Examples of using Cartesian in English and their translations into Turkish
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My name is Nancy Cartesian.
What? What? Cartesian coordinates.
Allow me to be our office Cartesian.
Of course, coded cartesian coordinates. Cartesian coordinates.
Some things aren't on the cartesian plane.
People also translate
The spy inside Cartesian is the killer, and I have an excellent plan for their capture.
To be our office Cartesian. Allow me.
If x and y are represented in Cartesian coordinates, then the dot product is defined by: formula_1The dot product satisfies the properties: It is symmetric in x and y: x· y y· x.
The trick is to translate it into modern Cartesian coordinates.
What great opponent of Cartesian dualism resists the reduction of psychological phenomena to physical states?
I have enhanced the viewing matrix… the yaw, pitch and roll… to give us the exact position and orientation of our baby. Yeah.to track both the Cartesian coordinates and three altitude angles.
The viewing matrix to track both the Cartesian coordinates the exact position and orientation of our baby.- Yeah. I have enhanced and three altitude angles, the yaw, pitch and roll to give us.
The vortex model of 1944, formulated by German physicist and philosopher Baron Carl Friedrich von Weizsäcker,which harkens back to the Cartesian model, involved a pattern of turbulence-induced eddies in a Laplacian nebular disc.
In the general n{\displaystyle n}-dimensional Cartesian space R n{\displaystyle\mathbb{R}^{n}}, the distance is measured from a fixed hyperplane parallel to the direction of displacement.
For instance, a physical problem with spherical symmetry defined in R3(for example, motion of particles under the influence of central forces)is usually easier to solve in spherical polar coordinates than in Cartesian coordinates.
And so you could also specify this point-- instead of specifying,this is the Cartesian coordinates, this is x comma y-- you could also specify it-- maybe, if we can figure out a way to do it.
If Cartesian coordinates in SI units are used, then the components of the position four-vector are given by: x0 t, x1 x, x2 y, and x3 z, where t is time in seconds, and x, y, and z are distances in meters.
A magnetic field is a vector field,but if it is expressed in Cartesian components X, Y, Z, each component is the derivative of the same scalar function called the magnetic potential.
Dimensional Minkowski space, also known as the split-complex plane, is a"complex plane" in thesense that the algebraic split-complex numbers can be separated into two real components that are easily associated with the point(x, y) in the Cartesian plane.
When measuring the height of an inverted image using the cartesian sign convention(where the x-axis is the optical axis) the value for hi will be negative, and as a result M will also be negative.
This article provides a few of the easier ones to follow in the context of special relativity, for the simplest case of a Lorentz boost in standard configuration, i.e. two inertial frames moving relative to each other at constant(uniform) relative velocity less than the speed of light,and using Cartesian coordinates so that the x and x′ axes are collinear.
For example, in 3-D Euclidean space and using Cartesian coordinates; the coordinate vector A(A1, A2, A3)(Ax, Ay, Az) shows a direct correspondence between the subscripts 1, 2, 3 and the labels x, y, z.
And this is a lot more than growing food, as you will see; this is a different way to think about nature anda way to get away from the zero-sum notion, the Cartesian idea that either nature's winning or we're winning, and that for us to get what we want, nature is diminished.
Another example is(slow) fluid in a straight circular pipe: in Cartesian coordinates, one has to solve a(difficult) two dimensional boundary value problem involving a partial differential equation, but in cylindrical coordinates the problem becomes one-dimensional with an ordinary differential equation instead of a partial differential equation.
Computation===== By polar coordinates===A standard way to compute the Gaussian integral, the idea of which goes back to Poisson, is* consider the function"e"-("x"2+"y"2)"e"-"r"2 on the plane R2, and compute its integral two ways:* on the one hand,by double integration in the Cartesian coordinate system, its integral is a square:*: formula_4* on the other hand, by shell integration(a case of double integration in polar coordinates), its integral is computed to be π.
While vector operations andphysical laws are normally easiest to derive in Cartesian coordinates, non-Cartesian orthogonal coordinates are often used instead for the solution of various problems, especially boundary value problems, such as those arising in field theories of quantum mechanics, fluid flow, electrodynamics and the diffusion of chemical species or heat.
In 1952 Georges de Rham proved the de Rham decomposition theorem,a principle for splitting a Riemannian manifold into a Cartesian product of Riemannian manifolds by splitting the tangent bundle into irreducible spaces under the action of the local holonomy groups.
In flat spacetime and using Cartesian coordinates, if one combines this with the symmetry of the stress-energy tensor, one can show that angular momentum is also conserved: 0( x α T μ ν- x μ T α ν), ν.{\displaystyle 0=(x^{\alpha}T^{\mu\nu}-x^{\mu}T^{\alpha\nu})_{,\nu}.\!} When gravity is non-negligible or when using arbitrary coordinate systems, the divergence of the stress-energy still vanishes.
Swiss astronomer Louis Jacot(in 1951, 1962, 1981), like Weisacker and Ter Haar,continued the Cartesian idea of vortices but proposed a hierarchy of vortices or vortices within vortices, i.e., a lunar system vortex, a Solar System vortex, and a galactic vortex.
For example, the pressure wave due to an explosion far from the ground(or other barriers)depends on 3D space in Cartesian coordinates, however the pressure predominantly moves away from the center, so that in spherical coordinates the problem becomes very nearly one-dimensional since the pressure wave dominantly depends only on time and the distance from the center.