1985
DOI: 10.1175/1520-0426(1985)002<0304:drcosb>2.0.co;2
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Dynamic Response Calibration of Sea-Bird Temperature and Conductivity Probes

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Cited by 26 publications
(10 citation statements)
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“…This has been shown by many prior investigations to be mainly due to misalignment of the temperature and conductivity measurements due to physical separation of the thermistor and the conductivity cell, as well as to mismatches between the response times of the two sensors (Horne and Toole 1980;Gregg and Hess 1985). With pumped CTD systems such as the commonly used SBE 911, where the flow through the T/C duct is constant, the proper alignment is easily achieved by advancing conductivity in time by a fixed amount.…”
Section: Introductionmentioning
confidence: 99%
“…This has been shown by many prior investigations to be mainly due to misalignment of the temperature and conductivity measurements due to physical separation of the thermistor and the conductivity cell, as well as to mismatches between the response times of the two sensors (Horne and Toole 1980;Gregg and Hess 1985). With pumped CTD systems such as the commonly used SBE 911, where the flow through the T/C duct is constant, the proper alignment is easily achieved by advancing conductivity in time by a fixed amount.…”
Section: Introductionmentioning
confidence: 99%
“…Temperature is measured with a pressure-protected, fast-response thermistor mounted near the duct intake, while conductivity is sensed inside a long, narrow, three-electrode cell located downstream of the intake. Accurate salinity data requires corrections for temporal and spatial mismatches in these sensor responses (Fofonoff et al 1974;Gregg and Hess 1985;Lueck 1990;Lueck and Picklo 1990;Morison et al 1994).…”
Section: Introductionmentioning
confidence: 99%
“…The exhaust of the pumped duct is at the same (pressure) level as the intake, so as to eliminate the ram effect of dynamic pressure (Sea-Bird, 2012). Thus, in theory the flow speed is constant past the sensors, which simplifies the dynamic response calibration (Gregg and Hess, 1985) by eliminating errors in T-measurement due to sensor-friction (≈ +110 -3 °C for a 1 m s -1 flow speed; Larson and Pedersen, 1996) and weaker errors due to flow-induced pressure variations in an adiabatic lapse rate environment (p d = 1/2ρU 2 , ρ the water density; for a speed range of U = [0, 4.5] m s -1 this yields a pressure range of [0, 1] dbar).…”
Section: Datamentioning
confidence: 99%