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This is the defence presentation for the dissertation Dynamics of Helical Flow Structures

This is the defence presentation for the dissertation Dynamics of Helical Flow Structures

This is the defence presentation for the dissertation Dynamics of Helical Flow Structures A Description of Vortex Formation in Turbulent Fluids by Nikolaj Nawri given on 2 April 2003 at the Department of Meteorology of the University of Maryland at College Park.

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639 views • 57 slides
Lecture 6 Ensemble Learning (1) Boosting

Lecture 6 Ensemble Learning (1) Boosting

Lecture 6 Ensemble Learning (1) Boosting. Adaboost Boosting is an additive model Brief intro to lasso The relationship. Boosting. Combine multiple classifiers. Construct a sequence of weak classifiers, and combine them into a strong classifier by a weighted majority vote.

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524 views • 28 slides
COMPARISON OF ASTROMETRIC CATALOGUES UCAC4, XPM, PPMXL

COMPARISON OF ASTROMETRIC CATALOGUES UCAC4, XPM, PPMXL

COMPARISON OF ASTROMETRIC CATALOGUES UCAC4, XPM, PPMXL. A.S.Tsvetkov and V.V.Vityazev SPb University, Russia. MOTIVATION. The pre-GAIA modern astrometric catalogues UCAC4, PPMXL and XPM

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376 views • 23 slides
The Mathematics of Quantum Mechanics 3. State vector, Orthogonality, and Scalar Product

The Mathematics of Quantum Mechanics 3. State vector, Orthogonality, and Scalar Product

The Mathematics of Quantum Mechanics 3. State vector, Orthogonality, and Scalar Product. Measurement in Quantum Mechanics. Measuring is equivalent to breaking the system state down to its basis states:. The basis states are eigenfunctions of a hermitian operator:.

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364 views • 9 slides
A Study of the O 2 A band including Polarisation Effects

A Study of the O 2 A band including Polarisation Effects

A Study of the O 2 A band including Polarisation Effects. Vijay Natraj. Equation of RT. Stokes Parameters. Stokes parameters are time averages: I = <a l 2 +a r 2 > Q = <a l 2 -a r 2 > U = 2<a l a r cos?> V = 2<a l a r sin?> Pol = (Q 2 +U 2 +V 2 ) 1/2 /I. Scattering Matrix.

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621 views • 7 slides

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