19.01.2015 Views

humidity / dew point / tempeRAtuRe / moistuRe in oil ... - Vaisala

humidity / dew point / tempeRAtuRe / moistuRe in oil ... - Vaisala

humidity / dew point / tempeRAtuRe / moistuRe in oil ... - Vaisala

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

<strong>Vaisala</strong> Sensor Technologies for W<strong>in</strong>d and Ra<strong>in</strong> Measurements<br />

<strong>Vaisala</strong> WINDCAP® Sensor<br />

<strong>Vaisala</strong> WINDCAP ® Ultrasonic W<strong>in</strong>d Sensor uses ultrasound<br />

to determ<strong>in</strong>e w<strong>in</strong>d speed and direction. The sensor has<br />

no mov<strong>in</strong>g parts, which makes it <strong>in</strong>dependent of the<br />

limitations of mechanical w<strong>in</strong>d sensors such as friction,<br />

<strong>in</strong>ertia, time constant, over-speed<strong>in</strong>g, and start<strong>in</strong>g treshold.<br />

How It Works<br />

WINDCAP ® sensor features an array of three ultrasonic<br />

transducers oriented to form an equilateral triangle. W<strong>in</strong>d<br />

measurement is based on time of flight (TOF) of the sonic<br />

impulse - the time it takes for the signal to travel from one<br />

transducer to another. TOF is measured <strong>in</strong> both directions<br />

for each pair of transducer heads. Simple algebra allows<br />

solv<strong>in</strong>g for the parallel component of w<strong>in</strong>d velocity<br />

<strong>in</strong>dependently of the static speed of sound.<br />

The equilateral triangle configuration of the three<br />

Transducer separation length, L<br />

Transmit<br />

Receive<br />

1<br />

1<br />

Time of flight, t 1<br />

Vw<br />

Parallel component of w<strong>in</strong>d velocity<br />

Time of flight, t 2<br />

For static speed of sound V s:<br />

Comb<strong>in</strong>e to remove V s:<br />

Solve for V<br />

w<br />

V w =<br />

1 =<br />

t 1<br />

V s + V<br />

L<br />

w<br />

L 1<br />

1<br />

2<br />

( - )<br />

t 1<br />

t 2<br />

and<br />

2<br />

2<br />

Receive<br />

Transmit<br />

1 V s + V<br />

=<br />

t 2<br />

L<br />

w<br />

<strong>Vaisala</strong> RAINCAP® Sensor<br />

<strong>Vaisala</strong> RAINCAP ® Sensor is an acoustic sensor that<br />

measures the impact of <strong>in</strong>dividual ra<strong>in</strong>drops on a smooth<br />

sta<strong>in</strong>less steel surface us<strong>in</strong>g a piezoelectric detector. The<br />

sensor provides real time <strong>in</strong>formation on ra<strong>in</strong> <strong>in</strong>tensity,<br />

duration, and accumulated ra<strong>in</strong>fall.<br />

How It Works<br />

The RAINCAP ® sensor consists of a round sta<strong>in</strong>less steel<br />

cover, approximately 90 mm <strong>in</strong> diameter mounted to a<br />

rigid frame. A piezoelectric detector is located beneath<br />

the cover.<br />

Ra<strong>in</strong>drops hit the RAINCAP ® sensor surface at term<strong>in</strong>al<br />

velocity, which is a function of the ra<strong>in</strong>drop diameter.<br />

Ra<strong>in</strong> measurement is based on acoustic detection of each<br />

<strong>in</strong>dividual ra<strong>in</strong> drop as it impacts the sensor cover. Larger<br />

drops create a larger acoustic signal than smaller drops.<br />

The piezoelectric detector converts the acoustic signals<br />

<strong>in</strong>to voltages. Total ra<strong>in</strong> is calculated from the sum of the<br />

<strong>in</strong>dividual voltage signals per unit time and the known<br />

surface area of the RAINCAP ® sensor. In addition, the<br />

<strong>in</strong>tensity and duration of ra<strong>in</strong> can be calculated.<br />

p v = mv t<br />

transducers provides three possible sets of basis vectors.<br />

The comb<strong>in</strong>ations yield bi-directional measurements on<br />

the paths labeled A, B and C. These measurements are<br />

used to determ<strong>in</strong>e the w<strong>in</strong>d velocity components parallel<br />

to each of the three paths.<br />

Electronics<br />

Piezo detector<br />

Algorithm<br />

path a<br />

60˚<br />

1<br />

60˚<br />

path C<br />

60˚<br />

2 3<br />

path b<br />

Basis<br />

set 1<br />

Basis<br />

set 2<br />

Basis<br />

set 3<br />

A<br />

A<br />

B<br />

B<br />

C<br />

C<br />

Output<br />

Pv = vertical momentum<br />

m = mass of drop<br />

v t<br />

= term<strong>in</strong>al velocity of drop<br />

Weather<br />

For more <strong>in</strong>formation, visit<br />

www.vaisala.com or contact<br />

us at sales@vaisala.com<br />

Ref. B211233EN-A ©<strong>Vaisala</strong> 2012<br />

This material is subject to copyright protection, with all copyrights<br />

reta<strong>in</strong>ed by <strong>Vaisala</strong> and its <strong>in</strong>dividual partners. All rights reserved.<br />

Any logos and/or product names are trademarks of <strong>Vaisala</strong> or<br />

its <strong>in</strong>dividual partners. The reproduction, transfer, distribution or<br />

storage of <strong>in</strong>formation conta<strong>in</strong>ed <strong>in</strong> this brochure <strong>in</strong> any form<br />

without the prior written consent of <strong>Vaisala</strong> is strictly prohibited.<br />

All specifications — technical <strong>in</strong>cluded — are subject to change<br />

without notice.<br />

167

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!