Oceans '78 1978
DOI: 10.1109/oceans.1978.1151111
|View full text |Cite
|
Sign up to set email alerts
|

Development of a Small In-Situ Conductivity Instrument

Abstract: The instrument was originally developed by the Applied Physics Laboratory, University of Washing-The initial development and testing of a small ton,+ and is now commercially available from Seain-situ conductivity instrument was reported at Bird Electronics (under license from the University OCEAN 73.l Since then, extensive operational ex-of Washington) as Model SBE-4 ( Figure 1).perience has been obtained with a number of these instruments an moorings and on free and tethered ~ ~~~ ~~ . = ~~ ~ ~ ~ platforms … Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1

Citation Types

0
2
0

Year Published

1988
1988
2023
2023

Publication Types

Select...
1
1

Relationship

0
2

Authors

Journals

citations
Cited by 2 publications
(2 citation statements)
references
References 6 publications
0
2
0
Order By: Relevance
“…The transmission sensor voltage was measured for about 0.1 sec in the center of the VACM sampling interval. Conductivity was measured by means of a Sea Bird Inc. conductivity sensor (Peterson and Gregg, 1979). Output of the sensor was averaged for 1.875 sec in the center of the VACM sampling interval.…”
Section: Vector-averaging Current Metermentioning
confidence: 99%
“…The transmission sensor voltage was measured for about 0.1 sec in the center of the VACM sampling interval. Conductivity was measured by means of a Sea Bird Inc. conductivity sensor (Peterson and Gregg, 1979). Output of the sensor was averaged for 1.875 sec in the center of the VACM sampling interval.…”
Section: Vector-averaging Current Metermentioning
confidence: 99%
“…SBE build standard CTD instruments which produce measurements that are high in both precision and accuracy. The conductivity measurement is performed in a cylindrical glass cell with a volume of 1.51 cm 3 containing three electrodes which ensures that the measurement is only affected by the volume within the cell (Gregg & Hess, 1985; Pederson, 1973; Pederson & Gregg, 1979). To be precise, the cell measures resistance, R cell , which is converted to the conductivity of the water, σ , by taking into account the cell geometry: Rcell=ρlA=lAσ ${R}_{\mathit{cell}}=\frac{\rho l}{A}=\frac{l}{A\sigma }$ with ρ=1σ $\rho =\frac{1}{\sigma }$ the resistivity of the water, l the effective length of the conductivity cell (which depends on cell length and water velocity though the cell), and A the cross‐sectional area of the sampled water.…”
Section: Introductionmentioning
confidence: 99%