Methods to calibrate a critical nozzle and flowmeter using reference critical nozzles

2000 ◽  
Vol 11 (4) ◽  
pp. 293-303 ◽  
Author(s):  
Masahiro Ishibashi ◽  
Masaki Takamoto
Author(s):  
Masahiro Ishibashi

The paper describes primary calibration of high-precision nozzles (HPNs), which have ideal geometries, at critical condition, theoretical calculation of the discharge coefficient to be verified by the primary calibration, concept of fluid dynamical standard using HPN, precise measurement of boundary layer transition in HPNs in terms of flowrate, superfine structure in the critical flowrate, discrepancy which can occur between primary calibrations and field applications of critical nozzles, and 3D flow velocity field measurements based on recovery temperature, which visualizes many interesting phenomena in axi-symmetric transonic flow as shock interactions, acceleration by edge, reflection of shocks, Fano flow and so on.


Author(s):  
Junji Nagao ◽  
Shigeru Matsuo ◽  
Mamun Mohammad ◽  
Toshiaki Setoguchi ◽  
Heuy Dong Kim

2020 ◽  
Vol 24 (5 Part A) ◽  
pp. 2667-2687
Author(s):  
Zhipeng Xu ◽  
Feipeng Xu ◽  
Dailiang Xie

Piston prover has been widely used as a gas flow standard for its advantages of high accuracy in standard volume, flow stability and repeatability. It has also been employed as the primary gas flow standard in many countries to calibrate meters. However, it is difficult to ensure the uniformity of the inside dimension of the piston, thus the application of conventional piston provers are limited by the maximum calibration flow generated by the piston cylinder volume. In this paper, an improved piston gas prover that mainly consists of two uniform plungers was proposed. Their external diameter constitutes the flow standard. The plungers are driven by servo motor, and the high speed fieldbus EtherCAT has been introduced as the control unit. Hence the two pistons could work collaboratively and operate in three modes: single-piston mode, double-pistons parallel mode, and double-pistons reciprocating mode. Besides generating steady-flow rate, the double-plunger prover can even produce an unsteady-flow rate which could be used to research the dynamic characteristics of flow meters. The structure and working principle of the three modes were carefully introduced. Then experiments for calibrating critical nozzles were carried out, and the results show that the repeatability of the discharge coefficient could be better than 0.06%, and the pressure fluctuation during the process was less than 50 Pa.


1998 ◽  
Vol 34 (7) ◽  
pp. 698-706
Author(s):  
Masahiro ISHIBASHI ◽  
Masaki TAKAMOTO ◽  
Yu-ichi NAKAO ◽  
Toshio YOKOMIZO
Keyword(s):  

Volume 1 ◽  
2004 ◽  
Author(s):  
Masahiro Ishibashi

It is shown that the recovery temperature measured by a thin thermocouple wire inserted in airflow does not depend on the angle of incidence of the flow onto the wire and agrees very well with the theoretical value assuming the recovery factor of the square root of the Prandtl number. This fact allows RTA (Recovery Temperature Anemometry) employing a sensor of various structures; pRTA (probe RTA) is one of the examples where the thermocouple wire is bent at its contact point forming the probe apex. The paper demonstrates that pRTA measures the same flow velocity distributions in a critical nozzle as those by sRTA (streamwise RTA) where a thermocouple wire is settled parallel to the axis of symmetry of the nozzle.


2010 ◽  
Vol 19 (3) ◽  
pp. 222-227 ◽  
Author(s):  
Jae Hyung Kim ◽  
Heuy Dong Kim ◽  
Toshiaki Setoguchi

1962 ◽  
Vol 84 (4) ◽  
pp. 447-457 ◽  
Author(s):  
B. T. Arnberg

Critical flowmeters for accurately measuring the mass flow rates of nonreacting real gases were reviewed. Discussions were presented on theoretical flow functions, on parameters for correlating discharge coefficients, and on the importance of real gas properties. The performance characteristics of critical nozzles and orifices of several designs were reviewed. Approaches were discussed to problems which must be researched before the fullest potential of this type of flow measurement can be realized.


1989 ◽  
Vol 32 (11) ◽  
pp. 1092-1094
Author(s):  
M. Kh. Khamatov ◽  
O. K. Semenova ◽  
T. A. Smolina

2013 ◽  
Vol 38 (21) ◽  
pp. 9043-9051 ◽  
Author(s):  
Junji Nagao ◽  
Shigeru Matsuo ◽  
Shotaro Suetsugu ◽  
Toshiaki Setoguchi ◽  
Heuy Dong Kim

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