Development of an infrared seed-sensing system to estimate flow rates based on physical properties of seeds

2019 ◽  
Vol 162 ◽  
pp. 874-881 ◽  
Author(s):  
Bahram Besharati ◽  
Hossein Navid ◽  
Hadi Karimi ◽  
Hossein Behfar ◽  
Iraj Eskandari
1969 ◽  
Vol 42 (5) ◽  
pp. 1336-1349
Author(s):  
W. G. DePierri

Abstract The results which we discussed in this paper show that the demands made on the compound in an injection molding operation are more severe than those made by compression molding. The flow properties of the compound are much more critical in injection molding because of the high flow rates which are encountered. Compounds must have viscosities which are low enough to allow the mold to fill completely in the injection step. The level of oil and black in the compound are very important factors in controlling compound viscosity. The cure system is more critical, for it must give good physical properties at the elevated temperatures used in injection molding. The ability to attain good physical properties at low cure temperatures does not necessarily mean that good properties will be achieved at elevated cure temperatures as was shown by the comparison of physical properties of specimens prepared by high temperature injection and low temperature compression molding. The physical properties of injection molded specimens made from some compounds cured at high temperatures indicated a lower state of cure at optimum cure than compression molded specimens cured at lower temperature. Much of this effect can be explained by changes in state of cure caused by the increased temperature. The oil type used in the compound did not appear to be especially important in determining the physical properties of molded items. Oil level, however, is an important factor in determining both the processability of a compound and the physical properties of the finished product. Some of the problems associated with injection molding of EPDM compounds encountered in this work may result from the experimental injection molding equipment used in the study and may not be evident when commercial equipment is employed. Other of the problems could be solved by compounding, especially by changes in the cure system.


2012 ◽  
Vol 76 ◽  
pp. 23-28 ◽  
Author(s):  
Roberta Claro da Silva ◽  
Fabiana Andreia Schaffer De Martini Soares ◽  
Marcia Hazzan ◽  
Isabele Renata Capacla ◽  
Maria Inês Almeida Gonçalves ◽  
...  

2019 ◽  
Vol 48 (7) ◽  
pp. 1529-1537 ◽  
Author(s):  
Siti SalwaHarun Alias ◽  
Zawati Harun ◽  
Ahmad Nazreen Ahmad Ismail ◽  
Noor Hasliza Kamarudin

2012 ◽  
Vol 259 ◽  
pp. 172-177 ◽  
Author(s):  
R.S. Vemuri ◽  
G. Carbjal-Franco ◽  
D.A. Ferrer ◽  
M.H. Engelhard ◽  
C.V. Ramana

1991 ◽  
Vol 71 (3) ◽  
pp. 983-992 ◽  
Author(s):  
K. J. Sullivan ◽  
H. K. Chang

The influence of flow characteristics and gas physical properties on nasal resistance (NR) is difficult to ascertain with traditional rhinomanometric methods because the respiratory airflows used in these methods are largely uncontrolled. As an alternative, we used a novel method of rhinomanometry in which an externally generated flow is passed through the nasal passage via a mouthpiece. The transnasal pressure-flow relationships for both quasi-steady and oscillating flows and with different gases were obtained in five healthy adults with this method. For quasi-steady nasal flows the dimensionless pressure losses were largely independent of physical properties of the gas and a function of the Reynolds number (Re) of the flow. Values of NR for quasi-steady flows were largely independent of flow direction for Re up to roughly 3,000 in all five subjects and for Re up to roughly 19,000 in two of the five subjects. Airway collapse occurred in two subjects at Re greater than 3,000, suggesting that the nonrigid segments of the nasal passage contribute to the intersubject variations in NR at high flow rates. Pressure losses associated with oscillating flows measured at frequencies between 1 and 16 Hz were similar to steady flow losses provided that Re was less than roughly 3,000. For Re greater than 3,000 the oscillating flow resistances were affected by the phasic redistribution of flow into compliant segments of the nasal passage. These results indicate that, for flow rates and harmonic frequencies associated with breathing at rest, the nasal passage behaves as a rigid rough-walled pipe in which pressure losses are largely determined by forces relating to viscous friction and convective accelerations.


2003 ◽  
Author(s):  
Graciela Velasco Herrera ◽  
Victor M. Velasco Herrera ◽  
Antonio H. Barosio ◽  
Valerii K. Volosyuk

1979 ◽  
Vol 193 (1) ◽  
pp. 237-244 ◽  
Author(s):  
W. A. Woods ◽  
G. K. Goh

This work is put in perspective by mentioning some of the applications of butterfly throttle valves and explaining how the next tests are complementary to other work (1). The present tests examine the flow characteristics of a butterfly throttle valve in relation to valve opening, pressure ratio and circumferential and axial location of the pressure tappings. The paper gives results of a comprehensive series of steady flow tests and, also, results of a limited number of unsteady flow tests. In the latter, the butterfly throttle valve was located in the intake system of a single cylinder diesel engine. The paper highlights the importance of the position of pressure tappings when pressure measurements are used to estimate flow rates. The results of the present study show that when suitable precautions are taken the quasi-steady flow method may be used to predict the flow rates under pulsating conditions.


2017 ◽  
Vol 17 (4B) ◽  
pp. 51-57
Author(s):  
A. D. Tuan ◽  
N. X. Anh ◽  
T. P. Hung

Lidar is an active remote-sensing system that uses laser radiation in the ultraviolet, visible and near-infrared wavelength domain. It allows the measurement of the physical properties of the atmosphere with spatial and temporal resolution. We have simulated the system and researched the initial design of the Lidar system to monitor the aerosol with the main parameters: high power Nd - YAG pulse laser emitted at the 532 nm wavelength. The system includes 28 cm diameter optical glass, photomultiplier tube (PMT) - H6780-03 photodetector, and optical components for convergence and filtering of reflected reflections. Initial measurements show that the Lidar system is highly sensitive, which determines important atmospheric properties such as the distribution and physical properties of the aerosol and height of ABL (atmospheric boundary layer).


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