Mixing Duct Pressure Distributions and Exhaust Flow Characteristics of a High Temperature and Pressure Cylindrical Ejector

Mixing Duct Pressure Distributions and Exhaust Flow Characteristics of a High Temperature and Pressure Cylindrical Ejector
Author: Brian Quinn
Publisher:
Total Pages: 95
Release: 1975
Genre: Air ducts
ISBN:

The thermodynamic and mixing characteristics of a family of inlet area ratio 26 ejectors have been measured across a range of primary reservoir pressures (0 to 80 psig) and temperatures (65 to 1000 degrees F). The length-to-duct diameter ratio of the ejectors was the family parameter and varied from 12.36 to 3.46. The distribution of pressure along the wall of the mixing duct clearly identified up to three distinct modes of turbulent mixing. They also substantiated prior observations that mixing is accelerated by heating the primary jet. The discrete modes of mixing were subjectively related to the acoustic properties of the greatly underexpanded primary nozzle.

Heat, Mass and Momentum Transfer in a Condensing Ejector Mixing Section. Part I. Mixing Section Analysis. Part II. Experimental Data

Heat, Mass and Momentum Transfer in a Condensing Ejector Mixing Section. Part I. Mixing Section Analysis. Part II. Experimental Data
Author: S. William Gouse (Jr)
Publisher:
Total Pages: 20
Release: 1967
Genre:
ISBN:

Many applications of the condensing ejector involve the pumping of a gas mixture containing a condensable vapor and one or more non-condensable gases. A theoretical model for the mixing process is given. presence of a high-velocity liquid jet surrounded by the higher Correlations for heat- and mass-transfer coefficients are used where necessary. Boundary conditions are satisfied for velocity, temperature, and shear stress at the liquid jet-gas stream interface. Wall shear stresses and compressible flow aspects for the gas stream are included. Available experimental data have been used to evaluate the mixing section analysis for condensing ejector operation with carbon dioxide as the non-condensable gas and steam as the condensable vapor. Direct comparisons with measured axial static pressure distributions and observed choking conditions are included. (Author).

Studies on Mixing Processes in Ejectors

Studies on Mixing Processes in Ejectors
Author: A. Krothpalli
Publisher:
Total Pages: 97
Release: 1984
Genre:
ISBN:

The capability of producing additional thrust along with the ability of vectoring the thrust makes the ejector an attractive device for V/STOL aircraft applications. In addition, the acoustic shielding provided by the walls of the shroud, and lowered exhaust velocities and temperatures at the ejector exit offer important advantages in the area of nozzle exhaust cooling. One of the physical processes which is known to play a large role on the performance of the total system is the mixing between the hot primary and cold secondary streams. Thus an attempt is made here to investigate the mixing process of a hot rectangular jet with an entrained cold ambient fluid in a simple form of a ejector. Primary jet heating, over the temperature range tested, has no significant effect on the velocity field within the ejector shroud. The temperature decay within the ejector shroud displayed differences in comparison with the free jet up to a location where the primary jet spreads to the mixing duct wall. Downstream of this location the centerline temperature within the ejector is higher than that of a free jet. A theoretical analysis is made to set up a determinate mathematical problem for the flow through a constant area ejector. It is shown that multiple solution (more than two) occur, and admissible ones out of these are those that fulfill the entropy condition.

A Study of a Supersonic Ejector Mixing Chamber

A Study of a Supersonic Ejector Mixing Chamber
Author: George Einar Strand
Publisher:
Total Pages: 82
Release: 1965
Genre:
ISBN:

An experimental investigation was performed to study the characteristics of the flow in a two-dimensional air ejector in which the center stream entered the mixing chamber at a Mach number of 1.90 while the velocity of the secondary flow was varied from zero to Mach 0.7. Mass flow ratios of the ejector were approximately equal when the pressures of the two streams were equal at the entrance to the mixing chamber. The chamber had a rectangular cross section and converged slightly; its length was equal to 16 times the width. Pressures measured at the walls and the centerline of the flow indicated that a maximum static pressure was reached at 8 widths of the chamber downstream of the nozzle when the flow was completely expanded at the nozzle exit. The maximum static pressure was achieved in less distance for the overexpanded condition and took longer for the underexpanded condition. The flow was always subsonic by the time the maximum pressure position was reached except in the underexpanded case, where the flow remained supersonic throughout the chamber and the maximum pressure was located at the exit to the chamber. (Author).

An Analysis of the Properties of Two-dimensional Incompressible Fluid Flow in the Mixing Chamber of a Constant Area Ejector

An Analysis of the Properties of Two-dimensional Incompressible Fluid Flow in the Mixing Chamber of a Constant Area Ejector
Author: Martin D. Kiefer
Publisher:
Total Pages: 85
Release: 1963
Genre: Mechanical engineering
ISBN:

The properties of an incompressible fluid in the mixing chamber of a constant area cylindrical ejector are analyzed in a two-dimensional form. The flow field for velocity and temperature is assumed to be made up of regions in which uniform flow of the primary and secondary fluids exist, and which diminish with axial distance from the ejector entrance. The velocity and temperature distributions in the mixed region are assumed to have cosine shaped profiles. The compatible solutions are given an axial distribution by assuming a parabolic spread rate for the secondary fluid jet boundary. Results are generated in the form of a non-dimensional velocity and pressure, a normalized temperature and a Momentum Factor, as functions of axial distance.