Search results
Results From The WOW.Com Content Network
Parallel transport of tangent vectors is a way of moving vectors from one tangent space to another along a curve in the setting of a general Riemannian manifold. Note that while the vectors are in the tangent space of the manifold, they might not be in the tangent space of the curve they are being transported along.
parallel, if they do not intersect in the plane, but converge to a common limit point at infinity (ideal point), or; ultra parallel, if they do not have a common limit point at infinity. [17] In the literature ultra parallel geodesics are often called non-intersecting. Geodesics intersecting at infinity are called limiting parallel.
These operations and associated laws qualify Euclidean vectors as an example of the more generalized concept of vectors defined simply as elements of a vector space. Vectors play an important role in physics: the velocity and acceleration of a moving object and the forces acting on it can all be described with vectors. [7]
For vectors with complex entries, using the given definition of the dot product would lead to quite different properties. For instance, the dot product of a vector with itself could be zero without the vector being the zero vector (e.g. this would happen with the vector a = [ 1 i ] {\displaystyle \mathbf {a} =[1\ i]} ).
The rejection of a vector from a plane is its orthogonal projection on a straight line which is orthogonal to that plane. Both are vectors. The first is parallel to the plane, the second is orthogonal. For a given vector and plane, the sum of projection and rejection is equal to the original vector.
Left: The vectors b and c are resolved into parallel and perpendicular components to a. Right: The parallel components vanish in the cross product, only the perpendicular components shown in the plane perpendicular to a remain. [12] The two nonequivalent triple cross products of three vectors a, b, c. In each case, two vectors define a plane ...
Such tangent vectors are said to be parallel transports of each other. Nonzero parallel vector fields do not, in general, exist, because the equation ∇ X = 0 is a partial differential equation which is overdetermined : the integrability condition for this equation is the vanishing of the curvature of ∇ (see below).
Consider n-dimensional vectors that are formed as a list of n scalars, such as the three-dimensional vectors = [] = []. These vectors are said to be scalar multiples of each other, or parallel or collinear , if there is a scalar λ such that x = λ y . {\displaystyle \mathbf {x} =\lambda \mathbf {y} .}