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For the family is the simplest example of just such a unit, composed of people, which gives us both some immunity from, and a way of dealing with, other people.
For example, suppose a man wearing a $200 watch, driving a 1959 Rolls Royce, stops to ask a man on the sidewalk, `` What time is it ''??
For example, there are persons who are in physical science, in the field of mineralogy, trained in crystallography, who use only X-rays, applying only the powder technique of X-ray diffraction, to clay minerals only, and who have spent the last fifteen years concentrating on the montmorillonites ; ;
For example, No. 56 printed the patent giving the Electoral Prince the title of Duke of Cambridge.
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For example, in the third chapter of Matthew, verses 13-16, describing the baptism of Jesus, the 1611 version reads:
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For example, for the problem Af, 10 from 25 equals 15, then 6 from 15 equals 9.
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For an example let's dream up an engine that has a final combustion chamber volume of 5 cubic inches and a cylinder volume of 45 cubic inches.
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For and Gaussian
For a Gaussian response system ( or a simple RC roll off ), the rise time is approximated by:
For general matrices, Gaussian elimination is usually considered to be stable in practice if you use partial pivoting as described below, even though there are examples for which it is unstable.
For example, if one assumes that data arise from a univariate Gaussian distribution, then one has assumed a Gaussian model:.
For example, a mixture of Gaussians with one Gaussian at each data point is dense is the space of distributions.
For example, a common choice for A < sub > o </ sub > is a Gaussian wave packet:
For example, a Gaussian wavefunction ψ might take the form:
For an ideal single-mode Gaussian beam, the D4σ, D86 and 1 / e < sup > 2 </ sup > width measurements would give the same value.
For both families, the lowest-order solution describes a Gaussian beam, while higher-order solutions describe higher-order transverse modes in an optical resonator.
For a Gaussian beam propagating in free space, the spot size ( radius ) w ( z ) will be at a minimum value w < sub > 0 </ sub > at one place along the beam axis, known as the beam waist.
For a Gaussian beam, the BPP is the product of the beam's divergence and waist size.
For a Gaussian intensity ( i. e. power density, W / m < sup > 2 </ sup >) distribution in a single-mode optical fiber, the mode field diameter is that at which the electric and magnetic field strengths are reduced to 1 / e of their maximum values, i. e., the diameter at which power density is reduced to 1 / e < sup > 2 </ sup > of the maximum power density, because the power density is proportional to the square of the field strength.
For large numbers the Poisson distribution approaches a normal distribution, typically making shot noise in actual observations indistinguishable from true Gaussian noise except when the elementary events ( photons, electrons, etc.
For example, the inverse of cumulative Gaussian distribution
For sufficiently nice prior probabilities, the Bernstein-von Mises theorem gives that in the limit of infinite trials and the posterior converges to a Gaussian distribution independent of the initial prior under some conditions firstly outlined and rigorously proven by Joseph Leo Doob in 1948, namely if the random variable in consideration has a finite probability space.
For any affine transformation of the Gaussian plane, z mapping to a z + b, a ≠ 0, a triangle is transformed but does not change its shape.
For a Gaussian distribution this is the best unbiased estimator ( that is, it has the lowest MSE among all unbiased estimators ), but not, say, for a uniform distribution.
For a Gaussian distribution, where, this means the MSE is minimized when dividing the sum by, whereas for a Bernoulli distribution with p = 1 / 2 ( a coin flip ),, the MSE is minimized for.
For example, for a laser producing pulses with a Gaussian temporal shape, the minimum possible pulse duration Δt is given by
For the HeNe laser with a 1. 5 GHz spectral width, the shortest Gaussian pulse consistent with this spectral width would be around 300 picoseconds ; for the 128 THz bandwidth Ti: sapphire laser, this spectral width would be only 3. 4 femtoseconds.
For large α, the shape of the Kaiser window ( in both time and frequency domain ) tends to a Gaussian curve.
For the Gaussian random approximation, the structure function of Tatarski ( 1961 ) can be described in terms
* For an orthogonal parametrization ( i. e., ), Gaussian curvature is:
* For a surface described as graph of a function, Gaussian curvature is:

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