Measuring the Wind
with Hot Metal
Supplemental
Information to "The Amateur Scientist"
(Scientific American, November 1995)
by Shawn Carlson
HOT BALL ANEMOMETRY
Thermal
anemometry measures wind speed by finding the rate at which flowing air
cools a hot piece of metal. The method has been around for a long time.
References to the technique go back as far as the 1840's. Today, researchers
use micro-fine platinum wires and sophisticated electronics to monitor
how turbulent processes at a million times a second. Unfortunately, such
complex and delicate equipment are not well suited for most amateur projects.
The devices are quite expensive and the probes break often.
Cup anemometers (what you normally see on a weather station) are bulky
and depend on a difference in dynamic pressure to determine the wind speed.
Their sensitivity scales as the square of the wind speed and this makes
them quite sensitive at large wind speeds but horribly insensitive at
low wind speeds. As a rule of thumb, cup anemometer should not be trusted
below 5 meters per second, unless they have been independently calibrated.
Thermal anemometers, on the other hand, are most sensitive at low wind
speeds and lose sensitivity at higher speeds. The anemometer described
in "The Amateur Scientist" (Scientific American, Nov, 1995) is quite accurate
starting below 0.1 meters per second and running all the up to at least
22 meters per second.
The anemometer described in "The Amateur Scientist" is ideal for amateur
use. It will respond to changing wind speeds in about 5 seconds-- fast
enough for many applications. It's small enough to fit inside a peanut
butter jar. It's inexpensive and durable. And it will perform under a
variety of environmental conditions from direct sunlight to the damp darkness
of a bat's cave.
AIR FLOW OVER THE
BALLS-- LAMINAR VS TURBULENCE
A hot object
cools in three different ways: radiation, conduction and convection. Heat
"radiates" from all objects as inferred light. But so little of the hot
ball's energy escapes in this way that we don't need to worry about it.
Now let's assume that the ball sits in still air. At first some heat will
be conducted away from the ball through the thermocouple wire. This can
be a significant source of heat loss early on, but since the wires and
the resistor are insulated, once the wire warms up very little heat escapes
through this path.
More important is the heat loss directly to the air. The ball will impart
heat into the air molecules that strike its surface. The air that touches
the ball is heated just a little bit, and, since hot air rises, it carries
this heat upward away from the ball. Cooler air then flows in from all
sides to fill the void. This new air is in turn warmed by the ball and
rises away to carry off additional energy. In this way, the hot ball sets
up a continuous air current that carries away heat. We call this process
"convection."
Of course, the hotter the ball is, the faster this will happen. A very
hot ball will heat the air around it very quickly, causing a sizable air
current to flow. A slightly warm ball will also be cooled in this way,
but at a much slower rate. The resister dumps heat energy into the ball
causing its temperature to rise until the energy leaving the ball equals
the energy being dumped into it.
As this self-generated current of air flows over the ball, different parts
of the ball achieve slightly different temperatures. Heat is most efficiently
conducted from the equator of the ball, and less so from the polls. You
can actually see this with your anemometer as follows: Turn on your resistor
and let the ball heat up until it reaches it's maximum temperature. Then,
very gently rotate the hot ball 90 degrees about the horizontal in place
by twisting the insulated thermocouple lead. You'll see your voltage readings
change as the heat flows around the ball to establish a new equilibrium.
A slight breeze flowing over the ball will conduct heat away. At slow
wind speeds, conduction and convection compete, but much above about 0.1
meter/second, the conductive losses to the wind dominate. This means that
the physical mechanism of heat loss changes between 0 and 0.1 meter/second
wind speed and this is important to keep in mind. It's tempting to calibrate
the anemometer at wind speeds above 0.1 meter per second and simply extrapolate
below that speed. This will not lead to reliable results because the physical
mechanism for the heat loss, and thereby the calibration curve, changes
below about 0.1 meter per second. If you want to make meaningful measurements
in this region, you'll need to take some measurements at wind speeds below
0.1 meter per second.
Above 0.1 meter per second conduction dominates. The balls aren't perfect
spheres because of the wires sticking out of them which interfere with
how the wind flows. If the wind speed isn't too fast, the air currents
flow in smooth continuous lines around the balls. We call such smooth
flow "laminar flow." As the wind speed increases, more air molecules are
brought against the ball per unit time and so more heat is taken away.
If the flow remains laminar, the temperature of the ball will fall exponentially
with wind speed.
Eventually, as the wind speed is increased ever faster, the air will rush
over so fast that smooth laminar flow is not longer possible. Eddies and
backwash develop behind the ball. The air flow becomes broken or "turbulent."
Turbulent flow removes heat much faster than laminar flow. If you take
your data carefully, you'll see the onset of turbulence in your calibration
curve. More about that later.
CALIBRATION
By far the
simplest way to get your anemometer calibrated is to place it in a wind
tunnel. So, before using the method described in The Amateur Scientist,
TRY TO GET ACCESS TO A WIND TUNNEL!
This may be easier than you think. Call your local universities and see
if any physics or engineering department has one has one. Tell the people
in charge of it what you're doing and you may very well get an hour on
the machine to calibrate your anemometer. Are there any aircraft or auto-makers
near you? Any engineering firms? Ask around. Only after you've exhausted
these options should you build your own calibration system.
You may calibrate the anemometer by comparing it to another anemometer.
However, if you have a standard cup anemometer, watch out! These anemometers
are notoriously inaccurate. Calibration errors as large as 200 percent
are common. The biggest errors for cup anemometers occur at the lowest
wind speeds because that is where they are least sensitive. Never trust
a cup anemometer that hasn't been independently calibrated. And even then,
never use a cup anemometer to calibrate a hot ball anemometer at speeds
below about 3 meters per second.
Professionals sometimes lay out a section of model railroad track down
a long hallway and affix their anemometer to a railroad car. They run
a string from the car to a tin can which they rotate with a very slow
(1 revolution per minute or so) electric motor. As the can rotates it
pulls the car along the rack at a known rate. (v = 2 PI x rf where is
the radius of the can, PI is 3.14159, r is the distance from the center
of motion, and f is the frequency of rotation or the number of revolutions
the can makes per unit time.) By using cans of different radius and rotating
the cans at different frequencies one can measure the anemometer's performance
at a number of different velocities.
A better way to do this is described in "The Amateur Scientist" and involves
using a ceiling fan motor to rotate the anemometer through the air at
a number of known speeds. The Scientific American article describes strapping
a digital voltmeter to the rotating armature, and reading this with a
strobe light. This technique works fine. But if you want to do a detailed
calibration, you may want a better way of reading the voltage.
GETTING THE SIGNAL
OFF THE PLATFORM
I do this
using ultrasound. The method is easy and inexpensive but you have to know
what you are doing. Ultrasound may sound exotic, but it's actually really
easy (if you know a little electronics) to generate, detect and use. Just
feed the signal into a voltage controlled oscillator (VCO, also known
as a "voltage to frequency converter") and use that to drive a piezoelectric
speaker at about 5 kHz. The VCO is a standard chip that's produced by
many different companies that only requires a capacitor and a resistor
to set the central frequency. The speaker can be purchased from Radio
Shack for a few dollars.
Put the speaker just above the center of the fan motor. I use a $3 microphone
from Radio Shack to pick up the signal. The microphone rests some distance
above the rotating platform. The output of the microphone goes into an
integrator circuit. Every time the microphone output goes high, the integrator
circuit puts a small but constant unit of change onto a capacitor. The
capacitor is part of an RC circuit with a time constant large compared
to the frequency of the sound pulses, but short compared to the time it
takes for the anemometer to respond to changing air speeds. The voltage
across the resistor is proportional to the frequency of the sound being
recorded by the microphone.
GENERAL CONSTRUCTION
TIPS
Here are
some useful tips to keep in mind while you're building the anemometer.
TIP: Cover Balls With Candle Wax To Avoid Splashing Them With Epoxy
Aluminized epoxy on the surface of the balls will alter their thermal
properties and lower the air speed at which turbulence becomes a problem.
It is vital that you do not have any excess epoxy marring the surfaces.
To avoid this problem, coat the balls with a layer of candle wax. I plugged
the holes with a dollop of silly putty and dipped the balls in melted
paraffin. You could, no doubt, drip candle wax onto the surfaces and spread
it around with your finger. Assemble the unit as described below. After
the epoxy has firmed up (about 30-45 minutes), but before it sets completely,
break off the wax and, using a sharp knife, scrap off any epoxy that may
be sticking up out of the holes.
TIP: Expose the Epoxy to Vacuum to Eliminate Air Bubbles
Mixing the resin with the hardener invariably adds many small air bubbles.
If allowed to cure, these air bubbles will weaken the bonds. Also, like
the air gap between the glass sheets inside a storm window, these bubbles
will reduce heat conduction through the epoxy, lengthening the time it
takes the ball to come to equilibrium. Neither problem is serious, but
they can be easily avoided if you have access to a vacuum pump and a bell
jar.
Pumping down on the freshly mixed epoxy causes the air bubbles to expand
and break out of the surface. The result is a nearly bubble-free mixture.
To avoid splatter, make sure to mix only small quantities in a disposable
Dixie cup. (Keep this tip in mind whenever you use epoxy.)
Of course, you'll add more bubbles when you insert the epoxy into balls
to glue the components in place. These can also be removed by placing
the whole assembly in a vacuum chamber just after it's put together but
before the epoxy has had a chance to set. Make sure to wipe off any splatter.
In fact, some of the material may bubble out and so you may have to repeat
this process a couple of times to fill the whole.
TIP: Mount the Hot Ball Above the Cold Ball
You should mount the hot ball above the cold ball. Otherwise, in still
air, air warmed by the hot ball will convect up over the cold ball and
warm it.
TIP: Color Code Your Wires
If you color code your wires by function, you'll find your circuits are
much easier to build and debug. For instance, you might make your ground
wires all black, your single wires red and your connection wires green.
TIP: Continuity Checks
Use the continuity tester on your voltmeter to verify the following connections:
A) Check the copper wire leads from the thermocouple as soon as they are
tapped for the signal leads. Make sure you have already doped the twisted
junctions with enamel but that you have not yet inserted them into the
balls. You should get continuity. If you don't, you'll need to remove
the enamel and rebuild the junction. If you do not get continuity, the
device will not work!
b) As soon as you insert the thermocouple junctions into the balls, but
before the epoxy sets, be sure that you have no continuity between the
copper lead wires and either of the balls. The thermocouple wires should
be electrically insulated from the spheres. If they are not, remove them,
remove the epoxy and the enamel and re-enamel the connections. The trick
is to make the junctions electrically insulated, but not thermally insulated.
c) After inserting the resistor inside the hot ball but before the epoxy
sets, make sure the resistor leads show no continuity between with the
hot ball. If there is continuity, you'll have to remove the resistor,
remove the epoxy and re-coat the resistor leads with enamel. Make certain
you only enamel up to the surface where the wire enters the resistor.
Do not get any enamel on the cylindrical surface of the resistor's body!
You want to let heat easily conduct out of the resistor into the ball.
TESTING THE CIRCUIT
After you've
built the circuit described in The Amateur Scientist, here are some easy
checks to make sure everything is working correctly.
CHECK 1: PRESS AN ICE CUBE AGAINST THE COLD BALL
The voltage should go down. If the voltage goes up, you've got the signal
leads reversed into the inputs on the op amp. Recheck the schematic. Make
sure the lead from the cold ball is inserted into ground and that the
lead from the hot ball is inserted into pin 3 of the Op Amp.
CHECK 2: PUT HOT BALL IN CUP OF HOT WATER
The voltage should go up. Ditto for check 1.
IF THE VOLTAGE DOES NOT CHANGE...
If the voltage does not change and is several volts positive or negative,
the op amp is probably saturated. One or more of your batteries may be
low. Check them with your voltmeter. Then check to make sure the battery
voltage is getting to everywhere in the circuit it's suppose to. Make
sure all of the parts of the circuit are at ground that should be at ground,
and that all the positive and negative connections are also correct. If
all that checks out, then perform continuity checks and make sure all
the closed circuit paths are closed. If you're still having problem, recheck
the wiring very carefully and make sure it exactly matches the schematic.
FIRST EXPERIMENT:
The first
experiment you should do is monitor the voltage output as the hot ball
heats up. To do this, measure the voltage just before you connect the
resistor to power and then again the instant after. The instant current
flows into the resistor you'll see the voltage jump by quite a few millivolts.
This is NOT due to the ball warming, because the jump occurs too fast
for the resistor to transfer a measurable amount of heat to the ball.
Rather, it occurs because the thermocouple is capacitively coupled to
the ball.
You should note this jump in your log book. Or better yet, record all
your data in a spread sheet program running on your home computer! Data
recorded on a personal computer can be processed so much faster and easier
than possible by hand. If you have access to a computer, use it!
The voltage you should use as your reference, that is the voltage before
the ball begins to warm, is the voltage you measure the instant AFTER
the resistor's power is turned on.
Then, record the voltmeter reading every 10 seconds. It's best to have
a colleague write down the numbers in a column in your laboratory notebook
or type them into a computerized spread sheet as you call them off.
You need an absolute commitment to honesty in data taking. Keep your eyes
rigidly fixed on the second hand of your timepiece. Wait until exactly
10 seconds has counted off. Then instantly snap your eyes to the voltmeter.
Write down or call out whatever number you see there the moment your eyes
focus. Often, the number fluctuates in the instant between the time you
see it and the time you look to the notebook. Always, ALWAYS, record the
very first number you see.
If you don't do this you may get yourself into trouble. Once you get into
the swing of things, it's impossible not to anticipate what number you'll
see when next you look at the voltmeter. Sometimes you'll see a different
number when you first look, but then before you look away to record the
datum the number will change into the number you expected. It's human
nature, but bad science, to write down the number you expected.
The battle between human nature and good science subtly creeps into every
scientific experiment you'll ever do. Sadly, many researchers, professional
and amateur, succumb to human nature and produce unreliable results. The
first defense against this is a deep appreciation for how easily we can
fool ourselves and bias our results. The second defense is to always establish
exactly what protocol, down to the very last detail, you will follow every
single time you record data and scrupulously follow through to the point
of obsession. This unwavering commitment to eliminating all human bias
from your experiments is very difficult to maintain but it is essential
to produce reliable data. Perfection in this matter must always be your
goal.
Keep taking data until the voltage measured remains constant for at least
2 minutes. For my apparatus, this took about 12 minutes.
When you've got all your data, make a second column and fill in the voltage
read minus the initial voltage, that is, subtract the voltage you measured
when the ball was cold from each voltage you measured. (See why it's nice
to have a computerized spread sheet?) Now graph the result.
This data should fit the following function:
V(t) = Vh(1 - exp(-t/t0)) + V0
V0 is the voltage your first measure before beginning the resistor begins
to heat. Vh is how much the voltage increased. It's easy to get from the
graph. Just subtract the initial voltage from the final voltage. Vh will
depend on how much power you're dumping into the ball and how effective
the atmosphere is at taking that energy away. If you insulated the ball
so very little heat escaped, this voltage would be quite high. If you
did the experiment in a tank of water, where the energy could be conducted
away very quickly, this voltage would be quite low. Also, if you dumped
a great deal of power into the ball this voltage would be high because
the ball would run hotter. If you lowered the power, the temperature,
and therefore this voltage, would drop.
t0 measures how fast the voltage rises. It depends on how much heat it
takes to raise the ball's temperature (the ball's heat capacity) and on
how much power the resistor dumps into it. If the ball's heat capacity
is large (if it takes a lot of heat to raise the ball's temperature 1
degree) then it will take a long time for the resistor to supply enough
energy to do that. If the resistor delivers a lot of power, the ball's
temperature will rise quickly. t0 is also easy to find. Multiply Vh by
0.368 and add that to V0. Clearly, the result will be about one third
of the way up the curve. Find the time it took for the voltage to reach
that value. That time is t0.
V0, Vh and t0 can tell you a lot about the heat capacity and thermal conductivity
of the system.
TIP: ALWAYS WAIT FOR THE BALL TO HEAT UP BEFORE MAKING MEASUREMENTS.
Now you know how long it takes for the ball to heat once the current is
turned on. Always make sure to wait at least that long before starting
to take data.
MORE ABOUT FOR CALIBRATING
THE DEVICE
The Amateur
Scientist column described a method to calibrate the anemometer using
a ceiling fan motor to swing the anemometer about at a known speed. Here
are some important fine points you will need to consider to do this calibration
correctly.
First: If you live in an area with a lot of radio noise, you may well
pick up excess voltage in the lead wires running from the anemometer to
the amplifier. This problem can be so severe that rotating the meter stick
90 degrees can cause fluctuations in the voltage by 30 millivolts or more!
You could place the device inside a Faraday cage (basically a box with
metal wire mesh on all sides) to absorb all the radio energy. Low pass
filters DO NOT solve the problem. The best thing to do is to avoid the
noise all together and take the device to a location where the noise is
less. You don't necessary have to head for the mountains. I was able to
find locations within 20 yards of my residence where the metal in the
surrounding structures blocked the radio signals enough to substantially
reduce the noise.
Even if you can find a place where this effect is small, the ionosphere
may cause you problems. Once while calibrating the device I noted a slow
steady drift in the signal voltage even though the device was isolated
from any air movement. Investigations showed that the drift was likely
due to radio energy bounced from the ionosphere.
These radio problems arise because the long signal leads between the anemometer
and the electronics box act as radio antenna and couple the radio energy
into the system. The best way to eliminate this problem is to mount the
anemometer directly to the electronics box, then move the entire electronics
box to change the wind speed.
CALIBRATION BETWEEN V to VCO and Vout.
One problem... If you attach the anemometer to the electronics box, the
box will create turbulent air as it whips around. The anemometer will
then run into the box's wake on the next pass. To reduce this problem,
I use a cardboard spoiler which I place in both and in front and behind
the box to make sure the air flow around the box is "smooth" (or more
correctly, "laminar"). If you go this route, make the electronics box
as small as possible.
EXPLORING TURBULENCE
Here's how
to use your calibration set up to explore the onset of turbulence.
The further out a point rests along the rotating arm, the faster it travels.
That means that the outer surface of the anemometer balls travel faster
than their inner surface. At some speed, the outer surface will just begin
to create turbulent flow around the outer edge of the ball. When that
happens, the temperature will take a sudden drop because turbulent flow
removes heat substantially faster than laminar flow. At a slightly higher
speed the inner surface will also create turbulence. Above this speed
the ball's temperature vs. speed will follow a different curve. With sufficient
care, you may be able to see this in your data.
Here are some issues you may want to explore:
- At what
speed does the onset of turbulence occur?
- What
can you say about heat conduction between the speeds where the inner
and outer rim of the ball create turbulence?
- If you
attach irregularities onto the surface, how does that affect the speed
at which turbulence becomes important?
- Try getting
balls of different size and materials. What effect does shape, substance
and size have on the onset of turbulence?
Researchers with SAS are beginning to explore this issue. I would be delighted
to see any results you obtain.
ONCE CALIBRATED...
your hot
ball anemometer is a useful and sensitive device. It is best used for
measuring low to medium wind speed (less than about 30 meters/second),
and it can be placed in all sorts of places where a conventional anemometer
just won't fit.
If you're looking for interesting science projects, here are just a few:
- Measure
how effectively a bird's nest cuts the chill of a winter storm. You
can do this by putting a bird's nest in a constant source of wind and
then measuring the wind speed at several locations above and inside
the nest.
- Measure
how effectively a thicket protects it's inhabitants from wind. First,
measure the wind speed at different distances in front of a strong fan.
Then place the fan in front of the thicket (you may need a portable
generator to power the fan) and measure the wind speed a several different
heights and distances inside the thicket.
- Measure
how a fan's efficiency changes as it's speed is increased. To do this
you'll need to measure the wind speed coming out of the fan for several
different fan settings. You'll also need to measure the power consumed
by the fan. You can get that by measuring the current being fed into
the fan, and the voltage across the fan's terminals. The power is just
the product of these two numbers. Working with electricity is always
potentially hazardous so be absolutely certain you know how to measure
the current and voltages safely. If you are under 18, be sure to conduct
these measurements under the supervision of an adult who understands
electricity and it's hazards.
- Measure
the wind speed at different, but connected, gopher holes. Figure out
how to measure the speed of the air moving somewhere deep inside the
burrow. Can you think of a way to also measure the wind's direction
(up the shaft or down)? How do these subterranean burrows get ventilated?
- How much
wind must an ant contend with while it's on an ant trail? How much work
(force x distance) must it do to move itself against the wind? How does
this affect how often it must eat?
- Measure
the wind speed at different heights in a forest. How does the tree cover
protect the life that inhabits different strata in different kinds of
forests? How can you quantify the density of plant life in the forest?
- Develop
a way to measure the wind speeds at different places around a bird in
flight. Think about using a wind tunnel to provide the wind for the
bird to fly against.
- Study
the updrafts near cliffs. Compare with what you get for similar studies
near the top of a tall building.
- Map out
the air flow patterns between large buildings. Can you relate the speed
and direction to physical features of the buildings?
- Identify
a microclimate that interests you and use the hot ball anemometer to
measure the wind speed under various conditions of importance to the
animals who live there.
Also, please do share your results of your experiments. If you use any
of these ideas in a science fair, or if this inspires you to do other
explorations, please let me know!

Shawn Carlson
scarlson@sas.org
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