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Measurement of Pressures and Temperatures

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Presentation on theme: "Measurement of Pressures and Temperatures"— Presentation transcript:

1 Measurement of Pressures and Temperatures
Prof. Václav Uruba IT ASCR, CTU Praha, UWB Plzeň

2 State of Fluids Liquids Gases – equation of state
Any physical quantity is function of temperature T and pressure P Ideal gas - air February 27, 2019

3 State Quantities Temperature – thermometers Pressure – manometers
Both STATIC – flowing fluid Total (stagnation) static February 27, 2019

4 High velocities T – static temperature
T0 – total (stagnation) temperature Adiabatic Compression February 27, 2019

5 Temperature on a sensor
We measure recovery temperature For February 27, 2019

6 Pressure February 27, 2019

7 Pressure Units Pascal [Pa = N/m2] mm H2O (9.81 Pa)
mm Hg, Torr ( Pa) bar (106 dyn/cm2 = 105 Pa) atm ( x 105 Pa) – sea level at (kgf/cm2 = x 105 Pa) – tech. atm. psi (Pound-force per square inch = 6895 Pa) February 27, 2019

8 Manometers Types Principles Differential pressure - PSID
Absolute pressure (rel. to ref.) - PSIA Gauge pressure (rel. to atm.) - PSIG Vacuum pressure (negative gauge) Sealed pressure (rel. to atm. at sea level) - PSIS Principles Liquid column Elastic parts February 27, 2019

9 Liquid Column Water k = 9.8 Alcohol k = 7.6 Mercury k = 133
February 27, 2019

10 Technology Elastic parts Deformation indication Bourdon tubes
Diaphraghms Bellows Deformation indication Mechanical Piezoresistive strain gauge Capacitive Electromagnetic Piezoelectric Optical Potentiometric February 27, 2019

11 Bourdon tubes Sealed tubes February 27, 2019

12 Elastic elements February 27, 2019

13 Capacitance measuring
Robust Linear Precise Stable Big Low frequency February 27, 2019

14 Piesoresistive diaphragms
High sensitivity High frequencies Small Temperature influence Nonlinear Fragile February 27, 2019

15 Pressure scanners Piesoresistive Up to 64 sensors Electronics
February 27, 2019

16 Pressure-Sensitive Paints
Deactivation of photoexcieted molecules of organic luminosphores by oxygen molecules (quenching). Discovered by H. Kautsky and H. Hirsch in 1935. Certain materials are luminous when excited by the correct light wavelength. The luminescence is dependent on air pressure. February 27, 2019

17 Pressure-Sensitive Paints
Qualitative Only high pressures α high velocities Surface pressure distribution February 27, 2019

18 Temperature February 27, 2019

19 Methods Thermal expansivity Electrical sensors Optical methods
February 27, 2019

20 Method of thermal expansivity
Liquid in Glass Thermometers Filled System Thermometers Bimetallic Thermometers February 27, 2019

21 Electrical sensors Thermocouples
Resistance Temperature Detectors (RTDs) Thermistors (THERMal resISTORS) February 27, 2019

22 Thermocouples + Cheep Small, small inertia Big range -
Small sensitivity Worse precision Reference February 27, 2019

23 Resistance Temperature Detectors
platinum: + Precision, stability Simple Range ( K) - Bigger Price wire 2w, 3w, 4w film February 27, 2019

24 Thermistors Semiconductors (oxids of Mn, Ni, Co, Cu, Fe, Ti)
Steinhart-Hart equiation + Sensitivity - Nonlinear Low temp (upto 300°C) February 27, 2019

25 Optical Methods Liquid crystals Radiation Thermometers (RTs)
Thermal Imaging (Thermography) Laser-Induced Fluorescence Rayleigh scattering Temperature of surface!!! Temperature of fluid February 27, 2019

26 Liquid-crystal temperature-sensitive films
Hydrophobic derivatives of polyvinyl alcohol and cholesteric liquid crystals Encapsuled (friction) Temperature -5 to +150°C Thickness 30-50μm High sensitivity February 27, 2019

27 Radiation Thermometers (infrared)
Non-contact sensors Electromagnetic radiation received Range -40 °C to 3000 °C February 27, 2019

28 Thermal Imaging Infrared range of the electromagnetic spectrum (9 000–14 000nm) Black body radiation law (Planck) SURFACE !!! February 27, 2019

29 PLIF See more in „Optical methods“ Planar laser-induced fluorescence (planar-LIF) - instant whole-field concentration or temperature maps in liquid flows. February 27, 2019

30 Rayleigh scattering The Rayleigh signal is dependent on:
See more in „Optical methods“ The Rayleigh signal is dependent on: Laser intensity Scattering cross section Number density If species composition and pressure are known in the gas the gas temperature can be determined from imaging of the Rayleigh scattering. February 27, 2019


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