The Ohio Journal of Science. Vol. XVI., No. 2 (December, 1915) — John Shaqi
The Ohio Journal of Science. Vol. XVI., No. 2 (December, 1915)Various
History
The Ohio Journal of Science. Vol. XVI., No. 2 (December, 1915)
Various
Natural history -- Periodicals; Science -- Periodicals
In this article we shall discuss the geometry of the curves which
Edgeworth obtains by this transformation and derive a method for an
approximate solution of the two equations, one of the fourth and the
other of the sixth degree, which arise in the fitting of a curve of
this class.
In order that the final curve may be written in terms of the
co-ordinates x and y the equation of the base or generating normal
probability curve is written:
1
z = —————— e^(—(t^2/2))
√(2π)
where t denotes abscissas and z ordinates.
Let the abscissas of the transformed curve be functions of the
corresponding abscissas of the base curve. Then it may be assumed that
x can be developed in powers of t, and hence we may write on omitting
fourth and higher powers,
x = a(t + κt^2 + λt^3),
where a, κ and λ are constants to be determined in “fitting” the curve.
Since x denotes the value of a measurement and y the frequency of x,
that is, the number of individuals possessing that value of x, the
magnitude of an element of area denotes the number of individuals
between two values of x. Obviously, therefore, if the transformation is
to be of concrete value the magnitude of an element of area must not be
altered, though of course the shape will be changed. Hence
y dx = z dt,
and y = z dt/dx
1 1
= —————— e^(—(t^2/2)) · ——————————————————
√(2π) a(1 + 2κt + 3λt^2)
The formulas of transformation are thus:
x = a(t + κt^2 + λt^3),
1 1
y = —————— e^(—(t^2/2)) · ——————————————————
√(2π) a(1 + 2κt + 3λt^2)
=Maximum and Minimum Points.= Since only curves with one maximum
point or mode are practically useful it is desirable to determine what
values of the constants a, κ and λ give unimodal curves.
We have
dy dy dt
——— = ——— · ———
dx dt dx
1 (3λt^3 + 2κt^2 + (1 + 6λ)t + 2κ)
= —————— e^(—(t^2/2)) · ————————————————————————————————
√(2π) a(1 + 2κt + 3λt^2)
From the vanishing of the numerator of dy/dx there must result either
one or three real modes for each pair of values for λ and κ, that is,
for each translated curve. To determine what values of λ and κ give
uni-modal curves and what tri-modal it is convenient to consider the
plane of λ and κ.
The discriminant of the equation
3λt^3 + 2κt^2 + (1 + 6λ)t + 2κ = 0
is
16κ^4 - κ^2(1 + 66λ + 117λ^2) + 3λ(1 + 6λ)^3 = 0
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