Precipita)on measurements at Rothera research sta)on in Antarc)ca. Steve Colwell Bri)sh Antarc)c Survey

Similar documents
OUS31. Technical Information

REMOTE SENSING APPLICATION in WIND ENERGY

PAPER 2 THEORY QUESTIONS

E/ECE/324/Rev.1/Add.47/Rev.9/Amend.2 E/ECE/TRANS/505/Rev.1/Add.47/Rev.9/Amend.2

A Guide To Aviation Weather

BLOCKAGE LOCATION THE PULSE METHOD

Understanding How the Appearance of Optical Fiber Splices Relates to Splice Quality

L-708 / L-708LD Bore Alignment System

Look at the simplified diagram of the laser and cross-section of part of a disc. to detector

Anemometry. Anemometry. Wind Conventions and Characteristics. Anemometry. Wind Variability. Anemometry. Function of an anemometer:

These materials are based on L.C. McDermott, & P.S. Schaffer, Tutorials in Introductory Physics, Prentice Hall (2001)

Crave the Wave, Feb 16, 2008 TEAM Mentor Invitational Score Rank

SPECIFICATIONS PARTICLE SENSOR KS-18F Higashimotomachi, Kokubunji, Tokyo , Japan

OptonPro. High-power laser up to 7000 mw. Laser therapy natural healing with the power of light

PROJECT CYCLOPS: THE WAY FORWARD IN POWER CURVE MEASUREMENTS?

Windar Photonics Wind Sensor. Great at Control

Level MEASUREMENT 1/2016

Offshore Wind Turbine Wake Characterization using Scanning Doppler Lidar

Genesis MX SLM-Series

WAVE NOTES WAVE NOTES THROUGH A MEDIUM EMPTY SPACE

Laser-Induced Bubbles in Glycerol-Water Mixtures

Chapter 10 Mr. Davis, M.Ed.

Questions OSCILLATIONS AND WAVES

Verdi G-Series. High-Power Pumps for Ti:Sapphire Lasers and Amplifiers FEATURES

AIMING STRAIGHT FOR THE FLAGSTICK

Wallace Hall Academy

THE ADVANCED DIGITAL SNOW SONDE

3.6 Magnetic surveys. Sampling Time variations Gradiometers Processing. Sampling

Projection Lens Datasheet

! " " # $% $ % % & %

High Resolution Sea Surface Roughness and Wind Speed with Space Lidar (CALIPSO)

A real time vessel air gap monitoring system

Flow analysis with nacellemounted

4.4 WAVE CHARACTERISTICS 4.5 WAVE PROPERTIES Student Notes

Verdi G-Series Family

WMB-160F Multi-beam Fishing System

What is a wave? A wave is a disturbance that transfers energy from place to place.

Site audit of IZO, GAW Global station, Izaña, Tenerife

WMO LABORATORY INTERCOMPARISON OF RAIN INTENSITY GAUGES

Laser Cutting. Nitrogen Solutions for

Florida Benchmark Review Unit 3

Waves Questions - CfE

Any laboratory is equipped with specific tools, equipment,

4-9 Long-term Observations Using L-Band Wind Profiler in Asia

19 The diagrams show water waves that move more slowly after passing into shallow water at the broken line. shallow water.

Measurement of Bubble Velocity using Spatial Filter Velocimetry

RAMSTM. 360 Riser and Anchor-Chain Integrity Monitoring for FPSOs

SPECIFICATIONS PARTICLE SENSOR KS-19F Higashimotomachi, Kokubunji, Tokyo , Japan

Standard Operating Procedure - First Draft for Review Only- StarWeld Ultra DX

Scales of Motion and Atmospheric Composition

Experiment B-18 Heart Rate and Coughing

Downhole Optical Analysis of Formation Fluids

Measurement of court speed and bounce. Rod Cross, Physics Department, Sydney University 2nd July 2006

Section 1 Types of Waves. Distinguish between mechanical waves and electromagnetic waves.

FAP 800 Series. High-Brightness Fiber-Coupled Bars FEATURES

P.O.Box 43 Blindern, 0313 Oslo, Norway Tel.: , Fax: Statkraft,Postboks 200 Lilleaker, 0216 Oslo, Norway ABSTRACT

A Wind Profiling Platform for Offshore Wind Measurements and Assessment. Presenter: Mark Blaseckie AXYS Technologies Inc.

EMPOWERING OFFSHORE WINDFARMS BY RELIABLE MEASUREMENTS

NanoSight NS300. NanoSight NS300. Operation instructions. Laser Spectroscopy Labs, UCI

Air Sensor. FCS Ex. Manual. AQ Elteknik AB

TG-61 deals with: This part of the refresher course: Phantoms. Chambers. Practical Implementation of TG-61:

Mid-IR Lasers Market Review and Forecast 2010

National Report of China

Sound and Light Test

14/10/2013' Bathymetric Survey. egm502 seafloor mapping

Figure 2: Principle of GPVS and ILIDS.

Cover Page for Lab Report Group Portion. Boundary Layer Measurements

BOTTOM MAPPING WITH EM1002 /EM300 /TOPAS Calibration of the Simrad EM300 and EM1002 Multibeam Echo Sounders in the Langryggene calibration area.

Remote sensing standards: their current status and significance for offshore projects

FLUORESCENCE DETERMINATION OF OXYGEN

New Generation System M, leading the World in the Non-Invasive Measurement of Critical Real-Time Parameters.

Next Generation Quartz Pressure Gauges

OPERATION OF LIQUID PARTICLE COUNTER. GP-B P0045 Rev -

Chapter 16. Waves-I Types of Waves

Waves. Kevin Small or

Outline Chapter 7 Waves

T EK-COR 1100A. Coriolis Mass Flowmeter. FLOW. Technology Solutions

CERT Educational Series Light and Waves Module

Turbimax CUS31. Technical Information

Characteristics of Waves

Sensor for Air Bubble Detection at Liquid Filled Tubes. SONOCHECK Type ABD06.xx. Operating Manual

WindProspector TM Lockheed Martin Corporation

Optical-Polymer and Polymer-Clad- Silica-Fiber Data Buses for Vehicles and Airplanes Principles, Limits and New Trends

Measurement of Low GAS & Liquid Flows

E3G-L1/L3. Effectively Cuts the Influence of Workpiece Characteristics, Such as Gloss, Incline, and Color. Distance-setting Photoelectric Sensor

SEA SURFACE TEMPERATURE RETRIEVAL USING TRMM MICROWAVE IMAGER SATELLITE DATA IN THE SOUTH CHINA SEA

Boost Your Skills with On-Site Courses Tailored to Your Needs

Technical Note. Determining the surface tension of liquids by measurements on pendant drops

RESPIRATORY PHYSIOLOGY, PHYSICS AND

Ongoing research in Hong Kong has led to improved wind shear and turbulence alerts

What is a wave? Even here the wave more or less keeps it s shape and travelled at a constant speed. YouTube. mexicanwave.mov

A Study of the Normal Turbulence Model in IEC

The Gas Attenuator of FLASH

i-clicker Discussion Question

from ocean to cloud PARAMETRIC SUB-BOTTOM PROFILER, A NEW APPROACH FOR AN OLD PROBLEM

Figure 1 - JPIF proposal for ISO standardisation of the CAI test method

Calculations for Line-of- Balance Diagrams

High Definition Laser Scanning (HDS) Underwater Acoustic Imaging and Profiling

Research articles A laser alignment system for boat assembly

Social Studies CHAPTER 2: PART 2 CLIMATE AND WEATHER

Transcription:

Precipita)on measurements at Rothera research sta)on in Antarc)ca Steve Colwell Bri)sh Antarc)c Survey

Background Solid precipita)on is very hard to measure in Antarc)ca. The World Meteorological Organisa)on (WMO) is currently running a project called the Solid Precipita)on Intercomparison Experiment (SPICE). SPICE is trying to evaluate the best way to make electronic measurements of solid precipita)on. The WMO are using a double fence reference gauge BAS is trialling several precipita)on measuring devices at Rothera sta)on but does not have space for the reference gauge.

Biral VPF 730 combined precipita)on and visibility sensor

Mode of Operation of the VPF 730 The sensor uses an 850nm infrared light source that is then detected using a forward scatter receiver and also a backscatter receiver. The forward scatter is used to calculate visibility. The backscatter receiver gives the sensor the ability to discriminate between liquid and frozen precipitation, liquid precipitation scatters very little of the transmitted light towards the backscatter receiver, whilst frozen precipitation scatters a significant amount in this direction. Transmitter forward scatter receiver backscatter receiver

Thies Laser Precipita)on Monitor

Mode of Operation of the Laser Precipitation Monitor A laser-optical beaming source of wavelength 780nm produces a parallel light-beam. A photo diode with a lens is situated on the receiver side in order to measure the optical intensity by transforming it into an electrical signal. 20mm Infrared light beam 228 mm Particle 0.75mm When a precipitation particle falls through the light beam the receiving signal is reduced and the diameter of the particle is calculated from the amplitude of the reduction. The fall speed of the particle is determined from the duration of the reduced signal. The measured values are processed by a signal processor, and checked for plausibility (e.g. edge hits). Calculation comprises the intensity, quantity, and type of precipitation (drizzle, rain, snow, soft hail, hail as well as mixed precipitation)

PWS10present weather sensor

PWS10general arrangement

Delayed refrac)on to horizontal sensor The sensor comprises one laser head and two sensor heads. Each of the sensor heads is 20 off axis to the laser unit axis, one in the horizontal plane, the other in the vertical plane When a particle enters the beam it is first detected by the off axis receiver in the vertical plane and then a short time later by the second receiver in the horizontal plane. This allows the size and fall speed to be calculated.

Environmental Measurements Ltd Universal Precipita)on Gauge (UPG1000)

Universal Precipita)on Gauge Ini)ally the gauge was located up by the meteorological tower. The a wind shield was installed round the gauge a year later. Finally the gauge and wind shield were relocated behind one of the buildings to give some extra wind shielding. Each of the changes increased the amount of precipita)on that was captured.

120. Rothera snowgauge March 2015 100. 80. Snowgauge LPM PWS 10 60. VPF 73 40. 20. 0. 1 2 3 4 5 6 7 8 9 1 11 12 13 14 15 16 17 18 19 2 21 22 23 24 25 26 27 28 29 3 31

6 Weather March 24th 2015 45 5 4 35 4 3 3 25 2 2 15 1 1 5 2 4 6 8 1 12 14 16 18 2 22 Hours Temperature Wind Speed (knots)

6 March 24th 2015 5 4 P rec i p it a ti 3 o n( m ) 2 1 1 241 481 721 961 1201 Time in minutes LPM PWS10 Heated snowgauge VPF 73

0.4 March 24th 2015 1.2 0.35 1 0.3 0.25 0.8 R at e 0.2 0.6 0.15 0.4 0.1 0.05 0.2 1 241 481 721 961 1201 Time in minutes LPM PWS 10 VPF 73 Heated snowgage

14. Rothera snowgauge May 2015 12. 10. Snowgauge LPM PWS 10 8. VPF 73 6. 4. 2. 0. 1 2 3 4 5 6 7 8 9 1 11 12 13 14 15 16 17 18 19 2 21 22 23 24 25 26 27 28 29 3 31

Weather May 20th 2015 25 2 2 4 15 6 1 8 1 5 12 Hours 2 4 6 8 1 12 14 16 18 2 22 Temperature Wind Speed (knots)

n ( m 6 May 20th 2015 P r e c i p i t a5 t o i m ) 4 3 2 1 1 241 481 721 961 1201 1441 Time in minutes LPM PWS 10 Heated snowgauge VPF 73

0.08 May 20th 2015 0.12 0.07 0.1 0.06 0.05 0.08 R at e 0.04 0.06 0.03 0.04 0.02 0.01 0.02 1 241 481 721 961 1201 1441 Time in minutes LPM PWS10 VPF 73 Heated snowgauge

0.08 May 20th 2015 25 0.07 0.06 2 0.05 15 R at e 0.04 0.03 1 0.02 5 0.01 1 241 481 721 961 1201 1441 Time in minutes LPM PWS10 VPF 73 Wind speed (knots)

0.08 May 20th 2015 40 0.07 35 0.06 30 0.05 25 R at e 0.04 20 0.03 15 0.02 10 0.01 5 1 241 481 721 961 1201 1441 Time in minutes LPM PWS10 VPF 73 Wind direc)on

0.08 May 20th 2015 9 0.07 85 0.06 8 0.05 75 R at e 0.04 7 0.03 65 0.02 6 0.01 55 1 241 481 721 961 1201 1441 Time in minutes 5 LPM PWS10 VPF 73 LPM precip PWS 10precip

Conclusions For rain there is good agreement between all of the sensors. During solid precipita)on events both the LPM and VPF 73can at )mes over read. Most of the )me there is disagreement between all of the sensor and as there is no ground truth it is impossible to say which is the most accurate. The data needs to be examined in more detail to try and iden)fy why there is a discrepancy in the readings.

2 Thies LPMs on the meteorological tower at Halley. One at 5m and the other at 10m to look at the affect of blowing snow

Ques)ons