Physical Properties of Spermaceti Oil in the Sperm Whale
- 1 February 1978
- journal article
- research article
- Published by Cambridge University Press (CUP) in Journal of the Marine Biological Association of the United Kingdom
- Vol. 58 (1) , 19-26
- https://doi.org/10.1017/s0025315400024383
Abstract
This is the second of three papers describing the structure, properties and buoyancy function of the spermaceti organ of the sperm whale (Physeter macrocephalus Linnaeus 1758). The first paper (Clarke, 1978a) described the detailed structure and proportions of the spermaceti organ and related structures and considered relevant details of the blubber, skin and lungs. Here, three thermal properties of the spermaceti oil are described which are relevant to a study of the function of the oil. Finally, in a third paper (Clarke, 1978b) it will be shown that, over its great geographical and depth ranges, the whale varies considerably in buoyancy due to variations in water density and the volume of air in its lungs and it is suggested that, during dives, the whale can control its own density by changing the temperature of the spermaceti oil of the head and may attain neutral buoyancy in dives deeper than 200 m.This publication has 6 references indexed in Scilit:
- Buoyancy Control as a Function of the Spermaceti Organ in the Sperm WhaleJournal of the Marine Biological Association of the United Kingdom, 1978
- Structure and Proportions of the Spermaceti Organ in the Sperm WhaleJournal of the Marine Biological Association of the United Kingdom, 1978
- The lipid structure of the spermaceti organ of the sperm whale (Physeter catodon)Deep Sea Research and Oceanographic Abstracts, 1973
- An apparatus for accurate measurement of liquid densities over an extended temperature rangeJournal of Physics E: Scientific Instruments, 1970
- The Pressure-Volume-Temperature Properties of Fluorobenzene1Journal of the American Chemical Society, 1958
- The Apparatus and Method Used for the Measurement of the Compressibility of Several Gases in the Range 0° to 325° CProceedings of the American Academy of Arts and Sciences, 1934