Computation of Supersonic Flow over Flying Configurations

Nastase, Adriana

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Table of contents
  • Contentsv
  • About the Authorxiii
  • Prefacexv
  • Acknowledgmentsxvii
  • Chapter 1 Zonal, Spectral Solutions for the Three-Dimensional, Compressible Navier–Stokes Layer1
  • 1.1 Introduction1
  • 1.2 Three-dimensional, partial-differential equations of compressible Navier–Stokes layer (NSL)2
  • 1.3 The spectral variable and the spectral forms of the velocity's components and of the physical en4
  • 1.4 The first and second derivatives of the velocity's components5
  • 1.5 The implicit and explicit forms of the boundary conditions at the NSL's edge8
  • 1.6 The dependence of the density function R versus the spectral velocity, inside the NSL10
  • 1.7 Dependence of absolute temperature T versus the spectral velocity, inside the NSL11
  • 1.8 The scalar forms of the NSL's impulse's partial-differential equations and their equivalent quad12
  • 1.9 Determination of spectral coefficients of the velocity's components by solving an equivalent qua15
  • 1.10 An original iterative method to solve a quadratical algebraic system16
  • 1.11 Conclusions18
  • References19
  • Chapter 2 Hyperbolical Potential Boundary Value Problems of the Axial Disturbance Velocities of Oute20
  • 2.1 Introduction20
  • 2.2 Basic equations21
  • 2.3 Full-linearized partial-differential equations of the flow over flattened, flying configurations26
  • 2.4 The characteristic hypersurfaces of the partial-differential equations of second order28
  • 2.4.1 The classification of quasi-linear partial-differential equations of second order28
  • 2.4.2 The characteristic's condition and the characteristic hypersurface30
  • 2.5 The linearized pressure coefficient C[sub(p)] on flying configurations33
  • 2.6 The linearized boundary value problems for flying configurations, at moderate angles of attack &34
  • 2.7 Definitions and properties of the thin and thick-symmetrical components of the thick, lifting fl35
  • 2.8 The disturbance regions produced by a moving point in subsonic and supersonic flow38
  • 2.9 Disturbance regions and characteristic surfaces produced by triangular wings, in supersonic flow40
  • 2.10 Disturbance regions and characteristic surfaces produced by trapezoidal wings, in supersonic fl49
  • 2.11 Disturbance regions and characteristic surfaces produced by rectangular wings, in supersonic fl52
  • 2.12 The boundary value problems for the axial disturbance velocities on thin and thick-symmetrical53
  • 2.13 Conclusions56
  • References57
  • Chapter 3 Computation of Axial Disturbance Velocities on Wedged Wings, in Supersonic Flow, at NSL's58
  • 3.1 General considerations58
  • 3.2 The conical flow of first order60
  • 3.2.1 Definition of the conical flow60
  • 3.2.2 The Germain's complex plane61
  • 3.2.3 The Germain's compatibility conditions for the conical flow63
  • 3.2.4 The Carafoli's hydrodynamic analogy for the conical flow63
  • 3.2.5 The principle of the minimal singularities for the wedged triangular wings65
  • 3.3 The boundary conditions for the wedged triangular wings, in the Germain's plane68
  • 3.3.1 Introduction68
  • 3.3.2 The boundary conditions of the fictitious, complex potentials U and U* on the real axis of the68
  • 3.3.3 The wedged triangular wings with one subsonic and one supersonic leading edge72
  • 3.3.4 The wedged triangular wings with two supersonic leading edges73
  • 3.4 The solutions of direct boundary value problems for U and U* on wedged triangular wing component78
  • 3.4.1 The auxiliary plane χ=λ+iμ78
  • 3.4.2 The affine transformed wing and the transformed complex plane x78
  • 3.4.3 The contribution of a subsonic leading edge on the thin wedged triangular wing80
  • 3.4.4 The contributions of ridges of the thin and thick-symmetrical wedged triangular wings82
  • 3.4.5 The contribution of the supersonic leading edge on the thin wedged triangular wing84
  • 3.4.6 The contributions of the leading edges on the thick-symmetrical wedged triangular wings85
  • 3.5 The complex axial disturbance velocities U and U* on the wedged triangular wing components85
  • 3.5.1 Introduction85
  • 3.5.2 The complex axial disturbance velocity U on the thin wedged triangular wing86
  • 3.5.3 The complex axial disturbance velocity U* on the thick-symmetrical wedged triangular wing88
  • 3.6 The axial disturbance velocities u and u* on the wedged delta wing components91
  • 3.7 The axial disturbance velocities u and u* on the wedged trapezoidal wing components95
  • 3.8 The axial disturbance velocities u and u* on the wedged rectangular wing components101
  • 3.9 Conclusions102
  • References103
  • Chapter 4 Computation of Axial Disturbance Velocities on Flying Configurations with Arbitrary Shapes106
  • 4.1 General considerations106
  • 4.2 The theory of high conical flow of nth order107
  • 4.2.1 Definition of the high conical flow of the nth order and the homogeneity conditions107
  • 4.2.2 The Germain's compatibility conditions for the high conical flow of nth order111
  • 4.2.3 The Carafoli's hydrodynamic analogy for the high conical flow of nth order112
  • 4.2.4 The boundary conditions of the fictitious, complex potentials F[sub(f)] and Fast*[sub(f)], on114
  • 4.3 The principle of minimal singularities for the high conical flow of nth order119
  • 4.4 The solutions of boundary value problems of fictitious complex potentials F[sub(f)] and F*[sub(f121
  • 4.5 The axial disturbance velocities on the thin and thick-symmetrical triangular wings with arbitra129
  • 4.6 The axial disturbance velocities on delta wings with arbitrary shapes135
  • 4.7 The axial disturbance velocities on trapezoidal wings with arbitrary shapes137
  • 4.8 The axial disturbance velocities on rectangular wings with arbitrary shapes140
  • 4.9 The axial disturbance velocities on non-integrated or integrated delta wing-fuselage configurati142
  • 4.10 The axial disturbance velocities on non-integrated or integrated delta wing-fuselage configurat147
  • 4.11 Determination of the constants of axial disturbance velocities on flying configurations151
  • 4.12 Conclusions152
  • References153
  • Chapter 5 The Aerodynamical Characteristics of Flying Configurations with Arbitrary Shapes, in Super156
  • 5.1 General considerations156
  • 5.2 The computation of the aerodynamical characteristics of the delta wings158
  • 5.3 The computation of the aerodynamical characteristics of delta wing-fuselage configurations165
  • 5.4 The computation of the aerodynamical characteristics of delta wing-fuselage configurations, fitt172
  • 5.5 The computation of the lift, pitching moment and drag coefficients of the rectangular wings180
  • 5.6 Conclusions185
  • References185
  • Chapter 6 The Visualizations of the Surfaces of Pressure Coefficients and Aerodynamical Characterist188
  • 6.1 Introduction188
  • 6.2 The three-dimensional visualizations of the C[sub(p)]-surfaces on the LAF's wedged delta wing, i189
  • 6.3 Visualizations of the behaviors of the C[sub(p)]-surfaces on a wedged delta wing, by crossing of199
  • 6.4 Visualizations of the surfaces of lift and pitching moment coefficients of LAF's wedged delta wi201
  • 6.5 The visualization of the inviscid drag coefficient's surface of the LAF's wedged delta wing and202
  • 6.6 The polar surface of the LAF's wedged delta wing and its asymptotical behavior, by crossing of s204
  • 6.7 The visualizations of the C[sub(p)]-surfaces on the LAF's wedged rectangular wing207
  • 6.8 The behaviors of the C[sub(p)]-surfaces by changing of the LAF's wedged rectangular wing from lo213
  • 6.9 The three-dimensional visualizations of surfaces of aerodynamical characteristics of LAF's wedge215
  • 6.10 The polar surface of the LAF's wedged rectangular wing, in supersonic flow219
  • 6.11 Conclusions220
  • References222
  • Chapter 7 Qualitative Analysis of the NSL's Asymptotical Behaviors in the Vicinity of its Critical Z224
  • 7.1 Introduction224
  • 7.2 Reduction of quadratical, elliptical and hyperbolical algebraic equations to their canonical for226
  • 7.3 The asymptotical behaviors of quadratical algebraic equations with variable free term228
  • 7.3.1 General considerations228
  • 7.3.2 The qualitative analysis of the behaviors of quadratical, elliptical, algebraic equations in t229
  • 7.3.3 The qualitative analysis of the behaviors of quadratical, hyperbolical, algebraic equations in237
  • 7.4 The qualitative analysis of elliptical and hyperbolical, quadratical, algebraic equations with v247
  • 7.4.1 General considerations247
  • 7.4.2 The collapse of the elliptical QAEs along their critical parabola248
  • 7.4.3 The degeneration of the hyperbolical QAEs along their critical parabola250
  • 7.5 The Jacobi determinant and the Jacobi hypersurface251
  • 7.6 The aerodynamical applications of the qualitative analysis of the QAEs252
  • 7.7 Conclusions253
  • References254
  • Chapter 8 Computation of the Friction Drag Coefficients of the Flying Configurations256
  • 8.1 Introduction256
  • 8.2 Computation of the inviscid lateral velocity υ, at the NSL's edge258
  • 8.3 The coupling between the NSL's slopes and the velocity field263
  • 8.4 Computation of friction and total drag coefficients of the delta wings264
  • 8.5 Conclusions266
  • References267
  • Chapter 9 Inviscid and Viscous Aerodynamical Global Optimal Design269
  • 9.1 Introduction269
  • 9.2 The optimum–optimorum theory271
  • 9.3 Inviscid aerodynamical global optimal design, via optimum–optimorum theory273
  • 9.4 Inviscid aerodynamic global optimal design of delta wing model ADELA, via optimum–optimorum th277
  • 9.5 Inviscid aerodynamic global optimal design of fully-integrated wing/fuselage models FADET I and279
  • 9.6 The iterative optimum–optimorum theory and the viscous aerodynamical optimal design283
  • 9.7 Proposal for a fully-optimized and fully-integrated Catamaran STA285
  • 9.8 Conclusions287
  • References288
  • Chapter 10 Comparison of the Theoretical Aerodynamical Characteristics of Wing Models with Experimen292
  • 10.1 Introduction292
  • 10.2 The aims of the experimental program293
  • 10.3 Determination of experimental-correlated values of aerodynamical characteristics and of interpo297
  • 10.4 Comparison of theoretical aerodynamical characteristics of LAF's wedged delta wing model with e299
  • 10.4.1 The description of LAF's wedged delta wing model299
  • 10.4.2 The computation of axial disturbance velocities on the upper side of wedged delta wings299
  • 10.4.3 The comparison of the theoretical and experimental-correlated values of C[sub(l)] and C[sub(m304
  • 10.5 Comparison of theoretical aerodynamical characteristics of LAF's double wedged delta wing model311
  • 10.5.1 The description of LAF's double wedged delta wing model311
  • 10.5.2 Computation of downwashes and of axial disturbance velocities on double wedged delta wing314
  • 10.5.3 Comparison of theoretical and experimental-correlated C[sub(l)] and C[sub(m)] of LAF's double316
  • 10.6 Comparison of theoretical aerodynamical characteristics of LAF's wedged delta wing model, fitte319
  • 10.6.1 Description of LAF's delta wing-fuselage model319
  • 10.6.2 The computation of downwashes and of axial disturbance velocities on the wedged delta wing mo320
  • 10.6.3 Comparison of the theoretical and experimental-correlated values C[sub(l)] and C[sub(m)] of L324
  • 10.7 Comparison of theoretical aerodynamical characteristics of LAF's fully-optimized delta wing mod327
  • 10.7.1 Description of LAF's fully-optimized delta wing model ADELA327
  • 10.7.2 The computation of downwashes and of axial disturbance velocities on the fully-optimized delt330
  • 10.7.3 Comparison of theoretical and experimental-correlated values of C[sub(l)] and C[sub(m)] of LA332
  • 10.8 Comparison of theoretical aerodynamical characteristics of LAF's wedged rectangular wing model336
  • 10.8.1 Description of LAF's wedged rectangular wing model336
  • 10.8.2 The computation of axial disturbance velocities on wedged rectangular wing model339
  • 10.8.3 The comparison of theoretical and experimental-correlated values of C[sub(l)] and C[sub(m)] o340
  • 10.9 Comparison of theoretical aerodynamic characteristics of LAF's cambered rectangular wing model343
  • 10.9.1 Description of LAF's cambered rectangular wing model343
  • 10.9.2 Computation of the axial disturbance velocities on LAF's cambered rectangular wing model344
  • 10.9.3 The comparison of theoretical and experimental-correlated values of C[sub(l)] and C[sub(m)] o347
  • 10.10 Conclusions349
  • References352
  • Final Remarks354
  • Outlook356
  • Author Index357
  • Subject Index361
  • Plate Section391
Book details
  • Vendor Elsevier S & T
  • SKU 9780080449579
  • ISBN-13 9780080556994
  • Author Nastase, Adriana
  • Category Technology & Engineering
  • Subject Aeronautics & Astronautics

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This high-level aerospace reference book will be useful for undergraduate and graduate students of engineering, applied mathematics and physics. The author provides solutions for three-dimensional compressible Navier-Stokes layer subsonic and supersonic flows.

* Computational work and experimental results show the real-world application of computational results
* Easy computation and visualization of inviscid and viscous aerodynamic characteristics of flying configurations
* Includes a fully optimized and integrated design for a proposed supersonic transport aircraft