The Steam Battery: A Low-Cost Science
Experiment Performed with Ordinary Materials
Mark Valentine, Electrical Engineer
Introduction
Most semiconductor components are vulnerable
to static electricity, also referred to as electrostatic discharge
(ESD). These components are usually packaged with a piece
of black, electrically conductive foam (referred to hereafter
as “ESD foam”) placed over their electrical leads as a form
of protection from ESD. Because ESD foam has a large internal
surface area within a relatively small volume, it is plausible
to assume that certain changes in the environment surrounding
a sample of ESD foam might cause observable changes in the
electrical resistance of the sample.
Initial investigations revealed that a sudden
change in humidity from my breath did indeed result in a change
in resistance for several ESD foam samples. However, the resistance
readings appeared erratic and occasionally read as negative
on the digital multimeter (DMM) used for the measurements.
I soon found that the ESD foam samples were producing a DC
voltage, which led to the formulation of a new hypothesis
and experiment to address the means by which humidity could
be generating the observed DC voltage in an apparently uniform
ESD foam sample. Specifically, the experiment was designed
to determine whether the DC voltage in the ESD foam settles
into a steady state with the continuous localized application
of humid air. It was also designed to determine the relationship
between the polarity of the DC voltage across the sample and
the relative position of the region on the sample directly
exposed to the high-humidity airflow. If the experiment were
to be framed within the guidelines of the scientific method,
it might be expressed as follows:
Problem : Explain how an
apparently uniform sample of ESD foam can produce a DC voltage
in response to sudden exposure to high-humidity air.
Hypothesis: The polarity
and persistence of the observed DC voltage between two electrodes
in contact with a sample of ESD foam depends on the humidity
gradient created and maintained within the sample with respect
to the position of the electrodes.
Experiment: First, verify
that the DC voltage between two electrodes in contact with
the ESD foam sample can be sustained by constant and localized
application of humid air (breath) on the sample (which should
create a humidity gradient within the sample with respect
to the two electrodes). Second, apply localized humid air
to the opposite end of the sample (which should reverse the
previous humidity gradient with respect to the two electrodes)
and verify that the generated DC voltage is sustained with
reversed polarity.
Conclusions: The application
of humid air, and thus the formation of a humidity gradient,
was not carefully controlled in the previous resistance experiments
in which DC voltage generation was first observed in ESD foam
samples. If the expected results of the present experiment
do not occur, the hypothesis is incorrect, because the uncertainty
in the humidity gradient that plagued the previous experiment
has been eliminated. If the expected results do occur, then
they lend qualitative support to the hypothesis but reveal
further development is needed to explain the detailed relationship
between the high-humidity air stream and the polarity and
magnitude of the generated DC voltage.
Building the Apparatus
Figure 1 shows the apparatus I used to conduct
the experiment previously described. There are many other
possible designs. The only real requirements are that the
ESD foam sample under test be secured firmly to a non-conducting
surface by two electrodes that use the same metal (such as
aluminum foil, which can be seen in the photograph) to make
electrical contact with the sample, and that humid air can
be directed to opposite ends of the sample.

Figure 1. Sample pieces and apparatus (shown
with one sample piece installed) used to perform the ESD foam
experiment.
The following supplies are required for constructing
the apparatus shown in Fig. 1:
Perfboard—available from Radio
Shack.
Two large paperclips.
Two pieces of aluminum foil,
each cut to 5 cm x 2.5 cm (2” x 1”).
Ten cm (2 ft) of fishing line.
One new soda straw (please see
important WARNING below under “Conducting the Experiment”).
One paper towel.
Five black ESD foam samples
cut to approximately 2.5 cm x 1.25 cm x 0.6 cm (1.0” x 0.5”
x 0.25”).
The following tools will be required to build
the apparatus and conduct the experiment:
Digital Multimeter (manual ranging
DMM preferred in order to prevent erratic data readings that
can occur with auto ranging; analog meters will not work due
to their relatively low input impedance).
Stopwatch (or clock with second
hand).
Spring-loaded probe clips.
Needle-nose pliers.
Scissors.
The first step in building the apparatus
is to fashion two supporting electrodes from the two paper
clips. Use the needle-nose pliers to bend the paperclips into
the shape illustrated in Figure 2, noting for reference that
the electrodes should be about 2 cm (0.75 in) wide.
Figure 2. Illustration of paper clip electrode.
Insert the free ends of the electrodes through
holes in the perfboard so that the two electrodes will be
situated in a symmetrical fashion with the innermost segments
of the electrodes being slightly less than 2.5 cm (1 in) apart,
as shown in Fig. 1. Bend the inserted ends of the electrodes
(resembled by the dashed lines in Fig. 2) flat against the
bottom side of the perfboard so that they point toward the
outermost perfboard edges. Then, using the needle-nose pliers,
tightly compress the resulting elbow-shaped bends that pass
through the holes so the electrodes will be held tightly in
place.
Wrap one piece of aluminum around the innermost
segment of each electrode. It should be wrapped tightly, but
it is acceptable for the aluminum to roll on the electrode.
Install a piece of ESD foam with opposite ends secured lightly
under these aluminum coverings. Adjust the shape of the electrodes
so the contact force is firm enough to secure the foam against
the perfboard, but light enough to allow the foam to be removed
and replaced easily.
Next, cut the fishing line into four equal
pieces, and cut the soda straw in half. Place a round stopper
made from a tightly rolled piece of paper towel snugly into
one end of each straw half (the stopper should restrict foam
fibers from traveling back through the straw; it also restricts
the speed of the airflow through the straw). Position each
piece of straw so that the end with the stopper is pressed
against one end of the foam sample, and the other end projects
out beyond the edge of the perfboard. Secure both pieces of
straw into these positions with fishing line wrapped over
the ends of the straws and threaded through the underlying
holes in the perfboard. Tie each piece of fishing line in
a double knot so the straws are held firmly enough to the
perfboard to prevent slipping but not so tightly that the
straws cannot be replaced. Trim all the free ends of string.
This completes the assembly of the apparatus.
Conducting the Experiment
WARNING: Only one person
should use the apparatus. If more than one person uses the
same straws, there is a risk of contracting bacterial meningitis.
Young people, including college students, should not
share drinking straws, cups, or eating utensils for the same
reason.
The above warning is issued because it is
necessary to blow through the straws to conduct the experiment.
Breath has high relative humidity, which is the reason condensation
forms on a mirror brought in close proximity to exhaled air.
Breath therefore provides a convenient and safe source of
humid air if the above warning is heeded.
The experiment is conducted according to
the steps that follow. Following this procedure, there is
a section devoted to data collection that shows my data for
the experiment in Table 1. This might prove useful, because
a formatted table for data collection should be prepared before
performing the experiment. Also, it may be helpful to refer
to Fig. 3, a photograph of the complete apparatus used for
the experiment.

Figure 3. Apparatus connected to DMM.
Perform the following experimental procedure
on each of the five ESD foam samples:
Secure an ESD foam sample to
the apparatus.
Attach the probes of the DMM—using
the spring-loaded clips—to the electrodes of the apparatus
(the portion of the electrodes that are perpendicular to the
face of the perfboard work well for this).
Measure and record the resistance
of the sample and record.
Reverse the probe connections
at the DMM jacks; repeat step (3).
Change the mode setting and
the probe jack connections of the DMM to measure DC voltage
(black to “-“; red to “+”).
Using a pressure similar to
that for blowing up a balloon, apply slow deep breaths to
the straw closest to the electrode connected to the black
probe of the DMM for five minutes, recording the voltage observed
initially and then every 30 seconds. Bear in mind that some
samples will not produce a large voltage, so excessive pressure
is not necessary. Also, if this activity results in light-headedness,
please slow down!
After five minutes, stop applying
breaths. Record the elapsed time between the time of the last
applied breath and the time required for the magnitude of
the voltage to decay to the magnitude of the initial voltage,
or to the magnitude of 25 mV, whichever comes first.
Apply slow deep breaths to the
other straw for 5 minutes, recording the voltage observed
initially, and then every 30 seconds.
After 5 minutes, stop applying
breaths. Record the elapsed time between the time of the last
applied breath and the time required for the magnitude of
the voltage to decay to the magnitude of the initial voltage
or to the magnitude of 25 mV, whichever comes first.
Data Collection
Table 1 shows the data I collected while
performing the previously described experiment. When performing
this experiment, note that readings on the DMM will fluctuate,
and that the voltage data shown here are “snapshots” of the
values displayed on the DMM at the designated time intervals.
Sample # |
1 |
2 |
3 |
4 |
5 |
Resistance (ohms) |
230 K |
> 2 Meg |
> 2 Meg |
65 K |
> 2 Meg |
Reverse-polarity Resistance
(ohms) |
230 K |
> 2 Meg |
> 2 Meg |
61 K |
> 2 Meg |
Vo, Forward Air Flow
(volts) |
0.000 |
0.000 |
-0.018 |
0.000 |
0.000 |
Voltage at 30 sec |
0.165 |
0.022 |
0.196 |
0.004 |
0.007 |
Voltage at 60 sec |
0.220 |
0.030 |
0.143 |
0.007 |
0.004 |
Voltage at 90 sec |
0.230 |
0.037 |
0.122 |
0.013 |
0.010 |
Voltage at 120 sec |
0.260 |
0.042 |
0.176 |
0.023 |
0.020 |
Voltage at 150 sec |
0.224 |
0.047 |
0.079 |
0.020 |
0.009 |
Voltage at 180 sec |
0.160 |
0.05 |
0.139 |
0.172 |
0.005 |
Voltage at 210 sec |
0.199 |
0.050 |
0.169 |
0.380 |
0.006 |
Voltage at 240 sec |
0.219 |
0.050 |
0.106 |
0.027 |
0.004 |
Voltage at 270 sec |
0.292 |
0.053 |
0.127 |
0.512 |
0.013 |
Voltage at 300 sec |
0.225 |
0.053 |
0.149 |
0.330 |
0.008 |
Decay Time to |25mV|
or Vo (sec) |
653 |
358 |
704 |
170 |
1104 |
Vo, Reverse Air Flow
(volts) |
0.026 |
0.010 |
-0.003 |
0.001 |
-0.006 |
Voltage at 30 sec |
-0.170 |
0.030 |
-0.199 |
-0.002 |
-0.016 |
Voltage at 60 sec |
-0.225 |
-0.044 |
-0.069 |
-0.009 |
-0.017 |
Voltage at 90 sec |
-0.080 |
-0.089 |
-0.067 |
-0.003 |
-0.009 |
Voltage at 120 sec |
-0.108 |
-0.104 |
-0.199 |
-0.015 |
-0.034 |
Voltage at 150 sec |
-0.233 |
-0.107 |
-0.199 |
-0.020 |
-0.038 |
Voltage at 180 sec |
-0.177 |
-0.108 |
-0.150 |
-0.020 |
-0.038 |
Voltage at 210 sec |
-0.255 |
-0.108 |
-0.155 |
-0.011 |
-0.021 |
Voltage at 240 sec |
-0.155 |
-0.112 |
-0.154 |
-0.014 |
-0.013 |
Voltage at 270 sec |
-0.175 |
-0.115 |
-0.165 |
-0.014 |
-0.022 |
Voltage at 300 sec |
-0.188 |
-0.112 |
-0.154 |
-0.022 |
-0.033 |
Decay Time to |25mV|
or Vo (sec) |
208 |
943 |
536 |
244 |
46 * |
* Note:For sample #5, the Decay Time was
measured as the time for the sample to reach a magnitude of
6 mV, since the voltage magnitudes for this sample were mostly
below 25 mV except for a few outliers.
Table 1: Data collected from five samples
during the experiment.
Analysis and Conclusions
For all samples, the voltage was observed
to fluctuate but not decay during the portion of the experiment
where the humid air was steadily applied. For certain samples
the resistance was sufficiently high to allow for the possibility
that the meter was registering electrical noise. However,
for other samples the resistance was low enough to eliminate
that effect as the one responsible for voltage buildup. Furthermore,
the polarity of the voltage did reverse for each sample when
the flow of high-humidity air was reversed, which is critical
to the accuracy of the hypothesis. Therefore, the trends in
the data do not challenge the hypothesis.
There are, of course, other general observations
that lend support to the hypothesis by eliminating other mechanisms
that might be producing the observed DC voltage. For example,
the condensed water from breath should be relatively distilled,
preventing it from acting as an electrolyte for an electrochemical
reaction. Furthermore, high humidity would tend to suppress
the buildup of static electricity, and because the airflow
through the straws is restricted, static electricity probably
would not develop even if the ambient air were sufficiently
dry. These facts tend to refute the possibility that the observed
DC voltage is a form of triboelectricity. However, while these
observations are encouraging, it is obvious that much more
detailed experimentation is needed before the hypothesis can
be confirmed.
Going Further
There are many possibilities for more sophisticated
experiments. For one thing, it would be interesting to include
the detailed chemical composition for each sample of ESD foam
as part of the experimental data. Another interesting experiment
would be to monitor the buildup and decay of the DC voltage
on an oscilloscope to get a clearer picture of the voltage
fluctuations on small time scales. Yet another experiment
might simultaneously monitor and record the voltages at several
points on the surface of the ESD foam sample. Mechanical variations
on the experiment are also possible. For instance, steam from
heated water could be drawn through the ESD foam sample using
a weak vacuum pump, which might produce a more reliable humidity
gradient within the sample. However, while there are many
possibilities for new experiments, they would all share the
goal of testing any hypothesis that explains the generation
of the observed DC voltage in the ESD foam.
I hope that you will find this experiment
enjoyable and inspiring. However, the real purpose of this
experiment is to evoke appreciation for the scientific method,
which is not a mere formality for confirming an expected result,
but rather a process that equips the experimenter to make
new discoveries. 
|