1965
DOI: 10.2514/3.3021
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Minimum fuel closed-loop translation

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Cited by 5 publications
(4 citation statements)
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“…S. SAROA* Indian Institute of Technology, Kharagpur, India T HE problem of three-dimensional boundary-layer flow near a spinning cone for an incompressible viscous fluid was studied by Wu. 1 He showed that with a suitable choice of coordinate axes and a suitable independent variable, the velocity functions can be obtained from the same set of equations as that for a disk rotating in an infinite fluid at rest (Karman's problem), but the pressure distribution is modified. Datta 2 showed that this is also true for Reiner-Rivlin where m is a stress tensor, p is an indeterminate hydrostatic pressure, and vt and a; are velocity and acceleration vectors, respectively.…”
Section: Flow Of a Second-order Fluid Near A Spinning Conementioning
confidence: 98%
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“…S. SAROA* Indian Institute of Technology, Kharagpur, India T HE problem of three-dimensional boundary-layer flow near a spinning cone for an incompressible viscous fluid was studied by Wu. 1 He showed that with a suitable choice of coordinate axes and a suitable independent variable, the velocity functions can be obtained from the same set of equations as that for a disk rotating in an infinite fluid at rest (Karman's problem), but the pressure distribution is modified. Datta 2 showed that this is also true for Reiner-Rivlin where m is a stress tensor, p is an indeterminate hydrostatic pressure, and vt and a; are velocity and acceleration vectors, respectively.…”
Section: Flow Of a Second-order Fluid Near A Spinning Conementioning
confidence: 98%
“…A large number of fluids of technical importance can be represented by this constitutive equation. We discuss the aforementioned problem of Wu for an incompressible second-order fluid given by the constitutive equation (1).…”
Section: Flow Of a Second-order Fluid Near A Spinning Conementioning
confidence: 99%
“…Control considerations are beyond the scope of this study; an excellent closed-loop solution is provided in Ref. 3.…”
mentioning
confidence: 99%
“…Optimum values of vehicle tilt angle and translation time have been found to exist; these values are a function of translation requirements. Nomenclature a = acceleration, ft/sec 2 Fh = horizontal thrust vector, Ib F r = resultant thrust vector, Ib F v -vertical thrust vector, Ib g c = Earth gravity constant, ft/sec 2 g = local acceleration of gravity, ft/sec 2 a P = propellant specific impulse, Ib-sec/lb /tot = total impulse, Ib-sec $ 3 = total distance translated, ft T = design thrust of engine, Ib ttot = total hover and translation time, sec ti = acceleration time, sec tz = time-to-start of deceleration, sec 1 3 = total translation time, sec VQ = initial velocity, fps WF = weight function, Ib-sec/lb Wip = propulsion system inert parts weight, Ib Wo = vehicle weight, Ib W p = propellant weight, Ib W r = propulsion system weight, Ib T^eng = engine weight, Ib B = thrust vector angle, deg Introduction P REVIOUS studies 1 -2 have shown the existence of optimum conditions for minimum propellant consumption during vehicle translation parallel to the lunar surface. This study represents a more graphical approach in which the influence of over-all propulsion system weight is considered along with the effect of operating off of the optimum design points.…”
mentioning
confidence: 99%