Examples of using Is a vector in English and their translations into Turkish
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Colloquial
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Ecclesiastic
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Ecclesiastic
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Computer
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Programming
This is a vector.
We all know that force is a vector.
This is a vector as a function over time.
So if I draw a vector like this, if I draw a circle with an x in it like that, that is a vector that's going into the page or into the screen.
The gluon is a vector boson; like the photon, it has a spin of 1.
That's a vector-- so I put these funny little arrows on top-- times time plus the acceleration-- and, of course,acceleration is a vector-- times time squared over 2.
Properties==The gluon is a vector boson; like the photon, it has a spin of 1.
With this convention for depicting rotation, the velocity is given by a vector cross product as v ω× r,{\displaystyle\mathbf{v}={\boldsymbol{\omega}}\times\mathbf{r}\,} which is a vector perpendicular to both ω and r(t), tangential to the orbit, and of magnitude ω r.
Black Widow is a vector arcade game developed by Atari, Inc. released in 1982.
By combining the Lorentz force law above with the definition of electrical current, the following equation results, in the case of a straight, stationary wire::formula_10where ℓ is a vector whose magnitude is the length of wire, and whose direction is along the wire, aligned with the direction of conventional current flow"I.
The insect is a vector of Crimean-Congo hemorrhagic fever, a disease fatal to humans.
If"V" is a vector space with dual space"V"∗, then the application operator, is a bilinear map from to the base field.
As the electric field is defined in terms of force, and force is a vector, so it follows that an electric field is also a vector, having both magnitude and direction.
It is a vector for Avipoxvirus, Newcastle disease virus, Falconid herpesvirus 1(and possibly other Herpesviridae), and some mycoses and bacterial infections.
The simplest example is the photon: a photon is a vector particle it has an inner"arrow" which points to some direction, its polarization.
So this is a vector that's going into the page and this is a vector that's going out of the page. So we know that n is perpendicular to both a and b, and so the only way you can get a vector that's perpendicular to both of these, it essentially has to be perpendicular, or normal, or orthogonal to the plane that's your computer screen.
Because the potential has no angular components, its gradient is: formula_4where x is a vector of length"x" pointing from the point mass toward the small body andformula_5 is a unit vector pointing from the point mass toward the small body.
If a vector space V over the real numbers R carries an inner product, then the inner product is a bilinear map V× V→ R. In general, for a vector space V over a field F, a bilinear form on V is the same as a bilinearmap V× V→ F. If V is a vector space with dual space V∗, then the application operator, b(f, v) f(v) is a bilinear map from V∗× V to the base field.
Shown here is a vector presentation indicating, for two different positions, P1 and P2, of the Moon in its orbit around the Earth, the respective vectors LS1 and LS2 for the perturbing acceleration due to the Sun.
In mathematics, a weak Lie algebra bundle ξ( ξ, p, X, θ){\displaystyle\xi=(\xi, p,X,\theta)\,} is a vector bundle ξ{\displaystyle\xi\,} over a base space X together with a morphism θ: ξ⊗ ξ→ ξ{\displaystyle\ theta:\xi\otimes\xi\rightarrow\xi} which induces a Lie algebra structure on each fibre ξ x{\displaystyle\xi_{x}\.
Gravitational field==The gravitational field is a vector field that describes the gravitational force which wouldbe applied on an object in any given point in space, per unit mass.
In functional analysis, an F-space is a vector space V over the real or complex numbers together with a metric d: V× V→ R so that Scalar multiplication in V is continuous with respect to d and the standard metric on R or C. Addition in V is continuous with respect to d.
For a swept angledθ ω dt the change in v is a vector at right angles to v and of magnitude v dθ, which in turn means that the magnitude of the acceleration is given by a v d θ d t v ω v 2 r{\displaystyle a=v{\frac{d\theta}{dt}}=v\omega={\frac{ v^{ 2}}{ r}}} In non-uniform circular motion an object is moving in a circular path with a varying speed.
It's a vector.
Let V be a vector space over a field k.
And obviously, this is going to end up being a vector in Rm, so this whole thing is going to be a vector in Rm.
But we learned that the force on a moving charge from a magnetic field,and it's a vector quantity, is equal to the charge-- on the moving charge-- times the cross product of the velocity of the charge and the magnetic field.