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Consider and region
Consider a heart attack which damages the region of the heart between the SA node and the atrial foci.
Consider the entry corresponding to a particular region and crossing.

Consider and D
Suppose that U: D → C is a functor from a category D to a category C, and let X be an object of C. Consider the following dual ( opposite ) notions:
Consider a domain D in m-dimensional x space, with boundary B.
Consider a list with items and with R1 and R2 being registers containing, respectively, the address of the current ( say C ) list item and a work register containing the XOR of the current address with the previous address ( say C ⊕ D ).
Consider polynomials P ( x ), D ( x ) where degree ( D ) < degree ( P ).
Consider a relation variable ( relvar ) R with attributes ( A, B, C, D ) that has only the following two legal values r1 and r2:
Consider the first-order differential operators D < sub > i </ sub > to be infinitesimal operators on Euclidean space.
Consider an election in which there are 4 candidates A, B, C and D, each voter expresses a top-to-bottom ordering of the candidates, and the voters ' orderings are as follows:
Consider one example of what attracted attention to the style of Hand D.
Consider for example the dihedral group D < sub > 4 </ sub > of symmetries of a square.
Consider a once-punctured elliptic curve, given as the locus D of complex points satisfying, where and is a complex number.
Consider a triangle ABC Let D be the midpoint of, E be the midpoint of, F be the midpoint of, and O be the centroid.
Among the NCEW ’ s strongest champions for LTEs was Ronald D. Clark of the St. Paul Pioneer Press, who wrote, " Consider letters as a barometer of how well ( you are ) engaging readers or viewers.
Consider, for example, the case where Y is the disc D < sup > 2 </ sup >, and

Consider and plane
Consider a simple, closed, plane curve C which is a real-analytic image of the unit circle, and which is given by Af.
Consider, for example, the implication this has for plane rotations.
Consider the plane spanned by and, where is a ket in the subspace perpendicular to.
Consider an open subset U of the complex plane C. Let a be an element of U, and f: U
Consider the special case in which the axis of rotation lies in the xy plane.
Consider two points A and B in two dimensional plane flow.
Consider two dimensional plane flow within a Cartesian coordinate system.
Consider a sphere B of radius 1 and a plane P touching B at the South Pole S of B.
Consider now the Minkowski plane: R < sup > 2 </ sup > equipped with the metric
Consider the ( Euclidean ) complex plane equipped with the metric
* Consider a uniform layer of fluid over an infinite horizontal plane.
Consider a " small " light source located on-axis in the object plane of the lens.
Consider a plane with a compact arrangement of spheres on it.
Consider a pair of parallel lines in an affine plane A.
Consider the example of moving along a curve γ ( t ) in the Euclidean plane.
Consider a planar projection of each knot and suppose these projections are disjoint. Find a rectangle in the plane where one pair of sides are arcs along each knot but is otherwise disjoint from the knots.
Consider a point in a continuum under a state of plane stress, or plane strain, with stress components and all other stress components equal to zero ( Figure 7. 1, Figure 8. 1 ).
Consider a set of points R ( R is a vector depicting a point in a Bravais lattice ) constituting a Bravais lattice, and a plane wave defined by:
Consider the illustration, depicting a plane intersecting a cone to form an ellipse ( the interior of the ellipse is colored light blue ).
Consider two proof masses vibrating in plane ( as in the MEMS gyro ) at frequency.
* Consider a triangle in the plane with unequal sides.
Consider an inertial observer in Minkowski spacetime who encounters a sandwich plane wave.
Consider a plane wave where all perturbed quantities vary as exp ( i ( kx-ωt )).

Consider and unit
* Consider the set of all functions from the real number line to the closed unit interval, and define a topology on so that a sequence in converges towards if and only if converges towards for all.
#: Consider a unit sphere placed at the origin, a rotation around the x, y or z axis will map the sphere onto itself, indeed any rotation about a line through the origin can be expressed as a combination of rotations around the three-coordinate axis, see Euler angles.
Consider for instance the open unit disc, a non-compact Riemann surface without boundary, with curvature 0 and with Euler characteristic 1: the Gauss – Bonnet formula does not work.
Consider the unit circle.
Consider a curve lying on a submanifold in ambient manifold, parametrized by arclength, with unit tangent vector.
Consider the unit circle which is described by the ordinary ( Cartesian ) equation
Consider the unit circle S, and the action on S by a group G consisting of all rational rotations.
Consider an FCC compound unit cell.
In the case that T acts on euclidean space R < sup > n </ sup >, there is a simple geometric interpretation for the singular values: Consider the image by T of the unit sphere ; this is an ellipsoid, and its semi-axes are the singular values of T ( the figure provides an example in R < sup > 2 </ sup >).
Consider the set F of all those holomorphic functions f on the unit disk for which
Consider the simplified case of a vehicle with constant mass accelerating vertically upwards with a constant thrust per unit mass a in a gravitational field of strength g. The actual acceleration of the craft is a-g and it is using delta-v at a rate of a per unit time.
Consider eight cubical boxes of unit volume and unit area of a side.
Consider a unit circle in, shrinking in on itself at a constant rate, i. e. each point on the boundary of the circle moves along its inwards pointing normal at some fixed speed.
Consider a trader who has bought a unit portfolio consisting of one contract each for the Red Party, the Blue Party, and the Green Party, at a cost of $ 1.
Consider, for instance, the top half of the unit circle, x < sup > 2 </ sup > + y < sup > 2 </ sup > = 1, where the y-coordinate is positive ( indicated by the yellow arc in Figure 1 ).
Consider the timelike congruence generated by some timelike unit vector field X, which we should think of as a first order linear partial differential operator.

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