Private Tuition Institutions A Simple Form of Capitalism: Micro Investigation in District Anantnag

The normal method of background subtraction in quantitative EELS analysis involves fitting an expression of the form I=AE-r to an energy window preceding the edge of interest; E is energy loss, A and r are fitting parameters. The calculated fit is then extrapolated under the edge, allowing the required signal to be extracted. In the case where the characteristic energy loss is small (E < 100eV), the background does not approximate to this simple form. One cause of this is multiple scattering. Even if the effects of multiple scattering are removed by deconvolution, it is not clear that the background from the recovered single scattering distribution follows this simple form, and, in any case, deconvolution can introduce artefacts.The above difficulties are particularly severe in the case of Al-Li alloys, where the Li K edge at ~52eV overlaps the Al L2,3 edge at ~72eV, and sharp plasmon peaks occur at intervals of ~15eV in the low loss region. An alternative background fitting technique, based on the work of Zanchi et al, has been tested on spectra taken from pure Al films, with a view to extending the analysis to Al-Li alloys.

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System of thermodynamic quantities in the McMillan-Mayer solution theory

Collection of Czechoslovak Chemical Communications ◽

10.1135/cccc19850791 ◽

1985 ◽

Vol 50 (4) ◽

pp. 791-798 ◽

Cited By ~ 1

Author(s):

Vilém Kodýtek

Keyword(s):

Free Energy ◽

Generating Function ◽

Simple Form ◽

Unit Volume ◽

Thermodynamic Quantities ◽

Solution Theory ◽

Pure Solvent ◽

Second Derivatives ◽

Definition Of ◽

Derivatives Of

The McMillan-Mayer (MM) free energy per unit volume of solution AMM, is employed as a generating function of the MM system of thermodynamic quantities for solutions in the state of osmotic equilibrium with pure solvent. This system can be defined by replacing the quantities G, T, P, and m in the definition of the Lewis-Randall (LR) system by AMM, T, P0, and c (P0 being the pure solvent pressure). Following this way the LR to MM conversion relations for the first derivatives of the free energy are obtained in a simple form. New relations are derived for its second derivatives.

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MASTER STABILITY FUNCTIONS FOR SYNCHRONIZED COUPLED SYSTEMS

International Journal of Bifurcation and Chaos ◽

10.1142/s0218127499001814 ◽

1999 ◽

Vol 09 (12) ◽

pp. 2315-2320 ◽

Cited By ~ 18

Author(s):

LOUIS M. PECORA ◽

THOMAS L. CARROLL

Keyword(s):

Simple Form ◽

Coupled Systems ◽

Stability Function ◽

Coupled Oscillator ◽

Synchronous State ◽

Master Stability Function ◽

Stability Functions ◽

The Stability

We show that many coupled oscillator array configurations considered in the literature can be put into a simple form so that determining the stability of the synchronous state can be done by a master stability function which solves, once and for all, the problem of synchronous stability for many couplings of that oscillator.

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The Flow of an Incompressible Fluid through an Axial Turbo-Machine with any Number of Rows

Aeronautical Quarterly ◽

10.1017/s0001925900000585 ◽

1951 ◽

Vol 3 (2) ◽

pp. 133-144 ◽

Cited By ~ 3

Author(s):

J. W. Railly

Keyword(s):

Aspect Ratio ◽

Incompressible Fluid ◽

Radial Velocity ◽

Simple Form ◽

High Aspect Ratio ◽

Unknown Function ◽

Axial Velocity ◽

Velocity Fields ◽

Single Row ◽

Undetermined Constant

SummaryA method is described whereby, at any point in an infinite parallel annulus, the approximate axial velocity due to a single row of high aspect ratio blades may be calculated from a knowledge of the conditions of flow adjacent to the blades. The method is based on the assumption of a simplified expression for the radial velocity, being the product of an unknown function of the radius and an exponential term independent of the radius containing an undetermined constant; the function and the undetermined constant are calculated by reference to the conditions of flow in the plane of the row considered. The flow due to any number of rows is then obtained by summing the radial velocity fields due to each row and obtaining the axial velocities by integration of the equation of continuity.The solution of the problem with infinitely many rows is shown to have a simple form by virtue of the fact that the flow (provided that the velocities remain finite) settles down to a pattern which is periodic by one stage pitch.

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XXIV.—A simple form of gas regulator

Journal of the Chemical Society (Resumed) ◽

10.1039/js8762900488 ◽

1876 ◽

Vol 29 (0) ◽

pp. 488-489

Author(s):

Thomas Fletcher

Keyword(s):

Simple Form

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A PLEA FOR THE ADOPTION OF A MORE ACCURATE AND SCIENTIFIC METHOD IN THE INVESTIGATION AND TREATMENT OF LATERAL CURVATURE OF THE SPINE, WITH DESCRIPTION OF A SIMPLE FORM OF GAUGE

BMJ ◽

10.1136/bmj.1.2161.1332 ◽

1902 ◽

Vol 1 (2161) ◽

pp. 1332-1333

Author(s):

A. Young

Keyword(s):

Simple Form ◽

Scientific Method ◽

Lateral Curvature

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IV.—On a New Large Terebratula occurring in East Anglia

Geological Magazine ◽

10.1017/s0016756800209515 ◽

1870 ◽

Vol 7 (75) ◽

pp. 410-413 ◽

Cited By ~ 2

Author(s):

E. Ray Lankester

Keyword(s):

Simple Form ◽

The Other ◽

East Anglia ◽

Mesial Line ◽

New Name ◽

Gravel Pit ◽

Great Size

The forms which Mr. Davidson in his invaluable Monograph has included under T. ovoides, are so various that it would be possible to refer the shells figured in the plate to that species, but since T. trilineata, from the Inferior Oolite, and T. lata and T. ovoides, from drift-blocks—which I shall endeavour to show are of the very latest Jurassic horizon—are very different in many respects, I prefer to give a new name to this form, which may find its place near T. ovoides and T. simplex. The specimen drawn, Fig. 1 and la, is from the collection of Mr. Roper of Lowestoft, who obtained it, with another specimen, from a gravel-pit at Thorpe in Suffolk. It has the general simple form of T. ovoides, but is remarkable for its great size. The imperforate valve is flattened in the mesial line, whilst the perforate valve is deep and raised into a well-pronounced keel in the mesial line extending from the beak; the foramen is small. The specimen figured is longer than the other in Mr. Roper's collection, which has the shorter, squarer form of Fig. 2, resembling T. simplex. This fine Terebratula may be known as T. rex.

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