warn for text as path being impossible without a font

[PyX.git] / design / beziers.tex

\documentclass{article}
\usepackage{amsmath}
\usepackage{array}
\usepackage{graphicx}
\newcommand{\sign}{\operatorname{sign}}

\begin{document}

\section{B\'ezier curves with prescribed tangent directions and curvatures at the endpoints}

% <<<
Parameterization of the B\'ezier curve, for $x(t)$ and $y(t)$ equivalently,
%
\begin{align}
  x(t) &= x_0(1-t)^3 + 3x_1t(1-t)^2 + 3x_2t^2(1-t) + x_3 t^3\\
  \dot x(t) &= 3(x_1-x_0)(1-t)^2 + 3(x_3-x_2)t^2 + 6(x_2-x_1)t(1-t) \\
  \ddot x(t) &= 6(x_0 - 2x_1 + x_2)(1-t) + 6(x_1-2x_2+x_3) t \\
  \dddot x(t) &= 6(x_3-x_0) + 18(x_1-x_2)
\end{align}
%
The curvature is
\begin{equation}
  \kappa(t) = \frac{\dot x\ddot y - \ddot x\dot y}{[\dot x^2 + \dot y^2]^{3/2}}
\end{equation}
%
with the sign
%
\begin{equation}
  \begin{aligned}
    \sign\kappa &> 0 \quad\text{for left bendings}\\
    \sign\kappa &< 0 \quad\text{for right bendings.}
  \end{aligned}
\end{equation}
%
At the endpoints we can summarize:
%
\begin{align}
  \dot x(0)  &= 3(x_1 - x_0) \\
  \dot x(1)  &= 3(x_3 - x_2) \\
  \ddot x(0) &= 6(x_0 - 2x_1 + x_2) = -4\dot x(0) - 2\dot x(1) + 6(x_3 - x_0) \\
  \ddot x(1) &= 6(x_1 - 2x_2 + x_3) = +4\dot x(1) + 2\dot x(0) - 6(x_3 - x_0)
\end{align}
%
and the same for the $y$ coordinates.
The equations for the $\ddot x$ contain a convenient parameterization for this
problem, with given endpoints and tangent directions. We now introduce two
parameters for the distances between the first and the last pair of control
points:
%
\begingroup
\arraycolsep=0pt
\begin{align}
  \left(\begin{array}{cc}
    x_1-x_0 \\ y_1-y_0
  \end{array}\right)
  &= \frac{1}{3}
  \left(\begin{array}{cc}
    \dot x(0) \\ \dot y(0)
  \end{array}\right)
  =: \alpha
  \left(\begin{array}{cc}
    t_x(0) \\ t_y(0)
  \end{array}\right) \\
  \left(\begin{array}{cc}
    x_3-x_2 \\ y_3-y_2
  \end{array}\right)
  &= \frac{1}{3}
  \left(\begin{array}{cc}
    \dot x(1) \\ \dot y(1)
  \end{array}\right)
  =: \beta
  \left(\begin{array}{cc}
    t_x(1) \\ t_y(1)
  \end{array}\right) \qquad
\end{align}
\endgroup
%
Here, the externally prescribed tangent vectors are expected to be parallel to
the tangent vectors of the parameterization and normalized to 1. This implies
$\alpha>0$ and $\beta>0$ are the distances between the endpoints and their
corresponding control points.

The problem to now to find proper parameters $\alpha>0$ and $\beta>0$ for a given set of
endpoints $(x_0,y_0)$, $(x_3, y_3)$,
normalized tangent vectors $\mathbf{t}(0)$, $\mathbf{t}(1)$ and of
curvatures $\kappa(0), \kappa(1)$.
The rest of the control points is then given by
%
\begin{equation}
  x_1 = x_0 + \alpha t_x(0) \quad\text{and}\quad
  x_2 = x_3 - \beta  t_x(1).
\end{equation}
%
For the curvatures at the endpoints we get a nonlinear equation,
%
\begin{align}
  \kappa(0) (\dot x^2(0) + \dot y^2(0))^{3/2}
  &= \dot x(0) \ddot y(0) - \ddot x(0) \dot y(0) \\
  = 27 \kappa(0) |\alpha|^3
  &= \begin{aligned}[t]
      &+\dot x(0) \bigl[- 4\dot y(0) - 2\dot y(1) + 6(y_3-y_0)\bigr] \\
      &-\dot y(0) \bigl[- 4\dot x(0) - 2\dot x(1) + 6(x_3-x_0)\bigr]
     \end{aligned}\\
  &= \begin{aligned}[t]
      &-2 \bigl[\dot x(0) \dot y(1) - \dot y(0)\dot x(1)\bigr] \\
      &+6 \bigl[\dot x(0) (y_3-y_0) - \dot y(0) (x_3-x_0)\bigr]
     \end{aligned}\\
  &= \begin{aligned}[t]
      &-18 \alpha\beta \bigl[t_x(0)t_y(1) - t_y(0)t_x(1)\bigr] \\
      &+18 \alpha \bigl[t_x(0) (y_3-y_0) - t_y(0) (x_3-x_0)\bigr]
     \end{aligned}
\end{align}
%
And short,
%
\begin{equation}
  0 = \frac{3}{2}\kappa(0) \alpha^2 \sign(\alpha)
    + \beta \bigl[t_x(0)t_y(1) - t_y(0)t_x(1)\bigr]
    - \bigl[t_x(0) (y_3-y_0) - t_y(0) (x_3-x_0)\bigr]
\end{equation}
%
A similar calculation can be done for the end curvature,
%
\begin{align}
  \kappa(1) (\dot x^2(1) + \dot y^2(1))^{3/2}
  &= \dot x(1) \ddot y(1) - \ddot x(1) \dot y(1) \\
  = 27 \kappa(1) |\beta|^3
  &= \begin{aligned}[t]
       &+\dot x(1) \bigl[ 4\dot y(1) + 2\dot y(0) - 6(y_3-y_0)\bigr] \\
       &-\dot y(1) \bigl[ 4\dot x(1) + 2\dot x(0) - 6(x_3-x_0)\bigr]
     \end{aligned}\\
  &= \begin{aligned}[t]
       &-2 \bigl[\dot x(0) \dot y(1) - \dot y(0)\dot x(1)\bigr] \\
       &-6 \bigl[\dot x(1) (y_3-y_0) - \dot y(1) (x_3-x_0)\bigr]
     \end{aligned}\\
  &= \begin{aligned}[t]
       &-18 \alpha\beta \bigl[t_x(0)t_y(1) - t_y(0)t_x(1)\bigr] \\
       &-18 \beta \bigl[t_x(1) (y_3-y_0) - t_y(1) (x_3-x_0)\bigr]
     \end{aligned}
\end{align}
\begin{equation}
  0 = \frac{3}{2}\kappa(1) \beta^2 \sign(\beta)
    + \alpha \bigl[t_x(0)t_y(1) - t_y(0)t_x(1)\bigr]
    + \bigl[t_x(1) (y_3-y_0) - t_y(1) (x_3-x_0)\bigr]
\end{equation}
%
Alltogether, we find the system of equations that is to be solved.
%
\begin{gather}
  \begin{aligned}
    0 &= \frac{3}{2} \kappa(0) \alpha^2 \sign(\alpha) + \beta T - D \\
    0 &= \frac{3}{2} \kappa(1) \beta^2 \sign(\beta) + \alpha T - E
  \end{aligned}\\[\medskipamount]
  \begin{aligned}
    T &:= t_x(0)t_y(1) - t_y(0)t_x(1) \\
    D &:= \bigl[t_x(0) (y_3-y_0) - t_y(0) (x_3-x_0)\bigr]\\
    E &:= \bigl[t_x(1) (y_0-y_3) - t_y(1) (x_0-x_3)\bigr]
  \end{aligned}
\end{gather}
%
Decoupling the two equations causes problems with the absolute values,
%
\begin{align}
  \alpha = \frac{1}{T}\left(E - \frac{3}{2}\kappa(1)\beta |\beta |\right)\quad\text{and}\quad
  \beta  = \frac{1}{T}\left(D - \frac{3}{2}\kappa(0)\alpha|\alpha|\right)
\end{align}
%
Thus, for $\alpha>0$ and $\beta>0$ we need also
%
\begin{align}
  \frac{1}{T}\left(E - \frac{3}{2}\kappa(1)\beta |\beta |\right) > 0\quad\text{and}\quad
  \frac{1}{T}\left(D - \frac{3}{2}\kappa(0)\alpha|\alpha|\right) > 0
\end{align}
%
which is not always guaranteed. E.g. the combination
%
\begin{equation}
  T>0,\quad E<0\quad\text{and}\quad \kappa(1)>0
\end{equation}
%
is not compatible with a positive value of $\beta$. Under what circumstances do
we get such geometrically invalid results? Tests show that even allowing
arbitrary signs of the curvatures $\kappa(0)$~and $\kappa(1)$ does not help in
all cases.

The decoupled equations can be constructed by inserting $\alpha$~and $\beta$
into the equations for the curvatures. This reads
\begin{align}
  0 &= \frac{3}{2}\kappa(0)\sign(\alpha)
       \left(E - \frac{3}{2}\kappa(1)\beta |\beta |\right)^2
     + \beta T^3 - D T^2 \\
    &= \begin{aligned}[t]
         \frac{27}{8} \kappa(0) \kappa^2(1) \sign(\alpha) \beta^4
       - \frac{9}{2} E \kappa(0) \kappa(1) \sign(\alpha)\sign(\beta) \beta^2
       + \beta T^3 \\
     {}+ \frac{3}{2} \kappa(0) \sign(\alpha) E^2 - D T^2
       \end{aligned}\\
  0 &= \begin{aligned}[t]
         \frac{27}{8} \kappa^2(0) \kappa(1) \sign(\beta) \alpha^4
       - \frac{9}{2} D \kappa(0) \kappa(1) \sign(\alpha)\sign(\beta) \alpha^2
       + \alpha T^3 \\
     {}+ \frac{3}{2} \kappa(1) \sign(\beta) D^2 - E T^2
       \end{aligned}
\end{align}
%
% >>>

\section{Bounding boxes for B\'ezier curves}

% <<<
The bounding box is defined by the minimal and maximal values of a
curve. Hence the problem decouples for the two coordintes $x$ and $y$.
We can search for the minima and maxima within the valid range for the
parameter $t$ together with taking into account the values at the
boundaries at $t=0$ and $t=1$.

For the $x$ coordinate we have:
\begin{align}
  x(t) & = x_0(1-t)^3 + 3x_1t(1-t)^2 + 3x_2t^2(1-t) + x_3 t^3\\
       & = (x_3-3x_2+3x_1-x_0)t^3 + (3x_0-6x_1+3x_2)t^2 + (3x_1-3x_0)t + x_0\\
       & = a\,t^3 + \frac{3}{2}\,b\,t^2 + 3\,c\,t + x_0
\end{align}
%
The constants $a$, $b$, and $c$ are
%
\begin{align}
  a & = x_3-3x_2+3x_1-x_0 \\
  b & = 2x_0-4x_1+2x_2 \\
  c & = x_1-x_0
\end{align}
%
Now $\dot x(t)$ is
%
\begin{equation}
  \dot x(t) = 3\left[\,a\,t^2 + b\,t + c\,\right]
\end{equation}
%
For a numerically stable calculation of the roots of the function, we
first compute
%
\begin{equation}
  q = -\frac{1}{2}\left[\,b+\mathrm{sgn}(b)\sqrt{b^2-4ac}\right]\, .
\end{equation}
%
In case the square root is negative, we only need to take into account
the values at the boundaries. Otherwise we need to take into account
the two solutions
%
\begin{equation}
  t_1 = \frac{q}{a} \quad\text{and}\quad t_2 = \frac{c}{q}
\end{equation}
%
Again, for numerical failures (divisions by zero), we just need to skip
the particular solution. The minima and maxima for $x(t)$ can now
occur at $t=0$, $t=t_1$, $t=t_2$ and $t=1$.

% >>>

\section{Replacing B\'ezier curves by straight lines}

% <<<
\begin{figure}
\centerline{\includegraphics{beziertoline}}
\caption{Example for a replacement of a B\'ezier curve by a straight
line.}
\label{fig:beziertoline}
\end{figure}

To solve certain geometrical tasks like measuring the length of a
path or finding intersection points between paths, B\'ezier curves
are recusively reduced to smaller B\'ezier curves by splitting the
curves at the parameter value 0.5 until the parts become almost
straight. Using the notation shown in fig.~\ref{fig:beziertoline} the
straightness is expressed by a length measurement summing up the
distances $\overline{AB}=l_1$, $\overline{BC}=l_2$ and
$\overline{CD}=l_3$ and comparing this to the direct connection
$\overline{AD}$. When the difference becomes smaller than a threshold
$\epsilon$, the curve is adequately expressed by a straight line
either because the curve is almost straight or it is very short.

However, although the geometric changes are limited to distances of
$\epsilon$, the parametrization $t$ of the B\'ezier curve might be
mistakenly represented by the straight line on a much larger scale.
In the shown example, the point $X$ on the B\'ezier curve and $Y$ on
the straight line are both taken at the parameter value $t=0.5$, but
clearly are more separated from each other than one would expect from
the geometric distance of the two paths. While the parametrization on
a line is proportional to the arc length, a non-linear behaviour is
found on a B\'ezier curve. This non-linearity is originated in
considerably different lengths $l_1$, $l_2$ and $l_3$ and the mapping
of the non-linear parameter to a linear parametrization (in terms of
the arc length) can be reduced to a one-dimensional problem upon an
error $\epsilon$:
%
\begin{equation}
  x_0(1-t')+x_3t' = x_0(1-t)^3 + 3x_1t(1-t)^2 + 3x_2t^2(1-t) + x_3 t^3\,.
\end{equation}
%
In this one-dimensional approximation the parameter $t'$ performs a
linear mapping as for any straight line while $t$ represents the usual
B\'ezier curve parametrization. It now becomes a matter of expressing
$t$ by $t'$. The polynomial in $t$ to be solved is:
%
\begin{equation}
  0 = at^3+bt^2+ct+d
\end{equation}
%
with
%
\begin{align}
  a & = x_3-3x_2+3x_1-x_0 = l_1-2l_2+l_3 \\
  b & = 3x_0-6x_1+3x_2 = -3l_1+3l_2 \\
  c & = 3x_1-3x_0 = 3l_1 \\
  d & = t'(x_0-x_3) = -t'(l_1+l_2+l_3)\,.
\end{align}
%
For $0\le t'\le1$ there will be at least one solution $0\le t\le1$.
Several solutions are possible as well, although they should be close
to each other since otherwise the straight line approximation would
not be valid at all.
% >>>

\section{Relative coordinates}

% <<<
A B\'ezier curve is given by
\begin{equation}
  \vec b(t) = (1-t)^3\vec p_0 + 3t(1-t)^2\vec p_1 + 3t^2(1-t)\vec p_2 + t^3\vec p_3
\end{equation}
where $\vec p_0 = (x_0, y_0)$, $\vec p_1 = (x_1, y_1)$, $\vec p_2 =
(x_2, y_2)$, and $\vec p_3 = (x_3, y_3)$ are the control points.

When $\vec p_0$ differs from $\vec p_3$ we can express the B\'ezier
curve in relative coordinates $r(t)$ and $s(t)$ by
\begin{equation}
  \vec b(t) = \vec q + r(t)\vec r + s(t)\vec s
\end{equation}
with
\begin{align}
  \vec q & = \vec p_0\\
  \vec r & = \vec p_3 - \vec p_0 = \left(\begin{array}{c} x_3 - x_0 \\ y_3 - y_0 \end{array}\right)\\
  \vec s & = \left(\begin{array}{c} y_3 - y_0 \\ x_0 - x_3 \end{array}\right)
\end{align}

Note that
\begin{equation}
  \vec r\cdot\vec r = \vec s\cdot\vec s := l^2
\end{equation}
where $l$ is the distance between $\vec p_0$ and $\vec p_3$.

In addition $\vec r$ and $\vec s$ are perpendicular:
\begin{equation}
  \vec r\cdot\vec s = 0
\end{equation}

We can express the control points in the new coordinates:
\begin{align}
  \vec p_0 & = \vec q\\
  \vec p_1 & = \vec q + r_1\vec r + s_1\vec s\\
  \vec p_2 & = \vec q + r_2\vec r + s_2\vec s\\
  \vec p_3 & = \vec q + \vec r
\end{align}

The coefficients $r_1$, $r_2$, $s_1$, $s_2$ are given by scalar
products due to the properties of $\vec r$ and $\vec s$ given above:
\begin{align}
  r_1 l^2 & = (\vec p_1 - \vec p_0)\cdot\vec r\\
  r_2 l^2 & = (\vec p_2 - \vec p_0)\cdot\vec r\\
  s_1 l^2 & = (\vec p_1 - \vec p_0)\cdot\vec s\\
  s_2 l^2 & = (\vec p_2 - \vec p_0)\cdot\vec s
\end{align}

The parametric functions $r(t)$ and $s(t)$ become
\begin{align}
  r(t) & = 3t(1-t)^2 r_1 + 3t^2(1-t) r_2 + t^3\\
  s(t) & = 3t(1-t)^2 s_1 + 3t^2(1-t) s_2
\end{align}

\emph{Note:} Originally the idea was to use relative coordinates to
remove unstabilities in B\'ezier curves (especially cusps) considering
all points with $\dot r(t)$ being zero or extremal. This idea works
very well in general, and could, for example, also remove
self-intersections. (You can get rid of any backwards directed curve
sections, i.e. where $\dot r(t)<0$.) However, the whole idea has been
discarded as $\dot r(t)$ could be close to zero for $t=0$ and $t=1$.
The pre-removal of such problems would introduce major defects to the
B\'ezier curve (like changing the direction of the tangential vector
at the beginning and the end point).
% >>>

\section{Invalid parametrisation}

% <<<
If the derivative of the parametrisation vanishes (both coordinates) at a
parameter~$t\in[0,1]$, the parametrisation is considered to be invalid at this
point. Under which circumstances can this occur? We search for solutions~$t$ for
the quadratic equations
%
\begin{equation}
  \label{zeroderiv}
  \begin{aligned}
    0 = x(t)/3 &= t^2\bigl[(x_3-x_0) - 3(x_2-x_1)\bigr] + 2t\bigl[(x_2-x_1)-(x_1-x_0)\bigr] + (x_1-x_0) \\
    0 = y(t)/3 &= t^2\bigl[(y_3-y_0) - 3(y_2-y_1)\bigr] + 2t\bigl[(y_2-y_1)-(y_1-y_0)\bigr] + (y_1-y_0)
  \end{aligned}
\end{equation}
%
Using the usual formula for a quadratic equation $0=at^2 + bt + c$, we get the
same parameter for $x$- and $y$-coordinates, and the two inequalities from
$0\leq t\leq1$,
%
\begin{equation}
  \label{samet}
  t_{1,2} = \frac{1}{2a_x} \Bigl(-b_x \pm^1 \sqrt{b_x^2 - 4a_xc_x}\Bigr)
          = \frac{1}{2a_y} \Bigl(-b_y \pm^2 \sqrt{b_y^2 - 4a_yc_y}\Bigr)
\end{equation}
%
The two sign choices are independent of each other.

For the moment, we put aside the special cases $p_3=p_0$ and $p_1=p_0$. As
affine transformations cannot change the degeneracy of the parametrisation, we
can fix three points without loss of generality:
%
\begin{equation}
  \begin{aligned}
    (x_0, y_0) = (0, 0),\quad
    (x_1, y_1) = (0, 1),\quad
    (x_3, y_3) = (1, 0).
  \end{aligned}
\end{equation}
%
Thus, the only remaining true parameters are $(x_2, y_2)$. We will use $\Delta x
= x_2$ and $\Delta y = y_2 - 1$. Equation~\eqref{samet} now becomes
%
\begin{equation}
%   a_y \Bigl(-b_x/2 \pm^1 \sqrt{(b_x/2)^2 - a_xc_x}\Bigr)
% = a_x \Bigl(-b_y/2 \pm^2 \sqrt{(b_y/2)^2 - a_yc_y}\Bigr)
%
%   ( -3\Delta y) \Bigl(-(\Delta x  ) \pm^1 \sqrt{(\Delta x  )^2            }\Bigr)
% = (1-3\Delta x) \Bigl(-(\Delta y-1) \pm^2 \sqrt{(\Delta y-1)^2 + 3\Delta y}\Bigr)
%
 \label{samet2}
   ( -3\Delta y) \Bigl(-\Delta x  \pm^1 \sqrt{(\Delta x  )^2           }\Bigr)
 = (1-3\Delta x) \Bigl(1-\Delta y \pm^2 \sqrt{1 + \Delta y + \Delta y^2}\Bigr)
\end{equation}
%
Special care has to be taken if $a_x=0$ or $a_y=0$. For the inequalities, we
have to consider the signs of $a_x$ and $a_y$ explicitly:
\arraycolsep=0pt
%
\begin{equation}
  \begin{aligned}
  0 \leq -\Delta x \pm^1 \sqrt{\Delta x^2} \leq 1-3\Delta x &\quad\text{if $\Delta x < 1/3$ (or $a_x > 0$)} \\
  0 \leq  \Delta x \mp^1 \sqrt{\Delta x^2} \leq 3\Delta x-1 &\quad\text{if $1/3 < \Delta x$ (or $a_x < 0$)}
  \end{aligned}
\end{equation}
%
which can be reduced to
%
\begin{equation}
  \label{constr1}
  \begin{aligned}
  \text{no constraint} &\quad\text{if $\Delta x \leq 0$} \\
  \text{only the upper sign of $\pm^1$ is allowed} &\quad\text{if $0 < \Delta x < 1$} \\
  \text{no constraint} &\quad\text{if $\Delta x \geq 1$}
  \end{aligned}
\end{equation}
%
Between $0$ and $1$ the upper sign makes the inequality to be trivially
satisfied, because $-\Delta x + |\Delta x| = 0$.

The inequality constraint can equivalently be formulated for $\Delta y$,
%
\begin{equation}
  \begin{aligned}
  0 \leq 1-\Delta y \pm^2 \sqrt{1+\Delta y+\Delta y^2} \leq -3\Delta y &\quad\text{if $\Delta y < 0$ (or $a_y > 0$)} \\
  0 \leq \Delta y-1 \mp^2 \sqrt{1+\Delta y+\Delta y^2} \leq  3\Delta y &\quad\text{if $\Delta y > 0$ (or $a_y < 0$)}
  \end{aligned}
\end{equation}
%
In the first line, the comparison with~$0$ is always true. In the right
comparison, the lower sign is always possible and does not yield a constraint,
whereas the upper sign is only possible for $\Delta y \leq -1$. In the second
line, the upper sign is incompatible with the left comparison, and the lower
sign is always possible. We can reduce the conditions to
%
\begin{equation}
  \label{constr2}
  \begin{aligned}
  \text{no constraint} &\quad\text{if $\Delta y \leq -1$} \\
  \text{only the lower sign of $\pm^2$ is allowed} &\quad\text{if $\Delta y > -1$} \\
  \end{aligned}
\end{equation}
%

Equation~\eqref{samet2} with the two constraints \eqref{constr1} and
\eqref{constr2} is the system of equations that gives us the values $\Delta x,
\Delta y$ for which the parametrisation could be invalid.

First, let us check that the classic case for a cusp is well described. It has
$\Delta x=-1, \Delta y=0$. We have no constraint on $x$, and we have to take the
lower sign on $y$. Indeed, the left-hand side of eq.~\eqref{samet2} vanishes due
for the lower sign, and the right one vanishes also for the lower sign. This
case is shown among the examples in figure~\ref{fig:invalid3}.

%
\begin{figure}[ht]
  \centering
  \includegraphics{invalid2}%
  \caption{Absolute value of the difference between left- and right-hand side of
  eq.~\eqref{samet2}. The dotted lines are given by eqs.~\eqref{leftcurve} and
  \eqref{rightcurve}.}%
  \label{fig:invalid2}%
\end{figure}%
%
\begin{figure}[ht]
  \centering
  \includegraphics{invalid3}%
  \caption{Some examples of invalid parametrisations from the general
  (non-degenerate) case described by eqs.~\eqref{samet2}, \eqref{constr1},
  \eqref{constr2}.}%
  \label{fig:invalid3}%
\end{figure}%
%
Figure~\ref{fig:invalid2} shows the difference between left- and right-hand side
of Eq.~\eqref{samet2} for all valid signs, respecting the constraints. The
horizontal and vertical lines are those special cases where $a_x=0$ or $a_y=0$
and need further considerations. The zero-level curve at $\Delta x < 0$ (dotted
curve in the figure) is well described by the equation
%
\begin{equation}
  \label{leftcurve}
  \Delta x = \frac{1}{3}\Bigl(-1-2\Delta y - \sqrt{(2\Delta y+1)^2 + 3}\Bigr)
\end{equation}
%
which is obtained by taking the upper sign of $\pm^1$ in eq.~\eqref{samet2}:
With negative values of $\Delta x$ the left-hand side becomes $6\Delta x\Delta
y$. Isolating the square-root and then taking the square leads to a quadratic
equation for $\Delta x$, of which eq.~\eqref{leftcurve} is the negative
solution. A numerical check shows that this solution corresponds to the lower
sign of $\pm^2$ and has thus no restriction in $\Delta y$. The second solution
(dotted curve in the figure for $\Delta x>0$) of the mentioned quadratic
equation,
%
\begin{equation}
  \label{rightcurve}
  \Delta x = \frac{1}{3}\Bigl(-1-2\Delta y + \sqrt{(2\Delta y+1)^2 + 3}\Bigr)
\end{equation}
%
corresponds to the upper sign of $\pm^2$ and is thus subject to the constraint
\hbox{$\Delta y \leq -1$}.

Apart from the general cases on the two curves, we must treat some special cases
separately:
%
\begin{itemize}
\item $a_y=0$: This appears as a zero-level line in figure~\ref{fig:invalid2},
    but this is an artefact coming from both sides of eq.~\eqref{samet2} being
    zero. We have to go back to the original set of
    equations~\eqref{zeroderiv}: We have in the lower line $\Delta y=0$, thus
    $t=1/2$. Going back to the upper line with this value, we obtain $\Delta
    x=-1$. This parameter point is already covered by the general treatment.
\item $a_x=0$: This implies $\Delta x=1/3$, and the upper line gives $t=0$.
    This, however, contradicts the lower line. We do not get an invalid
    parametrisation point from $a_x=0$.
\item $p_1=p_0$: This is either an even more degenerate case (see below), or it
    can be mapped to the reverse situation of $\Delta x=1, \Delta y=-1$ which
    was $p_2=p_3$.
\item $p_1=p_0$ and $p_2=p_3$: This is a line.
\item $p_3=p_0$: There are invalid parametrisation points if all four
    $p_0,p_1,p_2,p_3$ are collinear. Depending on the sign of
    $(p_1-p_0)\cdot(p_3-p_2)$ there are one or two invalid points.
\item $p_1=p_0=p_2=p_3$: This is a point.
\end{itemize}
%
% >>>

\section{Self-intersections}

% <<<
In order to determine the control points which lead to self-intersections, we
could analyse the set of equations
%
\begin{equation}
    x(t_1) = x(t_2)\quad\text{and}\quad
    y(t_1) = y(t_2) \quad\text{for}\quad t_1\neq t_2.
\end{equation}
%
To solve the problem, we could express the solutions $t(\Delta x, \bar x)$ of
the cubic equation $\bar x = x(t)$, test their number via Cardano's equation,
and, if they are more than one, use a pair of them in the $y$-equation to see
whether we get two times the same $y$-value. This would be a formidable task.

We here take a different route. As for the invalid parametrisation above, we
exclude some degenerate cases and use affine transformations, such that only the
parameters $\Delta x=x_2$ and $\Delta y=y_2-1$ are left. It is geometrically
evident that a little left and right of the two relevant curves in
figure~\ref{fig:invalid2} we must have different situations as far as
self-intersections are concerned. Either we find one a little left or a little
right of the curves, and none on the respective other side. Further, a
self-intersection can clear away when parameters change such that the curve
passes through one of its endpoints. These two conditions boil down to the phase
diagram in figure~\ref{fig:selfinter2}. In the gray shaded areas,
self-intersections are possible.
%
\begin{figure}[t]
  \includegraphics{selfinter2}%
  \caption{Self-intersections are possible in the gray-shaded areas. The black,
  red, green, blue curves are from eqs.~\eqref{leftcurve}, \eqref{rightcurve},
  \eqref{pass00}, \eqref{pass10}, respectively.}%
  \label{fig:selfinter2}%
\end{figure}
%

We first calculate the parameters $0<t<t$ for which the curve passes through
$(0,0)$. The $x$-coordinate leads to $t=3\Delta x/(3\Delta x - 1)$, and the
$y$-coordinate to $t=-1/\Delta y$. From the latter we know that again $\Delta
y\leq 1$. Setting both parameters equal allows to express $\Delta x(\Delta y)$
or inverse,
%
\begin{align}
  \label{pass00}
  \Delta x &= \frac{1}{3(\Delta y+1)} \\
  \Delta y &= \frac{1-3\Delta x}{3\Delta x}
\end{align}
%

The calculation for passing through $(1,0)$ is a little more complicated, since
the cubic equation for $x$ (which had a double root at $t=0$ before) now reads
$0 = 3\Delta xt^2(1-t) + t^3 - 1$. The equation for~$y$ has not changed and
leads to the same solution with the same constraint. Using $t=-1/\Delta y$ in
the cubic equation for $x$ leads us to
%
\begin{align}
  \label{pass10}
  \Delta x &= \frac{1+\Delta y^3}{3(\Delta y+1)}.
\end{align}
%
% >>>

\section{Removing cusps}

A cusp is a point on a B\'ezier curve $\vec b(t)$, where
$\mathrm{d}\vec b(t)/\mathrm{d}t=\dot{\vec b}(t)$ vanishs.
For stability we don't want it to be almost zero either.
For comparison, a straight line
$\vec l(t)=\vec p_0 + (\vec p_3-\vec p_0)t$ has the constant derivative
$\mathrm{d}\vec l(t)/\mathrm{d}t = \dot{\vec l}(t) = \vec p_3-\vec p_0$.
As lines shorter than $\epsilon$ are forbidden, we have
$|\dot{\vec l}(t)| \ge \epsilon$. We want to enforce
this limit to B\'ezier curves as well, \emph{i.e.}
$|\dot{\vec b}(t)| \ge \epsilon$.

First we have to take into account the beginning ($t=0$) and end point
($t=1$) of the B\'ezier curve. Here, the derivates are given by
$\dot{\vec b}(0) = 3(\vec p_1-\vec p_0)$ and
$\dot{\vec b}(1) = 3(\vec p_3-\vec p_2)$. In case the absolute value
of the derivatives are smaller than $\epsilon$, we need to shift
$\vec p_1$ and $\vec p_2$, respectively. For $\vec p_1$ a new value is
choosen in the direction of $\vec p_2$ with respect to $\vec p_0$ if
$\vec p_2$ is more distant than $\epsilon/3$, otherwise the direction
of $\vec p_3$ is used. The distance of the new point is choosen such
that the absolute value of the derivate becomes $\epsilon$. $\vec p_2$
is shifted similarly using the unshifted position for $\vec p_1$.

Once the derivatives at the boundary fulfil the requirement, we need
to search for minimal values of the absolute value (or the square) of
the derivate within the valid parameter range. If the absolute value
is smaller at an extrema, the curve is split at that point.
\end{document}

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