Gas Analysis
Gas Analysis
Gas Analysis
where Pa is the partial pressure of oxygen within the cell, and Pb is the
partial pressure of oxygen outside the cell.
Since this effect is specific for oxygen, the instrument output is not affected
by the presence of water or CO2 .
However, hydrocarbons, hydrogen and other combustible gases will burn at
the operating temperature and result in an indication of less oxygen than is
actually present. The response of analysers using such cells is very fast.
Polarographic Cells
Polarographic cells are generally used to measure the partial pressure or
percentage of oxygen from injected samples, continuous streams or in
static gas monitoring.
They find maximum utility in the respiratory and metabolic laboratories.
Polarographic cells are based on the redox reactions, in a cell having
both the electrodes of noble metals.
When a potential is applied, oxygen is reduced at the cathode in the
presence of KCl as the electrolyte and a current will flow.
The cathode is protected by an oxygen permeable membrane, and the
rate a which oxygen reaches the cathode will be controlled by diffusion
through the membrane. The voltage-current curve will be a typical
polarogram.
A residual current flows in the cell at the low voltages.
The current rises with the increase in voltage, until it reaches a plateau
where it is limited by the diffusion rate of oxygen through the
membrane. For a given membrane and at a constant temperature, this
would be proportional to the partial pressure of oxygen across the
membrane.
The oxygen analyser incorporates oxygen sensor, which contains gold
cathodes, silver anode, potassium chloride electrolyte gel and a thin
membrane. The membrane is precisely retained across the exposed face
of the gold cathode, compressing the electrolyte gel beneath, into a thin
film. The membrane, permeable to oxygen, prevents airborne solid or
liquid contaminants from reaching the electrolyte gel. The sensor is
insensitive to other common gases. A small electrical potential (750 mV)
is applied across the anode and cathode
Conductometric Method
The conductometric method is convenient and is the most widely
used method for trace gas analysis. In practice, the sample gas is
passed through a cell containing a liquid reagent, which can react
with the gas of interest. The conductivity of the liquid is
measured before and after the reaction with the gas. The
difference in conductivity is proportional to the gas concentration
The metal oxide gas sensor works on chemi-resistance principle.
When the gas molecule interacts with metal oxide surface, it acts
as either an acceptor or donor. This changes the resistivity or
electrical conductivity of thin film.
The resistivity of the metal oxide semiconducting thin film
depends on the majority carrier in the film and also gas molecule
nature, i.e., whether it is oxidized or reduced in the ambient
temperature
Surface adsorption sites ensure appropriate interaction of gas
molecules with the material. In the case of n-type (electron being
majority carrier), the surface is generally get depleted with
electrons by the appearance of oxygen ion species (O−, O2−,
etc.), and upon exposure to sensing gas, these species react with
gas molecules to revert back electron on the surface, thereby
increasing conductivity.
The creation of these oxygen species on the surface is material
specific and broadly dependent of temperature. In the case of p-
type (hole being majority carrier), similar situation arises.
THERMAL CONDUCTIVITY ANALYSERS
The thermal conductivity of a gas is defined as the
quantity of heat (in calories) transferred in unit time
(seconds) in a gas between two surfaces 1 cm2 in area,
and 1 cm apart, when the temperature difference
between the surfaces is 1°C.
The ability to conduct heat is possessed by all gases, but
in varying degrees.
This difference in thermal conductivity can be employed
to determine quantitatively the composition of complex
gas mixtures.
Changes in the composition of a gas stream may give
rise to a significant alteration in the thermal
conductivity of the stream.
The changes in temperature can be detected by using
either platinum filament (hot wire) or thermistors.
A gas analysis based on the thermal conductivity
procedure presupposes binary gas mixtures or such gas
mixtures, respectively, which include a measuring
component, whose thermal conductivity differs
sufficiently from the thermal conductivity to the carrier
gas.
Examples: measurement of hydrogen in blast furnace
gases, the determination of argon in oxygen in the
process of air decomposition and of sulphur dioxide in
roasting gases in the production of sulphuric acid
Cont.
In a typical hot-wire cell thermal conductivity analyser, four platinum
filaments are employed as heat-sensing elements. They are arranged in a
constant current bridge circuit and each of them is placed in a separate
cavity in a brass or stainless steel block.
The material used for construction of filaments must have a high
temperature-coefficient of resistance.
The materials generally used for the purpose are tungsten, Kovar (alloy of
Co, Ni and Fe) or platinum
A reference gas is made to flow through all the cells and the bridge is
balanced precisely with the help of potentiometer D. When the gas stream
passed through the measuring pair of filaments, the wires are cooled and
there is a corresponding change in resistance of the filaments.
The higher the thermal conductivity of the gas, the lower would be the
resistance of the wire and vice versa.
Greater the difference in thermal conductivities of the reference and
sample gas, the greater the unbalance of the Wheatstone bridge.
The unbalance current can be measured on an indicating metre, or on a
strip-chart recorder.
Thermistors can also be used as heat-sensing elements arranged in a
similar manner, as hotwire elements in a Wheatstone bridge configuration.
Thermistors possess the advantage of being extremely sensitive to
relatively minute changes in temperature, and have a high NTC. When
used in the gas analysers, they are encapsulated in glass. Thermistors are
available which are fairly fast in response.
ANALYSERS BASED ON GAS DENSITY
It is known that the density of an ideal gas has a direct linear relation with the
molecular weight of that gas. Fortunately, all real gases behave as ideal gases
at room temperature and normal atmospheric pressure.
Figure illustrates the principle of operation of a gas-density balance. The
reference gas enters the balance at A, where it splits itself into two streams
and leaves the balance at D. Two detectors (B1 and B2 ), which may be either
hot wires or thermistors and mounted in the path of the two streams, are
connected as two arms of a Wheatstone bridge.
When the reference gas flows such that the flow is balanced, the two
detectors are equally cooled and the recorder would indicate a zero base line.
The sample gas enters the balance at C and it also splits into two streams.
It mixes with reference gas in the horizontal conduits and leaves at D. If the
sample gas has the same density as the reference gas, there will be no
unbalance of reference streams or of the detector elements.
If the sample carries a gas having a higher density than the reference gas, it
will cause a net downward flow, partially obstructing the flow in the lower
path, like A-B2 -D. This would result in raising the temperature of the detector
element B2 .
This in turn, increases the flow in the path A-B1 -D and causes more cooling of
the element B1 .
This temperature differential causes an unbalance in the bridge, the
unbalance being linearly proportional to the gas-density difference between
the reference and the sample gas.