Geometric arrangement for Fresnel's calculation Consider the case of a point source located at a point P < sub > 0 </ sub >, vibrating at a frequency f. The disturbance may be described by a complex variable U < sub > 0 </ sub > known as the complex amplitude.

Consider the case in which liquid crystal molecules are aligned parallel to the surface and an electric field is applied perpendicular to the cell as in the following diagram.

Consider the case of an airfoil accelerating from rest in a viscous flow.

Consider also the case of a vessel leaving a star system, or heading to the outer planets.

Consider the case where the far end of the cable is shorted ( that is, it is terminated into zero ohms impedance ).

Argument from rarity – Consider this case: a lottery winner is accused of cheating, based on the improbability of winning.

Consider the case when bits are already exchanged between the parties.

Consider the simplest case, a system with one independent variable, time.

Consider the simple case of two-body system, where object A is moving towards another object B which is initially at rest ( in any particular frame of reference ).

Consider the special case in which the axis of rotation lies in the xy plane.

Consider the manufacture and sale of any item, which in this case we will call a widget.

Consider the following quote: " How can the fact that, in the case of the brains in a vat, the language is connected by the program with sensory inputs which do not intrinsically or extrinsically represent trees ( or anything external ) possibly bring it about that the whole system of representations, the language in use, does refer to or represent trees or any thing external?

Consider the following theorem ( which is a case of the Pigeonhole Principle ):

Consider the case when a child executes an "" system call ( which is used to execute any executable file from within a C program ) or exits very soon after the.

Consider the Gram – Schmidt process applied to the columns of the full column rank matrix, with inner product ( or for the complex case ).

Consider a case of a level sensing platform on an aircraft flying due North with its three gimbal axes mutually perpendicular ( i. e., roll, pitch and yaw angles each zero ).

Consider the expression: in this case, the dummy variable of the product is not mentioned within the term.

Consider that in the case of the Mount Isa orebody, large amounts of capital are required to sink shafts and associated underground infrastructure, then laboriously drill and blast the ore, crush and process it, to extract the base metals, an activity which requires a large workforce.

Consider the case where ( that is, the jth element is one and all others zero ).

Consider the case when the surfaces are flat and planar cross-sections.

Consider the special case N = 1.

Consider the following test case: The field f has been on for infinite time and is switched off at t = 0

Consider the case this way-to a cat, catching and eating mice is perfectly natural and morally sound.

Consider the case of a 2-by-2 matrix

Consider it as a standby setup, at negligible cost, for those emergencies when the furnace quits, a blizzard holds up fuel delivery, or for cool summer mornings or evenings when you don't want to start up your whole heating plant.

Consider what happened during World War 1,, when the Protestant churches united to push the Prohibition law through Congress.

Consider, for example, what happens when an object in the periphery of the visual field moves, and a person looks toward it.

Consider, for example, that when the bride says " I do " at the appropriate time in a wedding, she is performing the act of taking this man to be her lawful wedded husband.

Consider, also, that all English speakers often pronounce ' Z ' where ' S ' is spelled, almost always when a noun ending in a voiced consonant or a liquid is pluralized, for example " seasons ", " beams ", " examples ", etc.

Consider what happens when the temperature of body " A " changes, but that of the Earth does not.

Consider a moment when a vertex's distance is updated by

Consider this snippet of C code as an example of the ambiguity encountered when determining SLOC:

But the one thing that I didn't expect was when an older player came to talk to me after the first concert and said, ' Consider this your future home.

Consider for example when a military is organising a secret attack against another nation: it may suffice to alert the other nation for them to know merely that there is a lot of secret activity going on.

Consider applying creational patterns when:

Consider a person standing in the rain on a day when there is no wind.

Consider the following when selecting clothing:

Consider what happens when someone sends a message to the list.

Consider what happens when we add two more voters ( to keep the total number odd ).

Consider some set P and a binary relation ≤ on P. Then ≤ is a preorder, or quasiorder, if it is reflexive and transitive, i. e., for all a, b and c in P, we have that:

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:

Again we start with a C < sup >∞</ sup > manifold, M, and a point, x, in M. Consider the ideal, I, in C < sup >∞</ sup >( M ) consisting of all functions, ƒ, such that ƒ ( x ) = 0.

Consider these three things we say about God: first, God is a spirit ; second, God is the creator of the world ; and third, God exists apart from space and time.

Consider a wave function that is a sum of many waves, however, we may write this as

Consider, for example cutlery: If one collection of cutlery is combined with another, we still have " cutlery.

Consider the implication " if I am in Massachusetts, then I am in North America ", which we might alternatively express as, " if I were in Massachusetts, then I would be in North America ".

Consider the approach we would take classically-we pick one block at random, and then perform a normal search through the rest of the blocks ( in set theory language, the compliment ).

Consider a non-interacting fermion system ( a Fermi gas ), and suppose we " turn on " the interaction slowly.

Consider an MDCT with 2N inputs and N outputs, where we divide the inputs into four blocks ( a, b, c, d ) each of size N / 2.

Consider a polygon P and a triangle T, with one edge in common with P. Assume Pick's theorem is true for both P and T separately ; we want to show that it is also true to the polygon PT obtained by adding T to P. Since P and T share an edge, all the boundary points along the edge in common are merged to interior points, except for the two endpoints of the edge, which are merged to boundary points.

Consider two waveforms f and g. By calculating the convolution, we determine how much a reversed function g must be shifted along the x-axis to become identical to function f. The convolution function essentially reverses and slides function g along the axis, and calculates the integral of their ( f and the reversed and shifted g ) product for each possible amount of sliding.

Consider a sphere S ( r ) with radius r. A point on the sphere is identified by its latitude φ and longitude λ, for which we introduce the random variables Φ and Λ that take values in Ω < sub > 1 </ sub > = respectively Ω < sub > 2 </ sub > =.

Consider the previous example with men's heights and suppose we have a random sample of n people.

Consider the Laurent expansion at all such z and subtract off the singular part: we are left with a function on the Riemann sphere with values in C, which by Liouville's theorem is constant.

Consider the Laurent series of f ( z ) about i, the only singularity we need to consider.

Consider the problem of estimating the probability that a test point in N-dimensional Euclidean space belongs to a set, where we are given sample points that definitely belong to that set.

Consider for example the proceedings that we call ' games '.

" Consider what is likely to happen if we don't further in aging research.

Consider what we have done to the Native Americans in this country-from the time of Columbus to the time of the great Western Migration.

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.