PMElogo.jpg (16797 bytes)
                                                                     Precision Measurement Engineering, Inc.


PME Home Page Contact Information View Product Information View Sales Information View Library Publications View What's New View Employment Opportunities View Useful Links Search PME Website



Description
Operation
Sensors
Analog Processing
Software
Specifications
Upgrade
Prices
References
FAQs
Projects

Self Contained Autonomous MicroProfiler (SCAMP)

in cooperation with the Centre for Water Research   cwr_small.gif (1693 bytes)


DESCRIPTION

The Self Contained Autonomous MicroProfiler (SCAMP) is a portable, lightweight microstructure profiler designed to measure extremely small scale (order 1 mm) fluctuations of electrical conductivity, temperature, and oxygen concentration in lakes, reservoirs, estuaries, and the oceans. These data can be used to infer the levels of dissipation of turbulent kinetic energy; in-situ fluxes of heat, salt, and oxygen; and the microstructure behavior of these parameters.

The SCAMP is waterproof, battery operated, capable of autonomous or on-line operation, and can easily be deployed by hand from a small dinghy. It is equipped with sensors that feature high spatial resolution and fast-time response. The unique drag plate and floats allow the SCAMP to ascend or descend vertically making measurements (1 scan of all sensors every mm) through undisturbed water. This allows the user to measure properties in the surface layer (ascent) or the benthic boundary layer (descent).

The software supplied with the SCAMP allows the user to upload, record, view, and analyze measurements. The new improved SCAMP now has a USB interface.   For more information read the USB manual.   For information about the first generation SCAMPs read the manual.


OPERATION

The SCAMP is designed to profile water columns of up to 100 meters in length, sampling all sensors every 1mm. The SCAMP can sample while traveling at 10 cm/sec either upward or downward through the water column. If the SCAMP is used in downward mode, then it can sample undisturbed water beginning somewhat below the surface and continuing all the way to the bottom. In upward mode, it can sample undisturbed water up through the surface. These two modes of travel enable the SCAMP to measure both surface mixing and benthic boundary layer mixing. The following photos show the SCAMP's position in the water for each mode.


DOWNWARD

When the SCAMP is used in downward mode, the floats are positioned against the drag plate. It is deployed with the sensors facing downwards as shown in the photos. In this mode, it sinks vertically downward at 10 cm/sec until the length of the retrieval line is reached or until the sensor guard touches the bottom. All the sensors are sampled every 1 mm during the descent. The samples are stored internally within the SCAMP.  When the profile is complete, the SCAMP is hauled back using the retrieval line.  Samples are recorded internally, then they are uploaded to the host computer after the SCAMP is recovered on the deck.

The pictures below show these features:  The weight release screw is visible, although the threads on this screw cannot be seen. The drag plate is the black, plastic support and circular disk. Note the stainless steel hinges. These allow the drag plate to fold away when retrieving the SCAMP. The white thumb screw allows easy removal of the drag plate for storage. Floats are shown just below the hand.


scamp75.jpg (78172 bytes)scamp77.jpg (71607 bytes)

 

UPWARD

When the SCAMP is used in upward mode, the floats are positioned against the sensor end and an expendable weight is connected. This weight is connected to the SCAMP's motorized release mechanism. The SCAMP is deployed with the sensors facing upward as shown in the images. In this mode it sinks sideways at an angle of approximately 45 degrees until it reaches the bottom or a pre-determined depth. Upon reaching this point, it activates the release motor and drops the expendable weight. The SCAMP then floats vertically upward at 10 cm/sec sampling all sensors every 1 mm. Samples are stored internally within the SCAMP. Sampling continues until the sensors pass through the surface. When the profile is complete, the SCAMP is hauled back using the retrieval line. Samples are uploaded to the host computer after the SCAMP is recovered on the deck.

These images show these features: the floats are shown above the hand, the drag plate is shown below the hand. Note that this plate is shown at a slight angle from perpendicular to the SCAMP body. The plate is hinged on the supports and it will swing up to 30 degrees. This causes the SCAMP to sink sideways. On ascent, the plate swings to the perpendicular position and the SCAMP floats straight up. There are two arms on the release plate, held together by a pin (not shown). The pin is attached to the retrieval line. This pin pulls away during retrieval and the sides of the drag plate fold away for easy towing through the water.

scamp58.jpg (121191 bytes)scamp.jpg (42749 bytes)

 

SENSORS

all_sensors_closeup.jpg (85369 bytes)


The SCAMP can carry many different types of sensors. Presently implemented are: fast conductivity, fast temperature, accurate conductivity and temperature, chlorophyll fluorometer, turbidity, and PAR. All these sensors are shown in the picture except the chlorophyll fluorometer, turbidity, and PAR. The SCAMP has many unused channels so that other sensors such as pH are possible. Space in the endcap and internal space for appropriate circuitry are the only limitations.

As the picture shows, the sensor design allows the fast sensors to be positioned very close to each other enabling temperature-temperature correlation.

   

ANALOG PROCESSING

In addition to the sensor electronics and the A/D converter, the SCAMP contains two types of analog processing circuits: offset-gain scaling and gradient-gain-filtering.

An offset-gain block is connected between sensor channels and the A/D converter. This block has the effect of allowing the SCAMP's A/D to sample a sub-range of the sensor range under software control. For example, the temperature sensor's electronics has valid output for the range 0 to 30 deg. C. Under software control, the offset and gain block can be programmed such that the A/D's full range occurs over the temperature range of 10 to 15 deg. C, giving 6X resolution. Sub-ranging can also be applied to other channels.

The SCAMP can support up to 8 gradient-gain-filter blocks. These blocks first compute the time derivative of a sensor channel, then amplify the result by a programmable gain of 1 to 256, then filter using a 6-pole anti-alias filter at a fixed frequency of 45 Hz. These circuits can be connected to any channel, but usually are connected only to the fast temperatures. These channels have the effect of eliminating A/D noise since the gradient signals are zero mean and can be amplified significantly.

The paramount design criteria in both the SCAMP's electrical design and mechanical packaging is to obtain a measurement system designed for spectral analysis and having the lowest measurement noise possible.


SOFTWARE

The SCAMP is supplied with software that enables control of the SCAMP, calibration, data acquisition with upload to host computer, complex analysis, and graphical display. This software runs under Windows 2000.

Control of the SCAMP includes many items related to the SCAMP's internal state such as measurement of battery voltages, various tests of analog and digital hardware, time keeper control, and other housekeeping functions.

Data acquisition and upload are managed by SCAMP's internal computer based on information provided by host computer software. The customer may set data acquisition start/stop parameters such as depth, time, or number of samples by using menus provided by the host computer software.  Subsequently when measurements are completed they appear in internal memory buffers within SCAMP.  Matlab software supplied with SCAMP allows the customer to save the measurements on disk for later viewing or analysis.

Matlab can perform various types of complex analysis of SCAMP measurements. The software can:

  • determine SCAMP velocity,
  • apply numerical filters for frequency compensation and filtering to all C & T sensors,
  • compute density for fresh and seawater,
  • compute sorted density,
  • compute gravity anomaly,
  • compute salinity for sea water,
  • compute Thorpe scales,
  • compute centered length scales,
  • compute buoyancy frequency,
  • compute power spectrum of Gradient Fast T0 channel,
  • compute estimation of best fit Batchelor spectrum to Gradient Fast T0 channel using kB and X as free parameters,
  • compute estimated dissipation of turbulent energy over 1E-10 to 1E-5 (M^2/S^3) range from Batchelor spectral fitting,
  • locate statistically stationary segments in the data for further analysis,
  • compute segmented turbulent energy dissipation, e, segmented buoyancy frequency, N, and segmented turbulence length scale, Lc,
  • compute segmented Kolmogorov length scales, Lk, and segmented Ozmidov length scales, Lo,
  • compute segmented turbulent Froude and turbulent Reynolds numbers,
  • compute segmented flux Richardson numbers and segmented buoyancy fluxes

 

Graphical display is an integral part of the calculations mentioned above. Each calculation has a representative display, often shown as the calculation result vs time or depth over full profiles or user-selected profile sections. The screen below shows a full profile at left of the (computed) Sigma-T channel measured by the SCAMP. The dotted lines indicate the segment selected for spectral analysis and Batchelor fitting. The center plot shows the Gradient Fast T0 channel, segment 9 of which (dotted lines) is analyzed and presented in the right two plots. The top right plot shows the matching of the observed power spectrum of Gradient Fast T0 (blue) to the ideal Batchelor spectrum (red) plus the anticipated electronic noise of SCAMP’s sensors and circuits (green).

More detailed information about the methods used to obtain these plots is given by the first two entries in the references section below.

SCAMPGUI1.gif (21097 bytes)

The screen above is representative of the various screen plots that Matlab software can display. 

Matlab software displays are available within a very short time after uploading the SCAMP measured data. It is possible to know the turbulent state of a profile in nearly real time.

The intent and design of the Matlab software are to allow easy control of SCAMP and to allow the customer to visualize the processes occurring within the water column in nearly real time. This enables the scientist to make sampling decisions based on conditions presently occurring within the water column, and is a powerful tool for the educator to provide motivation for students of environmental fluid dynamics.

For more information read the USB manual.


SPECIFICATIONS

SCAMP
Travel Rate 10 cm/sec
Overall Length 76 cm
Weight 6 kilos (13 lbs.)
Maximum Depth 100 meters
Sample Rate 100 scans/sec  (adjustable)
Batteries Required 6 alkaline AA; 2 alkaline 9V
Battery Life 4 hrs continuous operation minimum
FAST CONDUCTIVITY CHANNEL
Sensor PME 4-electrode microsensor
Range Ranged by scaling resistor(s):
        5E-2 to 0.1 siemens/meter         min.
        5E-2 to 9.0 siemens/meter         max.
Accuracy +/- 5% full scale depending on calibration
Stability +/- 5% full scale/4 hours
Bandwidth Approximately 400 cycles/meter
Filter 4 pole Butterworth @ 50 Hz
Calibration Performed by PME
CONDUCTIVITY CHANNEL
Sensor PME 4-electrode ceramic sensor
Range Jumper selected ranges:
5E-2 to 0.1 siemens/meter
5E-2 to 0.5 siemens/meter
5E-2 to 9.0 siemens/meter
Accuracy +/- 0.2% full scale (9 siemens/ meter range)
Stability +/- 0.2% full scale/month
Spatial Response Approximately 33 cycles/meter
Filter 4 pole Butterworth @ 50 Hz
Calibration Performed by PME
FAST TEMPERATURE CHANNEL
(2 available)
Sensor Thermometrics FP07 thermistor
Range 0 to 30 degrees C
Accuracy +/- 0.050 degrees C
Stability +/- 0.050 degrees C/month
Bandwidth Approximately 20 Hz
Filter 2 pole Butterworth @ 50 Hz
Calibration Performed by PME
TEMPERATURE CHANNEL
Sensor Thermometrics T1201 thermistor
Range 0 to 30 degrees C
Accuracy +/- 0.020 degrees C
Stability +/- 0.020 degrees C/month
Bandwidth Approximately 0.3 Hz
Filter 2 pole Butterworth @ 50 Hz
Calibration Performed by PME
OXYGEN CHANNEL
Sensor Unisense dissolved oxygen microsensor
Range 0 to 10E-3 grams/liter
Maximum Depth 10 meters
Accuracy +/- 1E-3 gram/liter depending on calibration
Stability +/- 1E-3 gram/liter / 4 hours
Bandwidth Approximately 1 Hz
Filter 2 pole Butterworth @ 50 Hz
Calibration Performed by the user
PRESSURE CHANNEL
Sensor Keller PSI PAA-10
Range 50 to 100 meters full scale
Accuracy +/- .5% full scale
Repeatability +/- 0.25% full scale
Stability +/- 0.25% / 6 months
Calibration Performed by PME
GRADIENT CHANNEL
(up to 8 available)
Function Computes d/dt using analog circuits
Gain Gains of 256/N N= 2,3,4... 255
Anti-alias Filter 6 pole Butterworth @ 45 Hz
DATA LOGGER, ANALOG
Channels 16 direct, 16 processed
Sampling rate 5000 samples/sec maximum
Sampling resolution 16 bit
Analog processing: gain 256/N N= 2,3,4 ... 255
Analog processing: offset +/- N/256 of full scale
N= 0... 255
RMS noise 91uV RMS on direct channels,

130 uV RMS on processed channels
DATA LOGGER, DIGITAL
CPU NEC V40
Instruction set 80186 compatible
Memory: program 128K static (battery backed)
Memory: data 1.7M static (battery backed)
Communication 19.2K baud RS485 3-wire up to 300 meter length
Digital ports one bi-directional 8 bit PIA and one IRQ
Memory usage 2 bytes per channel per sample


PRICE LIST

(subject to change without notice)

PART NUMBER

DESCRIPTION

PRICE
(USD)

5000 Includes the SCAMP profiler and all its accessories (see following tables)

Contact PME

5004 SCAMP upgrade Contact PME
5316 Fast Temperature Sensor

Contact PME

5346 Fast Conductivity Sensor   Contact PME
5199 Accurate Conductivity - Temperature Sensor Contact PME

5583

Fluorometer Addition Contact PME

5396

PAR Sensor Addition Contact PME

5469

Turbidity Sensor  (OBS- 3) Contact PME
5267 Dual Gradient Circuit Contact PME
  Sensor Installation   Contact PME 
  Pressure (recal or cal check)  Contact PME  
  Temperature (recal or cal check)  Contact PME
  Conductivity (recal or cal check) Contact PME
  Training at PME's facility

Contact PME

 

SCAMP profiler includes:

QUANTITY

DESCRIPTION

1

Fast temperature channel

1

Fast conductivity channel

1

Accurate conductivity- temperature channel

1

Pressure channel (100  meter depth)

1

Fast temperature gradient channel

1

Fast conductivity gradient channel

2

Spare temperature channels without sensors

1

Spare dissolved oxygen channel without sensor

1

64 MB MultiMedia card memory

2

Fast temperature sensor (mounted on profiler)
   

1

Accurate conductivity- temperature sensor (mounted on profiler)

 

SCAMP accessories included with the profiler are:

access.jpg (136140 bytes)

 

 
QUANTITY

PME PART NUMBER

DESCRIPTION

1 4803 drag plate
4 5322 and 5101 floats (3 rings and 1 nose)
1 5653 guard ring assembly
1 5357 and 5337 computer tent and stand
1 5078 retrieval line on roller (200 meters)
1 5527 USB short I/O cable
1 5151 float retaining ring
1 5104 seal pressure test adapter
1 5108 spare screw set
1 5107 spare o-ring set
1 5347 spare fuse assembly
1 5109 tool kit
1 4581 weight release line (100ft)
1 5330 lead weight set
1 5106 manual
1 5349 gray transportation case
1   SCAMP control and Matlab  software

 

 

tent.jpg (107147 bytes) 

 

Various other sensors can be mounted on the SCAMP. Contact PME regarding special projects.

REFERENCES

The following references describe the SCAMP or related instruments and measurements.

Anis, A. (2006), Similarity Relationships in the Unstable Aquatic Surface Layer, Geophys. Res. Lett., 33, L19609, doi:10.1029/2006GL027268. View the abstract.

Anis, A; Singhal, G. (July 2006), Mixing in the Surface Boundary Layer of a Tropical Freshwater Reservoir, Journal of Marine Systems, doi:10.1016/j.jmarsys.2006.07.003. View the abstract.

Chen, Huey-Long; Hondzo, Miki; Rao, A. Ramachandra (Dec., 2002). Segmentation of temperature microstructure, Journal of Geophysical Research-Oceans, 107(C12). Internet listing - http://www.agu.org/pubs/inpress.html

Etemad-Shahidi, Amir and Imberger, Jorg (1998).   Anatomy of Turbulence in Thermally Stratified Lakes.  Submitted to Limnology and Oceanography.  This paper presents a comparison of the dissipation obtained from shear with dissipation obtained from thermal gradients.  View the abstract in Adobe format.

Imberger, J. and Ivey, G.N.  (1990).    On the Nature of Turbulence in a Stratified Fluid.  Part II: Application to Lakes.  J. Physical Oceanography, Vol. 21, pages 659 to 680.   This paper (together with Part I) is the fundamental work upon which SCAMP is based.  View the abstract in Adobe format.

Ivey, G.N., and Imberger, J.  (1990).    On the Nature of Turbulence in a Stratified Fluid.  Part I: The Energetics of Mixing.  J. Physical Oceanography, Vol. 21, pages 650 to 658.   This paper (together with Part II) is the fundamental work upon which SCAMP is based.   View the abstract in Adobe format.

Krocsis, O., Prandke, H, Stips, A., Simon, A., and Wuest, A.(1999).  Comparison of Dissipation of Turbulent Kinetic Energy Determined from Shear and Temperature Microstructure.  J. Marine Systems, Vol. 21, pages 67-84.  This paper presents an excellent comparison of the Batchelor temperature microstructure method with the velocity shear microstructure method for determining turbulent dissipation.

Luketina, David A. and Imberger, Jorg (1998).    Determining Turbulent Kinetic Energy Dissipation from Batchelor Curve Fitting.  Submitted to the J.. Atm. and Oceanic Tech.   This paper presents a method for fitting temperature gradient spectra to the Batchelor form. View the abstract or the complete paper in Adobe format.

MacIntyre, Sally (1998).   Turbulent Mixing and Resource Supply to Phytoplankton.  Physical Processes in Lakes and Oceans Coastal and Estuarine Studies Volume 54, pages 561-590.  This paper presents an example SCAMP use. View the abstract in Adobe format.

MacIntyre, Sally, Flynn, Kevin M., Jellison, Robert, and Romero, Jose R. (1999).   Boundary mixing and nutrient fluxes in Mono Lake, California.  Limnology and Oceanography, Vol. 44, #3, pages   512 to 529.  This paper presents an example SCAMP use.  View the map of Mono Lake and the complete paper in Adobe format on Sally MacIntyre's web site.

Nash, Jonathan, and Moum, James (1997).   Estimating Salinity Variance Dissipation Rate from Conductivity Microstructure Measurements.  J. Atm and Oceanic Tech. Vol. 16,  #2, pages 263-274.  This paper presents data analysis based on the Fast C sensor mounted on another instrument. 

Piera, J., Roget, E., Catalan, J., 2002. Turbulent patch identification in microstructure profiles: A method based on wavelet denoising and Thorpe displacement analysis. J.  Atmos. Ocean. Tech. 19 (9),  1390-1402.

Ruddick, Barry, Anis, Ayal, and Thompson, Keith (1999).    Maximum Likelihood Spectral Fitting: the Batchelor Spectrum.   This paper presents a method for fitting temperature gradient spectra to the Batchelor form.  Submitted to J. Atm and Oceanic Tech.  View the abstract  or the complete paper in Adobe format.

Sharples, Jonathan, C. Mark Moore, Edward R. Abraham (15-Jul-2001).  Internal tide dissipation, mixing and vertical nitrate flux at the shelf edge of NE New Zealand.  Journal of Geophysical Research, Vol. 106, No. C7, pages 14,069 - 14,081. View the abstract in Adobe format.

Soga, L.C.M. and Rehmann, C.R, 2004. Dissipation of Turbulent Kinetic Energy near a Bubble Plume. J. Hydraul. Eng., 130, 441-449. 

Stevens, Craig, Murray Smith, Alex Ross (1999).  SCAMP: measuring turbulence in estuaries, lakes, and coastal waters. NIWA - Water and Atmosphere, Vol. 7, #2, pages 20-21. View the complete article in Adobe format.