Consider now the force exerted at a certain time.

Consider, friend, as you pass by: As you are now, so once was I.

* Consider now L = Q ( ³ √ 2, ω ), where ω is a primitive third root of unity.

Consider now the acceleration due to the sphere of mass M experienced by a particle in the vicinity of the body of mass m. With R as the distance from the center of M to the center of m, let ∆ r be the ( relatively small ) distance of the particle from the center of the body of mass m. For simplicity, distances are first considered only in the direction pointing towards or away from the sphere of mass M. If the body of mass m is itself a sphere of radius ∆ r, then the new particle considered may be located on its surface, at a distance ( R ± ∆ r ) from the centre of the sphere of mass M, and ∆ r may be taken as positive where the particle's distance from M is greater than R. Leaving aside whatever gravitational acceleration may be experienced by the particle towards m on account of ms own mass, we have the acceleration on the particle due to gravitational force towards M as:

Consider the same aircraft, now travelling vertically instead of horizontally.

Consider now the change of variable.

Consider a hyperelliptic curve of genus over the field where is the power of a prime number and define as but now over the field.

Consider now a PDE of the form

During the course of this study, Derrida not only divulges the exact instances Socrates or his interlocutors make use of this concept, but also reveals the relationship between Plato and Socrates which scholars have kept in secret by questioning the validity of authorship in Plato's letters, where in the second letter Socrates writes: " Consider these fact and take care lest you sometimes come to repent of having now unwisely published your views.

Consider now a more elaborate example.

Consider now the free body diagram of a deformable body, which is composed of an infinite number of differential cubes as shown in the figure.

Consider now the case of disruptive selection.

Consider the sequential execution of the list of statements, s ( i ), and what can now be observed as the computation at statement, j:

Consider now the finite approximations to the Wallis product, obtained by taking the first k terms in the product:

Consider now the following form of v ( r-R ),

They are maps from flat 3-space into the Lie group G. Consider now glueing these two balls together at their boundary S².

Consider now the ring R defined as the intersection

" Consider the lyrics: Prayed through the nights / Felt so alone / Suffered from alienation / Carried the weight on my own / Had to be strong / So I believed / And now I know I've succeeded / In finding the place I conceived.

Consider now a material point neighboring, with position vector.

Consider an inertial observer in Minkowski spacetime who encounters a sandwich plane wave.

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 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 region D in the plane: a unit circle or general polygon — the asymptotics of the problem, which are the interesting aspect, aren't dependent on the exact shape.

* Consider a triangle in the plane with unequal sides.

Consider a plane wave where all perturbed quantities vary as exp ( i ( kx-ωt )).