Anemometer
A hemispherical cup anemometer of the type
invented in 1846 by John Thomas Romney
Robinson
Cup-type anemometer with vertical axis, a sensor
on a remote meteorological station deployed on
Skagit Bay, Washington July–August, 2009.
An anemometer is a device for measuring wind speed, and is a
common weather station instrument. The term is derived from the
Greek word anemos, meaning wind. The first known description of an
anemometer was given by Leon Battista Alberti around 1450.[1] They
are also very easy to make as a project.
Anemometers can be divided into two classes: those that measure the
wind's speed, and those that measure the wind's pressure; but as there
is a close connection between the pressure and the speed, an
anemometer designed for one will give information about both.
Velocity anemometers
Cup anemometers
A simple type of anemometer, invented (1846) by Dr. John Thomas
Romney Robinson, of Armagh Observatory. It consisted of four
hemispherical cups each mounted on one end of four horizontal arms,
which in turn were mounted at equal angles to each other on a vertical
shaft. The air flow past the cups in any horizontal direction turned the
cups in a manner that was proportional to the wind speed. Therefore,
counting the turns of the cups over a set time period produced the
average wind speed for a wide range of speeds. On an anemometer
with four cups it is easy to see that since the cups are arranged
symmetrically on the end of the arms, the wind always has the hollow
of one cup presented to it and is blowing on the back of the cup on the
opposite end of the cross.
When Robinson first designed his anemometer, he asserted that the
cups moved one-third of the speed of the wind, unaffected by the cup
size or arm length. This was apparently confirmed by some early
independent experiments, but it was incorrect. Instead, the ratio of the
speed of the wind and that of the cups, the anemometer factor, depends
on the dimensions of the cups and arms, and may have a value between two and a little over three. Every experiment
involving an anemometer had to be repeated.
The three cup anemometer developed by the Canadian John Patterson in 1926 and subsequent cup improvements by
Brevoort & Joiner of the USA in 1935 led to a cupwheel design which was linear and had an error of less than 3% up
to 60 mph (97 km/h). Patterson found that each cup produced maximum torque when it was at 45 degrees to the
wind flow. The three cup anemometer also had a more constant torque and responded more quickly to gusts than the
four cup anemometer.
The three cup anemometer was further modified by the Australian Derek Weston in 1991 to measure both wind
direction and wind speed. Weston added a tag to one cup, which causes the cupwheel speed to increase and decrease
as the tag moves alternately with and against the wind. Wind direction is calculated from these cyclical changes in
cupwheel speed, while wind speed is as usual determined from the average cupwheel speed.
Three cup anemometers are currently used as the industry standard for wind resource assessment studies.
Anemometer 2
A windmill style of anemometer
Windmill anemometers
The other forms of mechanical velocity anemometer may be described
as belonging to the windmill type or propeller anemometer. In the
Robinson anemometer the axis of rotation is vertical, but with this
subdivision the axis of rotation must be parallel to the direction of the
wind and therefore horizontal. Furthermore, since the wind varies in
direction and the axis has to follow its changes, a wind vane or some
other contrivance to fulfil the same purpose must be employed. An
aerovane combines a propeller and a tail on the same axis to obtain
accurate and precise wind speed and direction measurements from the same instrument. In cases where the direction
of the air motion is always the same, as in the ventilating shafts of mines and buildings for instance, wind vanes,
known as air meters are employed, and give most satisfactory results.
Hot-wire anemometers
Hot-wire sensor
Hot wire anemometers use a very fine wire (on the order of several
micrometres) electrically heated up to some temperature above the
ambient. Air flowing past the wire has a cooling effect on the wire. As the
electrical resistance of most metals is dependent upon the temperature of
the metal (tungsten is a popular choice for hot-wires), a relationship can be
obtained between the resistance of the wire and the flow speed.[2]
Several ways of implementing this exist, and hot-wire devices can be
further classified as CCA (Constant-Current Anemometer), CVA
(Constant-Voltage Anemometer) and CTA (Constant-Temperature
Anemometer). The voltage output from these anemometers is thus the
result of some sort of circuit within the device trying to maintain the specific variable (current, voltage or
temperature) constant.
Additionally, PWM (pulse-width modulation) anemometers are also used, wherein the velocity is inferred by the
time length of a repeating pulse of current that brings the wire up to a specified resistance and then stops until a
threshold "floor" is reached, at which time the pulse is sent again.
Hot-wire anemometers, while extremely delicate, have extremely high frequency-response and fine spatial resolution
compared to other measurement methods, and as such are almost universally employed for the detailed study of
turbulent flows, or any flow in which rapid velocity fluctuations are of interest.
Anemometer 3
Laser Doppler anemometers
Drawing of a laser anemometer. The laser is emitted (1) through the front lens (6) of the
anemometer and is backscattered off the air molecules (7). The backscattered radiation
(dots) re-enter the device and are reflected and directed into a detector (12).
Laser Doppler anemometers use a
beam of light from a laser that is
divided into two beams, with one
propagated out of the anemometer.
Particulates (or deliberately introduced
seed material) flowing along with air
molecules near where the beam exits
reflect, or backscatter, the light back
into a detector, where it is measured
relative to the original laser beam.
When the particles are in great motion,
they produce a Doppler shift for
measuring wind speed in the laser
light, which is used to calculate the
speed of the particles, and therefore the air around the anemometer.[3]
Sonic anemometers
3D ultrasonic anemometer
Sonic anemometers, first developed in the 1970s, use ultrasonic sound
waves to measure wind velocity. They measure wind speed based on
the time of flight of sonic pulses between pairs of transducers.
Measurements from pairs of transducers can be combined to yield a
measurement of velocity in 1-, 2-, or 3-dimensional flow. The spatial
resolution is given by the path length between transducers, which is
typically 10 to 20 cm. Sonic anemometers can take measurements with
very fine temporal resolution, 20 Hz or better, which makes them well
suited for turbulence measurements. The lack of moving parts makes
them appropriate for long term use in exposed automated weather
stations and weather buoys where the accuracy and reliability of
traditional cup-and-vane anemometers is adversely affected by salty air
or large amounts of dust. Their main disadvantage is the distortion of
the flow itself by the structure supporting the transducers, which
requires a correction based upon wind tunnel measurements to
minimize the effect. An international standard for this process, ISO
16622 Meteorology—Sonic anemometers/thermometers—Acceptance
test methods for mean wind measurements is in general circulation. Another disadvantage is lower accuracy due to
precipitation, where rain drops may vary the speed of sound.
Since the speed of sound varies with temperature, and is virtually stable with pressure change, sonic anomometers
are also used as thermometers.
Two-dimensional (wind speed and wind direction) sonic anemometers are used in applications such as weather
stations, ship navigation, wind turbines, aviation and weather buoys.
Anemometer 4
Ping-pong ball anemometers
A common anemometer for basic use is constructed from a ping-pong ball attached to a string. When the wind blows
horizontally, it presses on and moves the ball; because ping-pong balls are very lightweight, they move easily in light
winds. Measuring the angle between the string-ball apparatus and the line normal to the ground gives an estimate of
the wind speed.
This type of anemometer is mostly used for middle-school level instruction which most students make themselves,
but a similar device was also flown on Phoenix Mars Lander .
Pressure anemometers
The first designs of anemometers which measure the pressure were divided into plate and tube classes.
Plate anemometers
These are the earliest anemometers and are simply a flat plate suspended from the top so that the wind deflects the
plate. In 1450, the Italian art architect Leon Battista Alberti invented the first mechanical anemometer; in 1664 it was
re-invented by Robert Hooke (who is often mistakenly considered the inventor of the first anemometer). Later
versions of this form consisted of a flat plate, either square or circular, which is kept normal to the wind by a wind
vane. The pressure of the wind on its face is balanced by a spring. The compression of the spring determines the
actual force which the wind is exerting on the plate, and this is either read off on a suitable gauge, or on a recorder.
Instruments of this kind do not respond to light winds, are inaccurate for high wind readings, and are slow at
responding to variable winds. Plate anemometers have been used to trigger high wind alarms on bridges.
Tube anemometers
Helicoid propeller anemometer incorporating a
wind vane for orientation.
James Lind's anemometer of 1775 consisted simply of a glass U tube
containing liquid, a manometer, with one end bent in a horizontal
direction to face the wind and the other vertical end remains parallel to
the wind flow. Though the Lind was not the first it was the most
practical and best known anemometer of this type. If the wind blows
into the mouth of a tube it causes an increase of pressure on one side of
the manometer. The wind over the open end of a vertical tube causes
little change in pressure on the other side of the manometer. The
resulting liquid change in the U tube is an indication of the wind speed.
Small departures from the true direction of the wind causes large
variations in the magnitude.
The highly successful metal pressure tube anemometer of William
Henry Dines in 1892 utilized the same pressure difference between the
open mouth of a straight tube facing the wind and a ring of small holes
in a vertical tube which is closed at the upper end. Both are mounted at
the same height. The pressure differences on which the action depends
are very small, and special means are required to register them. The
recorder consists of a float in a sealed chamber partially filled with water. The pipe from the straight tube is
connected to the top of the sealed chamber and the pipe from the small tubes is directed into the bottom inside the
float. Since the pressure difference determines the vertical position of the float this is a measure of the wind speed.
The great advantage of the tube anemometer lies in the fact that the exposed part can be mounted on a high pole, and
requires no oiling or attention for years; and the registering part can be placed in any convenient position. Two
connecting tubes are required. It might appear at first sight as though one connection would serve, but the differences in pressure on which these instruments depend are so minute, that the pressure of the air in the room where the
recording part is placed has to be considered. Thus if the instrument depends on the pressure or suction effect alone,
and this pressure or suction is measured against the air pressure in an ordinary room, in which the doors and
windows are carefully closed and a newspaper is then burnt up the chimney, an effect may be produced equal to a
wind of 10 mi/h (16 km/h); and the opening of a window in rough weather, or the opening of a door, may entirely
alter the registration.
While the Dines anemometer had an error of only 1% at 10 mph (16 km/h) it did not respond very well to low winds
due to the poor response of the flat plate vane required to turn the head into the wind. In 1918 an aerodynamic vane
with eight times the torque of the flat plate overcame this problem.
Effect of density on measurements
In the tube anemometer the pressure is measured, although the scale is usually graduated as a velocity scale. In cases
where the density of the air is significantly different from the calibration value (as on a high mountain, or with an
exceptionally low barometer) an allowance must be made. Approximately 1½% should be added to the velocity
recorded by a tube anemometer for each 1000 ft (5% for each kilometer) above sea-level.
Notes
[1] Invention of the Meteorological Instruments, W.E. Knowles Middleton, Johns Hopkins Press, Baltimore, 1969
[2] "Hot-wire Anemometer explanation" (http:/ / www. efunda. com/ designstandards/ sensors/ hot_wires/ hot_wires_intro. cfm). eFunda. .
Retrieved September 18, 2006.
[3] Iten, Paul D. (June 29, 1976). "Laser doppler anemometer" (http:/ / patft. uspto. gov/ netacgi/ nph-Parser?patentnumber=3966324). United
States Patent and Trademark Office. . Retrieved September 18, 2006.
References
• Dines, William Henry. Anemometer. 1911 Encyclopædia Britannica.
• Meteorological Instruments, W.E. Knowles Middleton and Athelstan F. Spilhaus, Third Edition revised,
University of Toronto Press, Toronto, 1953
• Invention of the Meteorological Instruments, W.E. Knowles Middleton, The Johns Hopkins Press, Baltimore,
1969