A New Approach to the Theory of Thin, Slightly Cambered Profiles

1957 ◽  
Vol 24 (2) ◽  
pp. 177-182
Author(s):  
F. S. Weinig

Abstract If real and imaginary parts of a function of a complex variable are interpreted as velocity potential and stream function, then real and imaginary parts of the kth derivatives are the (k–1) st derivatives of the velocity components in the direction of the real and negative imaginary axis. For slightly cambered profiles that deviate little from the real axis and have the shape of a polynomial of nth order, the imaginary part of the nth derivative of the complex potential is constant in first-order approximation. It is easy to establish such functions of the complex variable in the case of single as well as cascade profiles. Integration then yields the intended results. While there is no continuing need for such a method for single profiles, it is needed for cascades of profiles.

Geophysics ◽  
2007 ◽  
Vol 72 (5) ◽  
pp. D93-D106 ◽  
Author(s):  
Yaping Zhu ◽  
Ilya Tsvankin ◽  
Ivan Vasconcelos

One of the well-known factors responsible for the anisotropy of seismic attenuation is interbedding of thin attenuative layers with different properties. Here, we apply Backus averaging to obtain the complex stiffness matrix of an effective medium formed by an arbitrary number of anisotropic, attenuative constituents. Unless the intrinsic attenuation is uncommonly strong, the effective velocity function is controlled by the real-valued stiffnesses (i.e., independent of attenuation) and can be determined from the known equations for purely elastic media. Attenuation analysis is more complicated because the attenuation parameters are influenced by the coupling between the real and imaginary parts of the stiffness matrix. The main focus of this work is on effective transversely isotropic models with a vertical symmetry axis (VTI) that include isotropic and VTI constituents. Assuming that the stiffness contrasts, as well as the intrinsic velocity and attenuation anisotropy, are weak, we develop explicit first-order (linear) and second-order (quadratic) approximations for the attenuation-anisotropy parameters [Formula: see text], [Formula: see text], and [Formula: see text]. Whereas the first-order approximation for each parameter isgiven sim-ply by the volume-weighted average of its interval values, the second-order terms include coupling between various factors related to both heterogeneity and intrinsic anisotropy. Interestingly, the effective attenuation for P- and SV-waves is anisotropic even for a medium composed of isotropic layers with identical attenuation, provided there is a velocity variation among the constituent layers. Contrasts in the intrinsic attenuation, however, do not create attenuation anisotropy, unless they are accompanied by velocity contrasts. Extensive numerical testing shows that the second-order approximation for [Formula: see text], [Formula: see text], and [Formula: see text] is close to the exact solution for most plausible subsurface models. The accuracy of the first-order approximation depends on the magnitude of the quadratic terms, which is largely governed by the strength of the velocity (rather than attenuation) anisotropy and velocity contrasts. The effective attenuation parameters for multiconstituent VTI models vary within a wider range than do the velocity parameters, with almost equal probability of positive and negative values. If some of the constituents are azimuthally anisotropic with misaligned vertical symmetry planes, the effective velocity and attenuation functions may have different principal azimuthal directions or even different symmetries.


1976 ◽  
Vol 54 (10) ◽  
pp. 1550-1557 ◽  
Author(s):  
P. L. Prasad ◽  
Surjit Singh

Calculations of electro-optical parameters by the modified first order approximation (MFOA) method have been extended to X2CZ (X = H, F, Cl, Br; Z = O, S) molecules with a view to investigate the transferability of these parameters. The diagonal and cross elements of the bond moment derivative matrix have been evaluated. Unique values of µC−X are obtained for the A1 species. The bond moment derivatives are found to be transferable among A1 and B1 species. Transferability of the µC−Z in B1 and B2 species is obtained for thiocarbonyl halides. Bond moment derivatives with respect to angle deformations are not found to be very significant whereas other cross elements of the bond moment derivative matrix are found to be of high magnitude.


AIAA Journal ◽  
1998 ◽  
Vol 36 ◽  
pp. 1721-1727
Author(s):  
Prasanth B. Nair ◽  
Andrew J. Keane ◽  
Robin S. Langley

2021 ◽  
Vol 76 (3) ◽  
pp. 265-283
Author(s):  
G. Nath

Abstract The approximate analytical solution for the propagation of gas ionizing cylindrical blast (shock) wave in a rotational axisymmetric non-ideal gas with azimuthal or axial magnetic field is investigated. The axial and azimuthal components of fluid velocity are taken into consideration and these flow variables, magnetic field in the ambient medium are assumed to be varying according to the power laws with distance from the axis of symmetry. The shock is supposed to be strong one for the ratio C 0 V s 2 ${\left(\frac{{C}_{0}}{{V}_{s}}\right)}^{2}$ to be a negligible small quantity, where C 0 is the sound velocity in undisturbed fluid and V S is the shock velocity. In the undisturbed medium the density is assumed to be constant to obtain the similarity solution. The flow variables in power series of C 0 V s 2 ${\left(\frac{{C}_{0}}{{V}_{s}}\right)}^{2}$ are expanded to obtain the approximate analytical solutions. The first order and second order approximations to the solutions are discussed with the help of power series expansion. For the first order approximation the analytical solutions are derived. In the flow-field region behind the blast wave the distribution of the flow variables in the case of first order approximation is shown in graphs. It is observed that in the flow field region the quantity J 0 increases with an increase in the value of gas non-idealness parameter or Alfven-Mach number or rotational parameter. Hence, the non-idealness of the gas and the presence of rotation or magnetic field have decaying effect on shock wave.


1999 ◽  
Vol 08 (05) ◽  
pp. 461-483
Author(s):  
SEIYA NISHIYAMA

First-order approximation of the number-projected (NP) SO(2N) Tamm-Dancoff (TD) equation is developed to describe ground and excited states of superconducting fermion systems. We start from an NP Hartree-Bogoliubov (HB) wave function. The NP SO(2N) TD expansion is generated by quasi-particle pair excitations from the degenerate geminals in the number-projected HB wave function. The Schrödinger equation is cast into the NP SO(2N) TD equation by the variation principle. We approximate it up to first order. This approximate equation is reduced to a simpler form by the Schur function of group characters which has a close connection with the soliton theory on the group manifold.


Author(s):  
Bappaditya Banerjee ◽  
Anil K. Bajaj

Abstract Dynamical systems with two degrees-of-freedom, with quadratic nonlinearities and parametric excitations are studied in this analysis. The 1:2 superharmonic internal resonance case is analyzed. The method of harmonic balance is used to obtain a set of four first-order amplitude equations that govern the dynamics of the first-order approximation of the response. An analytical technique, based on Melnikov’s method is used to predict the parameter range for which chaotic dynamics exist in the undamped averaged system. Numerical studies show that chaotic responses are quite common in these quadratic systems and chaotic responses occur even in presence of damping.


2014 ◽  
Vol 20 (1) ◽  
pp. 132-141 ◽  
Author(s):  
Jianfeng Guo

The iteratively reweighted least-squares (IRLS) technique has been widely employed in geodetic and geophysical literature. The reliability measures are important diagnostic tools for inferring the strength of the model validation. An exact analytical method is adopted to obtain insights on how much iterative reweighting can affect the quality indicators. Theoretical analyses and numerical results show that, when the downweighting procedure is performed, (1) the precision, all kinds of dilution of precision (DOP) metrics and the minimal detectable bias (MDB) will become larger; (2) the variations of the bias-to-noise ratio (BNR) are involved, and (3) all these results coincide with those obtained by the first-order approximation method.


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