Eotvos (unit)
eotvos | |
---|---|
Unit system | Non-SI metric unit |
Unit of | Linear acceleration density |
Symbol | E |
Named after | Loránd Eötvös |
Derivation | 10−9 Gal/cm |
Conversions | |
1 E in ... | ... is equal to ... |
CGS base units | 10−9 s−2 |
SI base units | 10−9 s−2 |
The eotvos is a unit of acceleration divided by distance that was used in conjunction with the older centimetre–gram–second system of units (cgs). The eotvos is defined as 10−9 galileos per centimetre. The symbol of the eotvos unit is E.[1][2]
In SI units and in CGS units, 1 eotvos = 10−9 second−2.[3]
The gravitational gradient of the Earth, that is, the change in the gravitational acceleration vector from one point on the Earth's surface to another, is customarily measured in units of eotvos.
The eotvos unit is named for the physicist Loránd Eötvös, who made pioneering studies of the gradient of the Earth's gravitational field.[4]
Static sources
In free space, the gravitational gradient tensor has trace 0 by Poisson's equation, so the sum of gravity gradient along any 3 perpendicular directions is 0.
Near the surface of earth, the equipotential surface is nearly spherical, following the near-spherical shape of earth. Thus, the gravity gradient tensor has its 3 principal directions: a tensile direction along the local vertical direction, and 2 compressive directions perpendicular to the local vertical direction. The vertical tensile component gradient is ~3,080 E (an elevation increase of 1 m gives a decrease of gravity of about 0.3 mGal). For a perfectly spherical earth, this value is theoretically . Since the equipotential surface is nearly spherical, the two compressive gradients are roughly 1/2 of that, at ~1,540 E. Gravity gradiometry usually measures the perturbation away from this ideal value.
The effect of Earth's rotation creates an acceleration value of , where is its angular velocity, and is the latitude. This perturbs the measured gradient. The maximal perturbation is obtained at the equator, with a value of .
Geological formations can modify the gradient. A mountain range, or an underground formation with increased density, is a large amount of mass that increases the tensile component of the gradient, and tilts the direction of tensile component towards the mass. An underground formation of decreased density, such as a salt dome or an oil formation, has the opposite effect.
In general, the gradiometric perturbation of a structure falls off as , so a structure of characteristic size buried underground produces roughly the same amount of perturbation at the ground surface as a structure of characteristic size buried , for any .
Type of structure | Effect size (in E) | Reference |
---|---|---|
Earth's rotation | ~5 | theory |
Mountain ranges | ~200 | [5] |
shallow Texas salt domes | 50--100 | [5] |
aquifer, soil moisture, soil compaction | ~30 | [6] |
buildings, archeological sites | <100 | [6] |
a square 2×2 m pipe buried 0.5 m underground | ~150 | [6] |
Measurement
The Eötvös torsion balance was used in the exploration for oil and gas reservoirs during 1918–1940 period. It could achieve 1–3 E in accuracy, but requires up to 6 h per station.[7] Modern (2013) airborne systems can reach 3–6 E in rms accuracy at integration time of ~6 seconds. Such a system achieves higher spatial resolution on slower aircrafts, so the gradiometry maps have higher spatial resolution on the zeppelin and the helicopter than a fixed-wing aircraft. Spatial resolution is also higher for lower-flying aircrafts.[8]
Year | Type of instrument | Reading time | Sensitivity (in E) | Reference |
---|---|---|---|---|
1918–1940 | Eötvös torsion balance | 6 hours | 1–3 | [7] |
2012 | airborne systems | 6 seconds | 3–6 | [8] |
2022 | matter wave Mach–Zehnder interferometry | 10 minutes | 20 | [6] |
See also
References
- ^ "Basic measurement units / GOCE / Earth Explorers / The Living Planet Programme / Observing the Earth / Our Activities / ESA". Archived from the original on 14 March 2018. Retrieved 11 December 2016.
- ^ Glossary of the mapping sciences. American Society of Civil Engineers, American Congress on Surveying and Mapping, American Society for Photogrammetry and Remote Sensing. New York, NY: American Society of Civil Engineers. 1994. p. 177. ISBN 0784400504. OCLC 30893371.
{{cite book}}
: CS1 maint: others (link) - ^ "Gravity in detail – Content – Earth Online – ESA". earth.esa.int. Retrieved 26 September 2019.
- ^ Adelberger, E. G.; Heckel, B. R.; Smith, G.; Su, Y.; Swanson, H. E. (1990). "Eötvös experiments, lunar ranging and the strong equivalence principle". Nature. 347 (6290): 261–263. Bibcode:1990Natur.347..261A. doi:10.1038/347261a0. ISSN 1476-4687. S2CID 4286881.
- ^ a b Bell, Robin E.; Anderson, Roger; Pratson, Lincoln (January 1997). "Gravity gradiometry resurfaces". The Leading Edge. 16 (1): 55–59. Bibcode:1997LeaEd..16...55B. doi:10.1190/1.1437431. ISSN 1070-485X.
- ^ a b c d Stray, Ben; Lamb, Andrew; Kaushik, Aisha; Vovrosh, Jamie; Rodgers, Anthony; Winch, Jonathan; Hayati, Farzad; Boddice, Daniel; Stabrawa, Artur; Niggebaum, Alexander; Langlois, Mehdi; Lien, Yu-Hung; Lellouch, Samuel; Roshanmanesh, Sanaz; Ridley, Kevin (February 2022). "Quantum sensing for gravity cartography". Nature. 602 (7898): 590–594. Bibcode:2022Natur.602..590S. doi:10.1038/s41586-021-04315-3. ISSN 1476-4687. PMC 8866129. PMID 35197616.
- ^ a b Jekeli, Christopher (2011), "Gravity, Gradiometry", Encyclopedia of Solid Earth Geophysics, Encyclopedia of Earth Sciences Series, Springer, Dordrecht, pp. 547–561, doi:10.1007/978-90-481-8702-7_80, ISBN 978-90-481-8702-7
- ^ a b Dransfield, Mark H.; Christensen, Asbjorn N. (August 2013). "Performance of airborne gravity gradiometers". The Leading Edge. 32 (8): 908–922. Bibcode:2013LeaEd..32..908D. doi:10.1190/tle32080908.1. ISSN 1070-485X.