Consider taking the ratio of two probabilities:

( Consider the difference between book and books.

( Consider the difference between he ( nominative ) and him ( dative or accusative ), as in " He saw it " and " It saw him ".

* Consider the modulo 2 equivalence relation on the set of integers: if and only if their difference is an even number.

Consider the difference that arises in selecting the lumped element view of a circuit rather than the electrodynamic view of the same device.

Consider the difference between singing “ oooh ” and “ aaah ”, at the same pitch.

Consider, for example, the difference between strong and weak convergence of functions in the Hilbert space L < sup > 2 </ sup >( R < sup > n </ sup >).

Consider the difference between affirmative action ( systematic ) compared to racism and caste ( systemic ).

Consider the difference between a carrot and chewed bubble gum.

Consider the difference in values of two limits:

Consider the difference between the function differential and the actual increment:

Consider the difference between having to study a subject in one's native language versus trying to study a subject in a foreign language.

Consider the difference between the epistemic connection expressed by an indicative conditional and the causal or metaphysical relation expressed by a subjunctive conditional:

( Consider: " one team ", " two teams ", " most teams "; " one government ", " two governments ", " many governments ").

Consider two systems ; S < sub > 1 </ sub > and S < sub > 2 </ sub > at the same temperature and capable of exchanging particles.

Consider the following two probabilities, assuming a fair coin:

* The Infinite Moment ( 1961 ) ( US edition of Consider Her Ways, with two stories dropped, two others added )

Consider the following two examples.

Consider two observers O and O ', each using their own Cartesian coordinate system to measure space and time intervals.

Consider two noninteracting systems and, with respective Hilbert spaces and.

Consider two ISPs, A and B, which each have a presence in New York, connected by a fast link with latency 5 ms ; and which each have a presence in London connected by a 5 ms link.

Consider the two endpoints of a rod of length L. The length can be determined from the differences in the three coordinates Δx, Δy and Δz of the two endpoints in a given reference frame

Consider the 1592 season of Lord Strange's Men at the Rose Theatre as far more representative: between Feb. 19 and June 23 the company played six days a week, minus Good Friday and two other days.

Consider a sample space generated by two random variables and.

Consider two instances of Bayes ' theorem:

Consider code that adds two numbers and then multiplies by a third ; in the Cray, these would all be fetched at once, and both added and multiplied in a single operation.

Consider two transactions.

Consider the following two lists:

Consider two particles, denoted by subscripts 1 and 2.

Consider dividing the largest rectangle in two triangles, cutting along the diagonal.

Consider two variables said to be " inversely proportional " to each other.

: Consider two even integers x and y.

Consider Thomas Hood's " Bridge of Sighs :", in which the lines are of two feet, each composed of three syllables:

Consider a simple banking application where two users have access to the funds in a particular account.

Consider a state of the system, described by the single particle states ..., n < sub > N </ sub >.

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 a particle P that moves on the surface of a circular cylinder, it is possible to align the Z axis of the fixed frame F with the axis of the cylinder.

Consider a particle of mass, moving in a potential field.

Consider a quantum mechanical particle confined to a closed loop ( i. e., a periodic line of period L ).

Consider the example of a one dimensional nonrelativistic particle with a 2D ( i. e. two state ) internal degree of freedom called " spin " ( it's not really spin because " real " spin is for particles in three-dimensional space ).

Consider a particle that enters the contact area at the right side, travels through the contact patch and leaves at the left side.

Consider the case of a spin-1 / 2 particle in a magnetic field.

Consider a second particle with 4-velocity and a 3-velocity.

Consider any process involving an incoming particle with momentum p. For the particle to give a measurable contribution to the amplitude, it has to interact with a number of different particles with momenta via a vertex.

Consider a particle under the action of a non-uniform oscillating field.

Consider a particle or material point with position vector in the undeformed configuration ( Figure 2 ).