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1. Preface Many types of heart curves are seen in the site of Heart Curve as one of representation. Although it is tried that a Cardioid is reformed into a heart curve also in this page as samely as in the section 3 of the page of Heart Curve II (described in ),
the generalized treatment is performed in this page, and then,
the conversion equation of Eq.(9b) in the section 3 of the page of Heart Curve II is displaced to the equation using inverse-sinusoidal function etc.
from using the square root function.
2. Fundamental properties Though the Cardioid is introduced in the page of Wolfram Math World, the equation expressing a Cardioid is rewritten as the following after the length and the width are replaced. ,
(1)
where and indicate the moving radius and the phase angle respectively.
Here, we try to make a corner on the bottom of the Cardioid so as to converse the phase angle of a Cardioid (in Fig.1)
into the phase angle of a heart curve (in Fig.2) in the manner as shown in Fig.3.
Then, if the inverse-conversion function is given as , the following relation is expressed as
.
(2)
Thus, we should make a corner on the bottom of the Cardioid. |
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from into
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Moreover, in order to obtain beautiful shape of heart figure, both of the coefficient for the reformation
and the compression coefficient in the length direction
are included in the following conversion equations in the coordinates.
,
(3a)
and .
(3b)
3. The case using the inverse-sinusoidal function as
We adopt the following equation using a linear combination of the inverse-sinusoidal function and the proportional relation , which combination satisfies the characteristics given in Fig.3.
,
(4)
where is the positive real number.
may be regarded as a strength of the conversion.
It has to be taken in account that has not periodicity
and is applied only in the range of as shown in Fig.3.
In the result to use the above equation, a heart curve is expected to have a gentle cut on the heart. However, sharpness under the heart may tend to flow lengthily. By calculating Eqs.(1), (2), (3a), (3b) and (4), the coordinate data of a heart curve are obtained.
Examples of such obtained curves in the case of are shown in Figs.4 to 19
where decides only the size and does not relate to the shape.
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When the above figures are painted, these are shown in the followings.
4. The case using the inverse-sinusoidal function with narrower period interval as
In the previous section, sharpness under a heart tends to flow lengthily. Here, this tendency will be corrected. Though the full range of one period interval of the inverse sinusoidal function
was adopted in the previous section, the narrower period interval
(where ) is adopted here.
Then, the following linear combination of the inverse-sinusoidal function with narrower period interval and
the proportional relation is used instead of Eq.(4) written in the previous section.
,
(5)
where .
When , Eq.(5) is led to Eq.(4).
By calculating Eqs.(1), (2), (3a), (3b) and (5), the coordinate data of heart curves are obtained.
Examples of such obtained curves in the case of are shown in Figs.21 to 36
where decides only the size and does not relate to the shape.
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When the above figures are painted, these are shown in the followings.
5 The case using the tangential function as
As the conversion equation ,
we consider the following equation using a linear combination of the tangential function and the proportional relation ,
which combination nearly satisfies the characteristics given in Fig.3.
,
(6)
where and indicate the weighting ratios in respect to
the tangent function and the proportional relation respectively.
Therefore, is regarded as the coefficient expressing so-called degree of strength of the conversion.
is the arbitrary constant which is introduced to adjust the tangential function
to the boundaries of the curve in Fig.3 under the condition of as a principle.
By calculating Eqs.(1), (2), (3a), (3b) and (6), the coordinate data of heart curves are obtained.
Examples of such obtained curves are shown in Fig.37,
where is generally taken because the coefficient
relates only to the whole syze of the curve and does not relate to the shape of the curve.
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When the above figures are painted, these are shown in the followings.
6 The case using the inverse hyperbolic-tangential function as
As the conversion equation ,
we consider the following equation using a linear combination of the inverse hyperbolic-tangential function and
the proportional relation ,
which combination nearly satisfies the characteristics given in Fig.3.
,
(7)
where and indicate the weighting ratios in respect to
the inverse hyperbolic-tangential function and the proportional relation respectively.
Therefore, is regarded as the coefficient expressing so-called degree of strength of the conversion.
is the arbitrary constant which is introduced to adjust the inverse hyperbolic-tangent function
to the boundaries of the curve in Fig.3 under the condition of .
By calculating Eqs.(1), (2), (3a), (3b) and (7), the coordinate data of heart curves are obtained.
Examples of such obtained curves in the case of are shown in Fig.38,
where decides only the size and does not relate to the shape.
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When the above figures are painted, these are shown in the followings.
7 The case using the inverse Fermi distibution function as
Fermi distibution function is the energy distribution function of Fermi particles
(for example, electrons) in quantum mechanics and is given by the followings;
,
(8)
where denotes the particle energy normalized by the thermal energy.
The inverse function of Eq.(8) gives the curve resembling to that shown in Fig.3.
Thus, as the conversion equation ,
we consider the following equation using a linear combination of the inverse Fermi distibution function and
the proportional relation ,
which combination nearly satisfies the characteristics given in Fig.3.
,
(9)
where and indicate the weighting ratios in respect to
the inverse Fermi distibution function and the proportional relation respectively.
Therefore, is regarded as the coefficient expressing so-called degree of strength of the conversion.
is the arbitrary constant which is introduced to adjust the inverse Fermi distibution function
to the boundaries of the curve in Fig.3 under the condition of .
By calculating Eqs.(1), (2), (3a), (3b) and (9), the coordinate data of heart curves are obtained.
Examples of such obtained curves in the case of are shown in Fig.39,
where decides only the size and does not relate to the shape.
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When the above figures are painted, these are shown in the followings.
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