LFE's unique thermal conductivity detector is the heart of LFE's CONTHOS process TCD gas analyzer and has proven itself since 1979 in a wide range of applications. The TCD combines quick response, high corrosion-resistance and high-temperature capability without compromise. Further features are its extraordinary measurement stability, low range capabilities as well as highly suppressed ranges.
LFE's thermal conductivity detector is available in an OEM (original equipment manufacturer) version which can be implemented into a customer's gas analyzer (system). The TCD OEM version can be integrated into in a standalone instrument or be used to complement other analysis principles such as for example NDIR/UV, Laser, or FTIR.
Due to its high temperature capability LFE's OEM TCD can be integrated into thermostat controlled analyzer systems (e.g. 80 - 120°C) or close-coupled to customer high-temperature systems (up to 180°C).
Such a combination of high-temperature NDIR/UV with LFE's high-temperature TCD has been approved in several tough process control applications from a well-established process analyzer company with high-temperature solutions between 80° and 180°C since 1985.
Meanwhile the OEM version of the LFE TCD has been optimized making it attractive for more companies to round off their gas analysis portfolios.
A special infallible (fail-safe) OEM version of the TCD is available for flammable and even explosive gases requiring special measures to be fulfilled.
In conventional gas analyzers utilizing the principle of thermal conductivity a heated object is suspended in a volume containing the sample gas. Electrical energy passed through the object results in the object heating up and attaining an equilibrium temperature which is primarily dependent upon the thermal conduction properties of the surrounding gas. This temperature is normally measured directly as a change in the electrical resistance of the heated object itself.
LFE´s unique principle modifies this "classical" method by spatially and electrically decoupling the heated element from the temperature sensing element. The specially designed geometry of the TCD cell in conjunction with the decoupling effectively suppresses undesired competing thermal effects (i.e. free and forced convectional effects). The result is an instrument whose quick, stable response requires no compromise between gas flow and response time.
Technical specifications subject to change without notice | |
Electrical interface | |
Power requirements | 24 VDC; 25 VA max. (during initial heat-up phase) |
Data / service interface | RS232 or Ethernet (Telnet protocol) in conjunction with isolated logic level converter
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Dimensions and Weight | |
Dimensions | refer to dimensional diagram found in product data sheet |
Weight | 1.2 kg |
Materials in contact with sample gas | |
TC Detector | Al2O3 ceramic and sapphire, glass and SiOx-coated Pt measuring filaments |
Gas lines | Standard model with synthetic tubing: PTFE / PFA Model with optional stainless steel tubing: SS 321 (similar to 1.4541) |
Measuring characteristics | |
![]() | Note: The technical data is valid for operation of the OEM TCD within LFE's CONTHOS gas analyzer. The overall performance data for a particular implementation may depend on the chosen system integration, interfacing and signal processing options. |
Measuring principle | Thermal conductivity (TCD). Difference in thermal conductivity (Δλ) of various gases |
Measured quantity | Concentration of a particular gas component in binary and quasi-binary mixtures |
Gas interference | For the analyzer configuration, the knowledge of the sample gas composition is necessary. In complex (non-binary) gas mixtures, the measurement results may be affected by interfering components. Through the use of dynamic interference correction, the interference effects can be suppressed under certain circumstances. This must be implemented by the customer within his system or in conjunction with the appropriate optional interface expansion modules. Physical interference suppression is sometimes possible with certain gas combinations due to the wide temperature range of the CONTHOS' TC detector. |
Measuring ranges | Measured value signal output as raw value lowest range: 0 - 0.5% H2 in N2 or 99.5-100% H2 in N2 (or equivalent Δλ) |
Calibration | The device outputs RAW values that are neither fine-calibrated nor linearized. The customer must provide the appropriate algorithms. |
Detector operating temperature | TCD standard operating temperature: 70°C |
Warm-up time | dependent upon TCD operating temperature as well as the ambient temperature: |
Response time t90 | ≤ 3 sec (at 60 l/h gas flow and minimum signal dampening level) |
Influence of gas flow | between 3 - 30 l/h: < 0.5% of range span for a gas flow change of ±10 l/h Higher flow rates up to e.g. 120 l/h are possible. At these higher flow rates it is recommended that the analyzer be calibrated at the operating flow rate. |
Pressure drop | approx. 0.7 mbar at 60 l/h N2 |
Pressure influence | The TCD principle has a normally negligible pressure dependency. At very low ranges it can be seen as a proportional signal offset. Gas specific order of magnitude: < 0.02% H2 equivalent per 100 mbar |
Detection limit 1 | ≤ 0.5% of span (at signal dampening level: 1 sec) |
Reproducibility 1 | ≤ 0.5% of span |
Response drift 1 | Zero: ≤ 1% of span per week |
Influence of inclination | no influence |
Sample gas requirements | |
Sample gas temperature | min.: +5°C |
Sample gas dew point | Dew point low enough so as to prevent condensation in the gas paths under all ambient temperature conditions |
Particles in sample gas | The sample gas must be free of particles and aerosols. |
Sample gas pressure | max. 300 mbar above atmospheric pressure |
Sample gas flow | minimum: 3 l/h |
1 at constant temperature and pressure
LFE OEM-TCD Application questionnaire
Technical specifications subject to change without notice