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A bathythermograph

The bathythermograph, or BT, also known as the Mechanical Bathythermograph, or MBT;[1] is a small torpedo-shaped device that holds a temperature sensor and a transducer to detect changes in water temperature versus depth down to a depth of approximately 285 m. Lowered by a small winch on the ship into the water, the BT records pressure and temperature changes on a coated glass slide as it is dropped nearly freely through the water.[2] While the instrument is being dropped, the wire is being drug out until it reaches the predetermined depth, then a break is applied and the BT is drawn back to the surface.[1] Because the pressure is a function of depth (see Pascal's law), temperature measurements can be correlated with the depth at which they are recorded.[citation needed]


The true origins of the BT began in 1935 when Carl-Gustaf Rossby started experimenting. He then forwarded the development of the BT to his graduate student Athelstan Spilhaus. Who then fully developed the BT in 1938 [1] as a collaboration between MIT, Woods Hole Oceanographic Institution (WHOI), and the U.S. Navy.[3] The device was modified during World War II to gather information on the varying temperature of the ocean for the U.S. Navy. Originally the slides were prepared "by rubbing a bit of skunk oil on with a finger and then wiping off with the soft side of one's hand,” followed by smoking the slide over the flame of a Bunsen burner.[4] Later on the skunk oil was replace with an evaporated metal film.[1]

Throughout the use of the bathythermograph various technicians, watchstanders, and oceanographers noted how dangerous the deployment and retrieval of the BT was. According to watchstander Edward S. Barr:

"… In any kind of rough weather, this BT position was frequently subject to waves making a clean sweep of the deck. In spite of breaking waves over the side, the operator had to hold his station, because the equipment was already over the side. One couldn't run for shelter as the brake and hoisting power were combined in a single hand lever. To let go of this lever would cause all the wire on the winch to unwind, sending the recording device and all its cable to the ocean bottom forever. It was not at all uncommon, from the protective position of the laboratory door, to look back and see your watchmate at the BT winch completely disappear from sight as a wave would come crashing over the side. … We also took turns taking BT readings. It wasn't fair for only one person to get wet consistently." [5]

After witnessing this firsthand James M. Snodgrass began developing the expendable bathythermograph (XBT). Snodgrasses description of the XBT:

Briefly, the unit would break down in two components, as follows: the ship to surface unit, and surface to expendable unit. I have in mind a package which could be jettisoned, either by the “Armstrong” method, or some simple mechanical device, which would at all times be connected to the surface vessel. The wire would be payed out from the surface ship and not from the surface float unit. The surface float would require a minimum of flotation and a small, very simple sea anchor. From this simple platform the expendable BT unit would sink as outlined for the acoustic unit. However, it would unwind as it goes a very fine thread of probably neutrally buoyant conductor terminating at the float unit, thence connected to the wire leading to the ship.[6]
In the early 1960s the U.S. Navy contracted Sippican Corporation of Marion, Massachusetts to develop the XBT, whom became the sole supplier.[1]

Expendable BathythermographEdit

File:Expendable Bathythermograph.png

Merged content from Expendable bathythermograph to here. See Talk:Bathythermograph.

The unit is composed of a probe; a wire link; and a shipboard canister. Inside of the probe is a thermistor which is connected electronically to a chart recorder. The probe falls freely at 20 feet per second and that determines its depth and provides a temperature-depth trace on the recorder. A pair of fine copper wires which pay out from both a spool retained on the ship and one dropped with the instrument, provide a data transfer line to the ship for shipboard recording. Eventually, the wire runs out and breaks, and the XBT sinks to the ocean floor. Since the deployment of an XBT does not require the ship to slow down or otherwise interfere with normal operations, XBT's are often deployed from vessels of opportunity, such as cargo ships or ferries, rather than a dedicated research ship where a CTD would normally be used in preference. Airborne versions (AXBT) are also used; these use radio frequencies to transmit the data to the aircraft during deployment. Today Lockheed Martin Sippican has manufactured over 5 million XBTs.

Types of XBTs[7]Edit

Model Applications Maximum Depth Rated Ship Speed Vertical Resolution
T-4 Standard probe used by the U.S. Navy for ASW operations 460 m
1500 ft
30 knots 65 cm
T-5 Deep ocean scientific and military applications 1830 m
6000 ft
6 knots 65 cm
Fast Deep Provides maximum depth capabilities at the highest possible ship speed of any XBT 1000 m
3280 ft
20 knots 65 cm
T-6 Oceanographic applications 460 m
1500 ft
15 knots 65 cm
T-7 Increased depth for improved sonar prediction in ASW and other military applications 760 m
2500 ft
15 knots 65 cm
Deep Blue Increased launch speed for oceanographic and naval applications 760 m
2500 ft
20 knots 65 cm
T-10 Commercial fisheries applications 200 m
600 ft
10 knots 65 cm
T-11 High resolution for U.S. Navy mine counter-measures and physical oceanographic applications. 460 m
1500 ft
6 knots 18 cm

Participation by Month of Country and Institutions deploying XBTsEdit

Below is the list of XBT deployments for 2013:[8]

AUS 114 177 163 128 197 232 1011
AUS/SIO 8 52 0 0 48 90 198
CAN 16 53 31 24 70 129 323
FRA 2 10 199 43 19 11 284
GER 38 20 0 0 0 0 58
ITA 28 0 25 38 27 29 147
JPN 38 25 35 57 80 94 329
USA/AOML 469 474 753 1 782 339 2818
USA/SIO 788 87 604 240 349 591 2659
ZA 84 141 0 0 0 0 225
Total 1585 1039 1810 531 1572 1515 8052

XBT Fall Rate BiasEdit

Since XBTs do not measure depth (e.g. via pressure), fall-rate equations are used to derive depth profiles from what is essentially a time series. The fall rate equation takes the form:

$ z(t)=at^2+bt $

where, z(t) is the depth of the XBT in meters; t is time; and a & b are coefficients determined using theoretical and empirical methods. The coefficient A can be thought of as the initial speed as the probe hits the water. The coefficient B can be thought of as the reduction in mass with time as the wire spools off.

For a considerable time, these equations were relatively well-established, however in 2007 Gouretski and Koltermann showed a bias between XBT temperature measurements and CTD temperature measurements.[9] They also showed that this varies over time and could be due to both errors in the calculation of depth and in measurement of the temperature. From that the 2008 NOAA XBT Fall Rate Workshop [10] began to address the problem, with no viable conclusion as to how to proceed with adjusting the measurements. In 2010 the second XBT Fall Rate Workshop was held in Hamburg, Germany to continue discussing the problem and forge a way forward.[11]

A major implication of this is that a depth-temperature profile can be integrated to estimate upper ocean heat content; the bias in these equations lead to a warm bias in the heat content estimations. The introduction of Argo floats has provided a much more reliable source of temperature profiles than XBTs, however the XBT record remains important for estimating decadal trends and variability and hence much effort has been put into resolving these systematic biases. XBT correction needs to include both a drop-rate correction and a temperature correction.


See alsoEdit

External linksEdit


  1. 1.0 1.1 1.2 1.3 1.4 Scripps Institution of Oceanography: Probing the Oceans 1936 to 1976. San Diego, Calif: Tofua Press, 1978.
  2. Stewart, Robert H. (2007). Introduction to Physical Oceanography. College Station: Texas A&M University. OCLC 169907785. 
  4. Letter from Allyn Vine to Richard H. Fleming, 20 August 1941.
  5. “MIDPAC — The First Big Step,” manuscript, 17 August 1975.
  6. “New Techniques in Undersea Technology,” IEEE Transactions on Aerospace and Electronic Systems, Vol. AES-2, No. 6 (November 1966), 626.
  9. Gouretski, V. V., and K. P. Koltermann, 2007, How much is the ocean really warming? Geophysical Research Letters, L01610, doi:10.1029/2006GL027834
  10. "NOAA XBT Fall Rate Workshop". Retrieved 3 December 2013. 
  11. Viktor Gouretsk (25–27 August 2010). "XBT Bias and Fall Rate Workshop Summary Report" (pdf). Hamburg, Germany. pp. 14. Archived from the original. Error: If you specify |archiveurl=, you must also specify |archivedate=. Retrieved 3 December 2013. 
  • Blair, Clay Jr. (2001). Silent Victory, the U.S. Submarine war against Japan. Annapolis, Maryland: Naval Institute Press. p. 458. ISBN 1-55750-217-X. 

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