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United Sensor Gas Sampling probes have been
designed for accurate sampling of burner exhaust
gases primarily used in efficiency studies of
combustion and they
have been endurance tested
in routine test work.
An internal
static tap is located in the inner flow
passage of the probe near the sample
inlet as
shown in Fig. 1 so the static pressure of the
sampled
gas can be measured. In order to obtain
a true sample, it has been
found necessary to draw
off the gas at the same velocity as is flowing
in the
duct. If the sample is accelerated or decelerated as
it
is drawn into the probe, it will not be a true
average since, in the first
case, a disproportionate
share of low density components will be drawn
in,
and in the second case, too much of the high
density components
will be sampled.
This would not be true in a perfectly homogeneous mixture of gases, but in the region
most sampling is done the mixture is not homogeneous since the fuel particles
are usually still burning or have just completed burning and the products of
combustion are concentrated in "slugs" of gas interspersed by lighter, unburned
air.
The gas velocity in the duct is proportional to:
Where Pt, Ps, and d are total pressure, static
pressure, and density, and K
is a constant.
The gas velocity in the probe inlet is proportional
to:  |
Pt1 will automatically equal Pt2 since no work is
done on the gas in drawing
it into the probe so if
Ps1 is made equal to Ps2 it can be seen that V1will
equal V2. Since the static pressures are equal and
there
is no change in temperature, d1 and d2 will
also be equal.
By
measuring the static pressure Ps1 with a static
tap in the wall of the duct
at the same cross section
and Ps2 with the internal static tap on the
probe,
the two can be equalized by adjusting the sampling<
suction.
In
some cases, the resulting volume of gas flow
through the sample
probe is too high or too low for
the gas sampling apparatus.
The orifice inlet
diameter is picked to be high enough to give a flow
at the lowest duct velocity V1 sufficient for
analysis purposes and the
excess gas sampled at
higher duct velocities is by-passed around the
analyzer by a bypass line and valve.
United Sensor Sampling probes are made in three types:
Type A
Type A is uncooled, of welded construction,
suitable for use up to 2000°F
and is the smallest.
Type B
Type B can be used either as a heated or cooled
probe. The cooling
passages are especially
designed for unrestricted flow of cooling or
heating
fluids. For some applications, it is important to
keep
the sampled gas above500°F to the analyzer to
prevent condensation of evaporated
hydrocarbons.
In this case, the probe is heated by blowing hot
air
through the cooling passages. This is more
satisfactory than
trying to heat it with anelectric coil because the variation of heat loss conditions
from the surface of the probe makes it almost
impossible
to maintain an even temperature. For
higher temperatures, the probe can be
kept hot
enough to prevent condensation but cool enough
not to melt
by blowing unheated shop air through
the coolant passages. Above
3000°, even with
water cooling the stainless steel tip on the Type B
probe it would burn out. Therefore, Type C is
recommended.
Type C
Type C probes have a copper tip, which has a high enough conductivity
to prevent burning out at the highest temperatures and velocities.
Since the tip is easily damaged, it is not recommended for lower temperature
applications.
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