lines 6-66 of file: xrst/theory/sin_cos_forward.xrst {xrst_begin sin_cos_forward} Trigonometric and Hyperbolic Sine and Cosine Forward Theory ########################################################### Differential Equation ********************* The :ref:`standard math function differential equation` is .. math:: B(u) * F^{(1)} (u) - A(u) * F (u) = D(u) In this sections we consider forward mode for the following choices: .. csv-table:: :widths: auto ,,:math:`F(u)`,,:math:`\sin(u)`,,:math:`\cos(u)`,,:math:`\sinh(u)`,,:math:`\cosh(u)` ,,:math:`A(u)`,,:math:`0`,,:math:`0`,,:math:`0`,,:math:`0` ,,:math:`B(u)`,,:math:`1`,,:math:`1`,,:math:`1`,,:math:`1` ,,:math:`D(u)`,,:math:`\cos(u)`,,:math:`- \sin(u)`,,:math:`\cosh(u)`,,:math:`\sinh(u)` We use :math:`a`, :math:`b`, :math:`d` and :math:`f` for the Taylor coefficients of :math:`A [ X (t) ]`, :math:`B [ X (t) ]`, :math:`D [ X (t) ]`, and :math:`F [ X(t) ]` respectively. It now follows from the general :ref:`forward_theory@Standard Math Functions@Taylor Coefficients Recursion Formula` that for :math:`j = 0 , 1, \ldots`, .. math:: :nowrap: \begin{eqnarray} f^{(0)} & = & D ( x^{(0)} ) \\ e^{(j)} & = & d^{(j)} + \sum_{k=0}^{j} a^{(j-k)} * f^{(k)} \\ & = & d^{(j)} \\ f^{(j+1)} & = & \frac{1}{j+1} \frac{1}{ b^{(0)} } \left( \sum_{k=1}^{j+1} k x^{(k)} e^{(j+1-k)} - \sum_{k=1}^j k f^{(k)} b^{(j+1-k)} \right) \\ & = & \frac{1}{j+1} \sum_{k=1}^{j+1} k x^{(k)} d^{(j+1-k)} \end{eqnarray} The formula above generates the order :math:`j+1` coefficient of :math:`F[ X(t) ]` from the lower order coefficients for :math:`X(t)` and :math:`D[ X(t) ]`. {xrst_end sin_cos_forward}