\[\left|\left(ew \cdot \sin t\right) \cdot \cos \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right) + \left(eh \cdot \cos t\right) \cdot \sin \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)\right|
\]
↓
\[\begin{array}{l}
t_1 := \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)\\
\left|\cos t_1 \cdot \left(ew \cdot \sin t\right) + \sin t_1 \cdot \left(eh \cdot \cos t\right)\right|
\end{array}
\]
(FPCore (eh ew t)
:precision binary64
(fabs
(+
(* (* ew (sin t)) (cos (atan (/ (/ eh ew) (tan t)))))
(* (* eh (cos t)) (sin (atan (/ (/ eh ew) (tan t))))))))
↓
(FPCore (eh ew t)
:precision binary64
(let* ((t_1 (atan (/ (/ eh ew) (tan t)))))
(fabs (+ (* (cos t_1) (* ew (sin t))) (* (sin t_1) (* eh (cos t)))))))
double code(double eh, double ew, double t) {
return fabs((((ew * sin(t)) * cos(atan(((eh / ew) / tan(t))))) + ((eh * cos(t)) * sin(atan(((eh / ew) / tan(t)))))));
}
↓
double code(double eh, double ew, double t) {
double t_1 = atan(((eh / ew) / tan(t)));
return fabs(((cos(t_1) * (ew * sin(t))) + (sin(t_1) * (eh * cos(t)))));
}
real(8) function code(eh, ew, t)
real(8), intent (in) :: eh
real(8), intent (in) :: ew
real(8), intent (in) :: t
code = abs((((ew * sin(t)) * cos(atan(((eh / ew) / tan(t))))) + ((eh * cos(t)) * sin(atan(((eh / ew) / tan(t)))))))
end function
↓
real(8) function code(eh, ew, t)
real(8), intent (in) :: eh
real(8), intent (in) :: ew
real(8), intent (in) :: t
real(8) :: t_1
t_1 = atan(((eh / ew) / tan(t)))
code = abs(((cos(t_1) * (ew * sin(t))) + (sin(t_1) * (eh * cos(t)))))
end function
public static double code(double eh, double ew, double t) {
return Math.abs((((ew * Math.sin(t)) * Math.cos(Math.atan(((eh / ew) / Math.tan(t))))) + ((eh * Math.cos(t)) * Math.sin(Math.atan(((eh / ew) / Math.tan(t)))))));
}
↓
public static double code(double eh, double ew, double t) {
double t_1 = Math.atan(((eh / ew) / Math.tan(t)));
return Math.abs(((Math.cos(t_1) * (ew * Math.sin(t))) + (Math.sin(t_1) * (eh * Math.cos(t)))));
}
def code(eh, ew, t):
return math.fabs((((ew * math.sin(t)) * math.cos(math.atan(((eh / ew) / math.tan(t))))) + ((eh * math.cos(t)) * math.sin(math.atan(((eh / ew) / math.tan(t)))))))
↓
def code(eh, ew, t):
t_1 = math.atan(((eh / ew) / math.tan(t)))
return math.fabs(((math.cos(t_1) * (ew * math.sin(t))) + (math.sin(t_1) * (eh * math.cos(t)))))
function code(eh, ew, t)
return abs(Float64(Float64(Float64(ew * sin(t)) * cos(atan(Float64(Float64(eh / ew) / tan(t))))) + Float64(Float64(eh * cos(t)) * sin(atan(Float64(Float64(eh / ew) / tan(t)))))))
end
↓
function code(eh, ew, t)
t_1 = atan(Float64(Float64(eh / ew) / tan(t)))
return abs(Float64(Float64(cos(t_1) * Float64(ew * sin(t))) + Float64(sin(t_1) * Float64(eh * cos(t)))))
end
function tmp = code(eh, ew, t)
tmp = abs((((ew * sin(t)) * cos(atan(((eh / ew) / tan(t))))) + ((eh * cos(t)) * sin(atan(((eh / ew) / tan(t)))))));
end
↓
function tmp = code(eh, ew, t)
t_1 = atan(((eh / ew) / tan(t)));
tmp = abs(((cos(t_1) * (ew * sin(t))) + (sin(t_1) * (eh * cos(t)))));
end
code[eh_, ew_, t_] := N[Abs[N[(N[(N[(ew * N[Sin[t], $MachinePrecision]), $MachinePrecision] * N[Cos[N[ArcTan[N[(N[(eh / ew), $MachinePrecision] / N[Tan[t], $MachinePrecision]), $MachinePrecision]], $MachinePrecision]], $MachinePrecision]), $MachinePrecision] + N[(N[(eh * N[Cos[t], $MachinePrecision]), $MachinePrecision] * N[Sin[N[ArcTan[N[(N[(eh / ew), $MachinePrecision] / N[Tan[t], $MachinePrecision]), $MachinePrecision]], $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]
↓
code[eh_, ew_, t_] := Block[{t$95$1 = N[ArcTan[N[(N[(eh / ew), $MachinePrecision] / N[Tan[t], $MachinePrecision]), $MachinePrecision]], $MachinePrecision]}, N[Abs[N[(N[(N[Cos[t$95$1], $MachinePrecision] * N[(ew * N[Sin[t], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] + N[(N[Sin[t$95$1], $MachinePrecision] * N[(eh * N[Cos[t], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]]
\left|\left(ew \cdot \sin t\right) \cdot \cos \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right) + \left(eh \cdot \cos t\right) \cdot \sin \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)\right|
↓
\begin{array}{l}
t_1 := \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)\\
\left|\cos t_1 \cdot \left(ew \cdot \sin t\right) + \sin t_1 \cdot \left(eh \cdot \cos t\right)\right|
\end{array}
Alternatives
| Alternative 1 |
|---|
| Error | 0.2 |
|---|
| Cost | 52480 |
|---|
\[\left|\sin \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right) \cdot \left(eh \cdot \cos t\right) + \frac{ew}{\frac{\mathsf{hypot}\left(1, \frac{eh}{ew \cdot \tan t}\right)}{\sin t}}\right|
\]
| Alternative 2 |
|---|
| Error | 0.5 |
|---|
| Cost | 52416 |
|---|
\[\left|\sin \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right) \cdot \left(eh \cdot \cos t\right) + \cos \tan^{-1} \left(\frac{\frac{eh}{t}}{ew}\right) \cdot \left(ew \cdot \sin t\right)\right|
\]
| Alternative 3 |
|---|
| Error | 0.6 |
|---|
| Cost | 46080 |
|---|
\[\left|\sin \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right) \cdot \left(eh \cdot \cos t\right) + \frac{ew}{\frac{\mathsf{hypot}\left(1, \frac{eh}{ew \cdot t}\right)}{\sin t}}\right|
\]
| Alternative 4 |
|---|
| Error | 0.9 |
|---|
| Cost | 39232 |
|---|
\[\left|\sin \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right) \cdot \left(eh \cdot \cos t\right) + ew \cdot \sin t\right|
\]
| Alternative 5 |
|---|
| Error | 11.0 |
|---|
| Cost | 33096 |
|---|
\[\begin{array}{l}
t_1 := ew \cdot \sin t\\
\mathbf{if}\;ew \leq -4.5 \cdot 10^{-117}:\\
\;\;\;\;\left|eh + \cos \tan^{-1} \left(\frac{\frac{eh}{t}}{ew}\right) \cdot t_1\right|\\
\mathbf{elif}\;ew \leq 2.4 \cdot 10^{-199}:\\
\;\;\;\;\left|\sin \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right) \cdot \left(eh \cdot \cos t\right) + ew \cdot t\right|\\
\mathbf{else}:\\
\;\;\;\;\left|t_1 + eh \cdot \sin \tan^{-1} \left(\frac{eh}{ew \cdot \tan t}\right)\right|\\
\end{array}
\]
| Alternative 6 |
|---|
| Error | 11.1 |
|---|
| Cost | 32968 |
|---|
\[\begin{array}{l}
t_1 := ew \cdot \sin t\\
t_2 := \tan^{-1} \left(\frac{\frac{eh}{t}}{ew}\right)\\
\mathbf{if}\;ew \leq -9.5 \cdot 10^{-117}:\\
\;\;\;\;\left|eh + \cos t_2 \cdot t_1\right|\\
\mathbf{elif}\;ew \leq 4.4 \cdot 10^{-199}:\\
\;\;\;\;\left|\frac{t}{\frac{\frac{eh}{ew \cdot ew}}{t}} + \left(eh \cdot \cos t\right) \cdot \sin t_2\right|\\
\mathbf{else}:\\
\;\;\;\;\left|t_1 + eh \cdot \sin \tan^{-1} \left(\frac{eh}{ew \cdot \tan t}\right)\right|\\
\end{array}
\]
| Alternative 7 |
|---|
| Error | 1.1 |
|---|
| Cost | 32832 |
|---|
\[\left|\cos \tan^{-1} \left(\frac{\frac{eh}{t}}{ew}\right) \cdot \left(ew \cdot \sin t\right) + eh \cdot \cos t\right|
\]
| Alternative 8 |
|---|
| Error | 1.1 |
|---|
| Cost | 32832 |
|---|
\[\left|\cos \tan^{-1} \left(\frac{\frac{eh}{t}}{ew}\right) \cdot \left(ew \cdot \sin t\right) - eh \cdot \cos t\right|
\]
| Alternative 9 |
|---|
| Error | 13.4 |
|---|
| Cost | 27081 |
|---|
\[\begin{array}{l}
t_1 := \tan^{-1} \left(\frac{\frac{eh}{t}}{ew}\right)\\
\mathbf{if}\;ew \leq -2.3 \cdot 10^{-117} \lor \neg \left(ew \leq 3.75 \cdot 10^{-202}\right):\\
\;\;\;\;\left|eh + \cos t_1 \cdot \left(ew \cdot \sin t\right)\right|\\
\mathbf{else}:\\
\;\;\;\;\left|\left(eh \cdot \cos t\right) \cdot \sin t_1 + \left(ew \cdot ew\right) \cdot \frac{t \cdot t}{eh}\right|\\
\end{array}
\]
| Alternative 10 |
|---|
| Error | 11.2 |
|---|
| Cost | 27081 |
|---|
\[\begin{array}{l}
t_1 := \tan^{-1} \left(\frac{\frac{eh}{t}}{ew}\right)\\
\mathbf{if}\;ew \leq -1.75 \cdot 10^{-116} \lor \neg \left(ew \leq 5.1 \cdot 10^{-199}\right):\\
\;\;\;\;\left|eh + \cos t_1 \cdot \left(ew \cdot \sin t\right)\right|\\
\mathbf{else}:\\
\;\;\;\;\left|\frac{t}{\frac{\frac{eh}{ew \cdot ew}}{t}} + \left(eh \cdot \cos t\right) \cdot \sin t_1\right|\\
\end{array}
\]
| Alternative 11 |
|---|
| Error | 13.7 |
|---|
| Cost | 26304 |
|---|
\[\left|eh + \cos \tan^{-1} \left(\frac{\frac{eh}{t}}{ew}\right) \cdot \left(ew \cdot \sin t\right)\right|
\]
| Alternative 12 |
|---|
| Error | 42.8 |
|---|
| Cost | 20288 |
|---|
\[\left|\left(ew \cdot ew\right) \cdot \frac{t \cdot t}{eh} + eh \cdot \sin \tan^{-1} \left(\frac{\frac{eh}{t}}{ew}\right)\right|
\]