oath required. For personal study only.
โฆ Synopsis
Alternate energy forms that can be produced from coal and nuclear energy have been analyzed on effmiency, economic and end-use grounds. These forms include hydrogen, methane, electricity, and EVA-ADAM, a "chemical heat-pipe" approach to energy transmission.
The EVA-ADAM system for nuclear heat appears to be economically competitive with the other energy carriers except over very large distances. The cost of hydrogen derived from coal is approximately equal to that of methane derived from the same source when compared on an equal BTU basis. Thermochemically derived hydrogen from nuclear energy shows a break-even range with hydrogen derived from coal at coal costs of from $33-80/ton depending on the cost of nuclear heat. Electricity and electrolytically derived hydrogen are the most expensive energy carriers and electricity's use should be limited to applications involving work rather than heat.
Continued work in thermochemical hydrogen production schemes should be supported as an energy option for the future.
๐ SIMILAR VOLUMES
02 Liquid fuels (transport, refining, quality, storage) generated and released into the free fraction with apparent epimerization occurring at C-17, C-21, and C-22. The bound hopanoic acids may be both chemically bonded as well as possibly being physically encapsulated within the macromolecular frac
50% of the NO, emissions was obtained during the tests at a Ca/S ratio of -1. The optimum temperature for BioLime injection was found to be between 2000-2050ยฐF. The BioLime atomization air pressure was varied from 20 to 100 psig and the optimum pressure was found to be 50-60 psig. Influencing the r
The infrared chcmilumincscenco arising from the hydrogen abstraction reactions of ELuorinc atoms with 1120, H2S. Ii202 snd CH4 was investignted et low pressure in n ilow apparatus. Emission was found only from the HF product. The rclotive RF vibrational populations were determined under conditions w