| Alternative 1 |
|---|
| Accuracy | 98.3% |
|---|
| Cost | 59360 |
|---|
\[\begin{array}{l}
t_0 := \tan^{-1} \left(\frac{alphay}{alphax} \cdot \tan \left(\pi \cdot \left(2 \cdot u1 + 0.5\right)\right)\right)\\
t_1 := \frac{\cos t_0}{alphax}\\
\frac{1}{\sqrt{1 + \frac{u0}{\left(1 - u0\right) \cdot \mathsf{fma}\left(t_1, t_1, \sin t_0 \cdot \frac{\sin \tan^{-1} \left(\frac{alphay}{alphax} \cdot \tan \left(\pi \cdot 0.5\right)\right)}{alphay \cdot alphay}\right)}}}
\end{array}
\]
| Alternative 2 |
|---|
| Accuracy | 97.9% |
|---|
| Cost | 56256 |
|---|
\[\begin{array}{l}
t_0 := \tan^{-1} \left(\frac{alphay}{alphax} \cdot \tan \left(\pi \cdot \left(2 \cdot u1 + 0.5\right)\right)\right)\\
t_1 := \sin t_0\\
\frac{1}{\sqrt{1 + \frac{u0}{\left(1 - u0\right) \cdot \mathsf{fma}\left(\frac{\cos t_0}{alphax}, \frac{\frac{1}{\mathsf{hypot}\left(1, \frac{alphay}{alphax} \cdot \tan \left(\pi \cdot 0.5\right)\right)}}{alphax}, t_1 \cdot \frac{t_1}{alphay \cdot alphay}\right)}}}
\end{array}
\]
| Alternative 3 |
|---|
| Accuracy | 97.7% |
|---|
| Cost | 52992 |
|---|
\[\begin{array}{l}
t_0 := \sin \tan^{-1} \left(\frac{alphay}{alphax} \cdot \tan \left(\pi \cdot \left(2 \cdot u1 + 0.5\right)\right)\right)\\
\frac{1}{\sqrt{1 + \frac{u0}{\left(1 - u0\right) \cdot \mathsf{fma}\left(\frac{\frac{1}{\mathsf{hypot}\left(1, \frac{alphay}{alphax} \cdot \tan \left(\pi \cdot 0.5\right)\right)}}{alphax}, \frac{\cos \tan^{-1} \left(\frac{alphay}{\frac{\frac{\frac{alphax}{u1}}{\pi}}{2}}\right)}{alphax}, t_0 \cdot \frac{t_0}{alphay \cdot alphay}\right)}}}
\end{array}
\]
| Alternative 4 |
|---|
| Accuracy | 92.6% |
|---|
| Cost | 52960 |
|---|
\[\begin{array}{l}
t_0 := \sin \tan^{-1} \left(\frac{alphay}{alphax} \cdot \tan \left(\pi \cdot \left(2 \cdot u1 + 0.5\right)\right)\right)\\
t_1 := \frac{\cos \tan^{-1} \left(\frac{alphay}{\frac{\frac{\frac{alphax}{u1}}{\pi}}{2}}\right)}{alphax}\\
\frac{1}{\sqrt{1 + \frac{u0}{\left(1 - u0\right) \cdot \mathsf{fma}\left(t_1, t_1, t_0 \cdot \frac{t_0}{alphay \cdot alphay}\right)}}}
\end{array}
\]