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The lecture notes in earth sciences

The lecture notes in earth sciences

The lecture notes in earth sciences

... decrease in heat flow data obtained 19 The thermal regime of the back-deep of the Rhenish Variscan mountains, that of the Saar Basin, is nearly the same as that of the Ruhr Basin during the Westphalian ... of the f l u i d in inclusions can be estimated by the depression of the freezing point during cooling The higher the s a l i n i t y , the higher is the depression of the freezing p o i n t ROEDDER ... the borehole HOD in the Pannonian basin The curves are calculated t h e o r e t i c a l l y , based on the thermal h i s t o r y of the basin from McKENZIE's (1978) stretching theory The basin...
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Lecture notes in earth sciences   springer

Lecture notes in earth sciences springer

... data in the earth sciences Athanasios Dermanis (ed.) - Berlin; Heidelberg; New York; Barcelona; Hong Kong; London; Milan; Paris; Singapore; Tokyo: Springer, 2000 (Lecture notes in earth sciences; ... @geod.ethz.ch "For all Lecture Notes in Earth Sciences published till now please see final pages of the book" Library of Congress Cataloging -in- Publication Data Die Deutsche Bibliothek - CIP-Einheitsaufnahme ... Lecture Notes in Earth Sciences Editors: S Bhattacharji, Brooklyn G M Friedman, Brooklyn and Troy H J Neugebauer, Bonn A Seilacher, Tuebingen and Yale Springer Berlin Heidelberg...
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The Lecture Notes in Physics Part 1 doc

The Lecture Notes in Physics Part 1 doc

... Dynamics of Vortices in Rotating and Stratified Fluids Lect Notes Phys 805, 1 34 (2 010 ) c Springer-Verlag Berlin Heidelberg 2 010 DOI 10 .10 07/978-3-642 -11 587-5 _1 G.J.F van Heijst 1. 1 .1 Basic Equations ... 10 .10 07/978-3-642 -11 587-5 Lecture Notes in Physics ISSN 0075-8450 e-ISSN 16 16-63 61 ISBN 978-3-642 -11 586-8 e-ISBN 978-3-642 -11 587-5 DOI 10 .10 07/978-3-642 -11 587-5 Springer Heidelberg Dordrecht London ... generated in a rotating fluid in a number of different ways One possible way is to place a thin-walled bottomless cylinder in the rotating fluid and then stir the fluid inside this cylinder, either cyclonically...
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The Lecture Notes in Physics Part 2 pps

The Lecture Notes in Physics Part 2 pps

... and f = the constant Coriolis parameter in the rotating tank experiment (LAB) In general, moving into shallower water in the rotating fluid experiment corresponds with moving northwards in the GFD ... stratification within the confining cylinder, with a relatively sharp interface between the upper and the lower layers During the subsequent evolution of the vortex after removing the cylinder, this ... circulation sketched in (b) The resulting circulation arising in case 2, in which the centrifugal force is initially not in balance with the radial density gradient, is shown in (c) (from [2] ) ωθ = ∂vr...
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The Lecture Notes in Physics Part 3 ppsx

The Lecture Notes in Physics Part 3 ppsx

... ensured by the choice of the axial velocity of the co-moving frame Neglecting the torsion, the obtained flow is therefore similar to the one studied previously Indeed, the normal to the osculating plane ... stratification Then, when the strain, , is larger than the vorticity, ζ , the streamlines are hyperbolic as shown in Fig 2.8 and the continuous stretching along the unstable manifold of the stagnation point ... constrain the motion to be horizontal The motion tends to be uniform in the vertical in the presence of rotation effects but not in the presence of stratification In some cases the shallowness of the...
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The Lecture Notes in Physics Part 4 potx

The Lecture Notes in Physics Part 4 potx

... resulting in the formation of so-called rings or synoptic eddies These rings, and in particular the warm-core rings which are surface intensified, have long since been identified in the vicinity of the ... Fluids 3, 2 644 (1991) 44 , 53, 54 34 Miyazaki, T.: Elliptical instability in a stably stratified rotating fluid Phys Fluids 5, 2702 (1993) 44 , 45 35 Moore, D.W., Saffman, P.G.: The instability of ... discriminant, δ = R + (ζ + ), appears in (2.36) as the opposite of the determinant of the governing matrix Sipp and Jacquin [48 ] showed that if there exists a particular streamline on which δ < 0, the...
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The Lecture Notes in Physics Part 5 ppsx

The Lecture Notes in Physics Part 5 ppsx

... version of these theorems was presented in Sect 3.2.2 In the quasi-geostrophic framework, these theorems state that even in the presence of diabatic heating and frictional or other forces, there can ... which is the gradient wind balance presented above (further details are available in [100]) The problem of separating these two types of motions in numerical weather predictions, and in particular ... stretching dominates relative vorticity in potential vorticity): ∂t h + J h∇ h + |∇h|2 = In the two-layer model, when the flow is surface-intensified, a thin surface layer is the usual assumption Then...
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The Lecture Notes in Physics Part 6 ppt

The Lecture Notes in Physics Part 6 ppt

... (the isopycnals not pinch off) Therefore, they entrain the surrounding fluid and the motion of this fluid must be taken into account The surrounding fluid advected northward (resp southward) by the ... distributions These mathematics describe the first stage of the beta-drift in which the in uence of the far-field of the Rossby wave wake is not important In the ocean, his effect becomes dominant after ... on a seamount on the beta-plane in a 2D flow Large seamounts in the southern hemisphere can deflect the vortex northward or back to the southeast while in the northern hemisphere, the monopole will...
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The Lecture Notes in Physics Part 7 pot

The Lecture Notes in Physics Part 7 pot

... ρ2 h ) f ρi (4.60) The fast motions in the linear approximation are internal inertia-gravity waves propagating along the interface between the layers By linearizing about the rest state h = H1 ... simplicity in the frequently used limit r → and introduce the Lagrangian coordinate 124 V Zeitlin X (x, t) corresponding to the positions of the fluid particles in the lower layer In terms of ... the Model To introduce the baroclinic effects in the dynamics in the simplest way we consider the two-layer rotating shallow water model We use the rigid lid upper boundary condition and again...
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The Lecture Notes in Physics Part 8 pps

The Lecture Notes in Physics Part 8 pps

... rewriting the contour integral in (5.9) in terms of C, which mathematically amounts to a variable substitution in the integrand The only non-trivial step is the transformation of the line element ... operation consists of zonal averaging, which is the typical setup in atmospheric wave–mean interaction theory In this periodic case a material line traversing the domain in the zonal x-direction qualifies ... on the location of the coordinate origin unless the net integral of ∇ × u, which is the total circulation around the fluid domain, is zero For example, in two dimensions the impulse of a single...
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The Lecture Notes in Physics Part 9 pptx

The Lecture Notes in Physics Part 9 pptx

... lasting change in the mean flow It is also clear that the net residual forcing points in the direction of p So there is no intrinsic link between wave dissipation and mean flow forcing but there ... Crucially, the Bretherton flow points backward, i.e in the negative x-direction, at the vortex location above the wavetrain Therefore the Bretherton flow does indeed push the vortex to the left and ... for inhomogeneous wavetrain incident on barred beach The topography is indicated on the right The vortex couple has moved to the bar trough, away from the main wave breaking region over the bar...
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The Lecture Notes in Physics Part 10 ppsx

The Lecture Notes in Physics Part 10 ppsx

... of the wavepacket, because it compresses the wavepacket in the x-direction whilst stretching it in the y-direction At the same time, the Bretherton flow induced by the finite wavepacket pushes the ... For instance, Coriolis forces were neglected throughout, but they can be incorporated both in GLM theory and in the other theoretical developments; this has been done in the quoted references The ... couple in an essentially two-dimensional situation (see Fig 5.9) The Bretherton flow belonging to the wavepacket is described by (5 .105 ) In the three-dimensional Boussinesq system the Bretherton...
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Lecture Notes in Control and Information Sciences Editors: M. Thoma · M. Morari316.R.V. Patel pptx

Lecture Notes in Control and Information Sciences Editors: M. Thoma · M. Morari316.R.V. Patel pptx

... transformation mapping J e · · to q Let us decompose q as follows: · · · q = q +q (2.3.32) · q · q (2.3.33) P where P Je Je Using the definition of null space, we can write: · · · · · · X = Je q = ... differential kinematics are given in (2.2.4) We rewrite the equation as: · · · · X – Je q = Je q (2.3.29) · Following the procedure in Section 2.3.1, a similar formulation for q can be obtained to ... general form of a minimum 2-norm solution to the following least-squares problem: · · · · q J e q – X – J e q · (2.3.31) The solutions which are aimed at minimizing the norm of the joint acceleration...
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Tài liệu Lecture Notes in Control and Information SciencesEditors: M. Thoma pdf

Tài liệu Lecture Notes in Control and Information SciencesEditors: M. Thoma pdf

... characteristic in working coordinate by using nonlinear coordinate transform between the working coordinate and the joint coordinate about articulated robot arm (2) Servo Controller of Industrial ... input time interval Objective joint angle Inverse kinematics Servo controller [ Working coordinate ] Following joint angle Motor 37 Following trajectory Kinematics Fig 2.10 Block diagram of industrial ... divided into small intervals Concerning the various trajectories divided from the objective trajectory, the beginning point and end point in working coordinates within one divided small interval...
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