The drag of bodies has now assumed greater importance because, as shown in NACA RM L53I15a, 1953 and NACA RM A53H18a, 1953, the transonic drag rise of an airplane can be the same as its equivalent body. Obviously, the airplane designer would like his airplane to have a low-drag equivalent body. This paper shows some of the factors which minimize the drag of bodies at transonic and supersonic speeds and shows some of the penalties caused by deviating from low-drag body shapes. Drag reductions can be obtained in two ways, first, through increasing the body fineness ratio, and second, through better shaping of the body profile at a given fineness ratio. The effects of fineness ratio are discussed first and then, more completely, detail-shape e...
Approximate shapes of nonlifting bodies having minimum pressure foredrag at high supersonic airspeed...
In NACA RM L53I15a, 1953 and NACA RM A53H18a, 1953,it has been shown that, if the "area rule" is uti...
The drag and the power cost associated with the changing of the nose of a nacelle from a streamline ...
The drag of bodies has now assumed greater importance because, as shown in NACA RM L53I15a, 1953 and...
This paper is concerned primarily with the application of the "area rule" to the interpretation and ...
Approximate shapes of nonlifting bodies having minimum pressure foredrag at high supersonic airspeed...
An investigation was made in the Langley 300-mph 7- by 10-foot tunnel to determine the aerodynamic c...
It seems possible that, in supersonic flight, unconventional arrangements of wings and bodies may of...
An investigation has been made in the Langley transonic blowdown tunnel at Mach numbers between 0.84...
Effect of cross section shape on low speed aero- dynamic characteristics of low-wave drag hyper- son...
Drag measurements at transonic speeds on rectangular airfoils and on airfoils swept back 450 are rep...
An investigation has been conducted in the Langley 8-foot transonic tunnel to determine the effects ...
Ward's slender-body-theory formula for zero-lift drag contains three integrals plus a base-drag term...
Approximate shapes of nonlifting bodies having minimum pressure foredrag at high supersonic airspeed...
In NACA RM L53I15a, 1953 and NACA RM A53H18a, 1953,it has been shown that, if the "area rule" is uti...
The drag and the power cost associated with the changing of the nose of a nacelle from a streamline ...
The drag of bodies has now assumed greater importance because, as shown in NACA RM L53I15a, 1953 and...
This paper is concerned primarily with the application of the "area rule" to the interpretation and ...
Approximate shapes of nonlifting bodies having minimum pressure foredrag at high supersonic airspeed...
An investigation was made in the Langley 300-mph 7- by 10-foot tunnel to determine the aerodynamic c...
It seems possible that, in supersonic flight, unconventional arrangements of wings and bodies may of...
An investigation has been made in the Langley transonic blowdown tunnel at Mach numbers between 0.84...
Effect of cross section shape on low speed aero- dynamic characteristics of low-wave drag hyper- son...
Drag measurements at transonic speeds on rectangular airfoils and on airfoils swept back 450 are rep...
An investigation has been conducted in the Langley 8-foot transonic tunnel to determine the effects ...
Ward's slender-body-theory formula for zero-lift drag contains three integrals plus a base-drag term...
Approximate shapes of nonlifting bodies having minimum pressure foredrag at high supersonic airspeed...
In NACA RM L53I15a, 1953 and NACA RM A53H18a, 1953,it has been shown that, if the "area rule" is uti...
The drag and the power cost associated with the changing of the nose of a nacelle from a streamline ...