Chapter 1. Features and Capabilities
1.3 Theory of Operation
The XMTC measures the concentration of a gas in a binary gas mixture by measuring the thermal conductivity of the
sample gas and comparing it to the thermal conductivity of a selected reference gas.
Two ultra-stable, glass-coated thermistors are used: one in contact with the sample gas, and the other in contact with a
selected reference gas. The thermistors are mounted so that they are in close proximity to the stainless steel walls of the
sample chamber. The entire sensor is heated to 55°C/131°F, (or 70°C/158°F) and the thermistors are heated above the
sensor temperature using a constant current source. The thermistors lose heat to the walls of the sample chamber at a
rate that is proportional to the thermal conductivity of the gas surrounding them. Thus, each thermistor will reach a
different equilibrium temperature. The temperature difference between the two thermistors is detected in an electrical
bridge circuit. It is then amplified and converted to a 4-20 mA output proportional to the concentration of one of the
constituents of the binary gas mixture. For example:
•
To measure 0 to 25% H
calibration, the zero gas would be 100% N
•
To measure 90-100% H
the zero gas would be 90% H
Note: The XMTC has polarity adjustment jumpers which permit the measurement of gases (such as CO
relative thermal conductivity less than air/nitrogen.
Appendix A, Supplemental Information, contains a table of Relative Thermal Conductivity of Common Gases. Figure 1
below shows some of these values graphically.
0
1.0
2
in N
, the reference gas would be air (2-port version, sealed reference gas), and for
2
2
in N
, the reference gas would be 100% H
2
2
in N
, and the span gas would be 100% H
2
2
2.0
Figure 1: Relative Thermal Conductivity of Some Common Gases
(i.e. 0% H
) and the span gas would be 25% H
2
2
3.0
4.0
2
(4-port version, flowing reference gas),
2
(the same as the reference gas).
2
5.0
6.0
in N
.
2
) that have a
2
7.0
XMTC User's Manual
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