Example from Robby

Percentage Accurate: 99.8% → 99.8%

Time: 12.7s

Alternatives: 12

Speedup: 1.2×

Specification

Math

\[\begin{array}{l} \\ \begin{array}{l} t_1 := \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)\\ \left|\left(ew \cdot \sin t\right) \cdot \cos t\_1 + \left(eh \cdot \cos t\right) \cdot \sin t\_1\right| \end{array} \end{array} \]

FPCore

(FPCore (eh ew t)
 :precision binary64
 (let* ((t_1 (atan (/ (/ eh ew) (tan t)))))
   (fabs (+ (* (* ew (sin t)) (cos t_1)) (* (* eh (cos t)) (sin t_1))))))

C

double code(double eh, double ew, double t) {
	double t_1 = atan(((eh / ew) / tan(t)));
	return fabs((((ew * sin(t)) * cos(t_1)) + ((eh * cos(t)) * sin(t_1))));
}

Fortran

module fmin_fmax_functions
    implicit none
    private
    public fmax
    public fmin

    interface fmax
        module procedure fmax88
        module procedure fmax44
        module procedure fmax84
        module procedure fmax48
    end interface
    interface fmin
        module procedure fmin88
        module procedure fmin44
        module procedure fmin84
        module procedure fmin48
    end interface
contains
    real(8) function fmax88(x, y) result (res)
        real(8), intent (in) :: x
        real(8), intent (in) :: y
        res = merge(y, merge(x, max(x, y), y /= y), x /= x)
    end function
    real(4) function fmax44(x, y) result (res)
        real(4), intent (in) :: x
        real(4), intent (in) :: y
        res = merge(y, merge(x, max(x, y), y /= y), x /= x)
    end function
    real(8) function fmax84(x, y) result(res)
        real(8), intent (in) :: x
        real(4), intent (in) :: y
        res = merge(dble(y), merge(x, max(x, dble(y)), y /= y), x /= x)
    end function
    real(8) function fmax48(x, y) result(res)
        real(4), intent (in) :: x
        real(8), intent (in) :: y
        res = merge(y, merge(dble(x), max(dble(x), y), y /= y), x /= x)
    end function
    real(8) function fmin88(x, y) result (res)
        real(8), intent (in) :: x
        real(8), intent (in) :: y
        res = merge(y, merge(x, min(x, y), y /= y), x /= x)
    end function
    real(4) function fmin44(x, y) result (res)
        real(4), intent (in) :: x
        real(4), intent (in) :: y
        res = merge(y, merge(x, min(x, y), y /= y), x /= x)
    end function
    real(8) function fmin84(x, y) result(res)
        real(8), intent (in) :: x
        real(4), intent (in) :: y
        res = merge(dble(y), merge(x, min(x, dble(y)), y /= y), x /= x)
    end function
    real(8) function fmin48(x, y) result(res)
        real(4), intent (in) :: x
        real(8), intent (in) :: y
        res = merge(y, merge(dble(x), min(dble(x), y), y /= y), x /= x)
    end function
end module

real(8) function code(eh, ew, t)
use fmin_fmax_functions
    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((((ew * sin(t)) * cos(t_1)) + ((eh * cos(t)) * sin(t_1))))
end function

Java

public static double code(double eh, double ew, double t) {
	double t_1 = Math.atan(((eh / ew) / Math.tan(t)));
	return Math.abs((((ew * Math.sin(t)) * Math.cos(t_1)) + ((eh * Math.cos(t)) * Math.sin(t_1))));
}

Python

def code(eh, ew, t):
	t_1 = math.atan(((eh / ew) / math.tan(t)))
	return math.fabs((((ew * math.sin(t)) * math.cos(t_1)) + ((eh * math.cos(t)) * math.sin(t_1))))

Julia

function code(eh, ew, t)
	t_1 = atan(Float64(Float64(eh / ew) / tan(t)))
	return abs(Float64(Float64(Float64(ew * sin(t)) * cos(t_1)) + Float64(Float64(eh * cos(t)) * sin(t_1))))
end

MATLAB

function tmp = code(eh, ew, t)
	t_1 = atan(((eh / ew) / tan(t)));
	tmp = abs((((ew * sin(t)) * cos(t_1)) + ((eh * cos(t)) * sin(t_1))));
end

Wolfram

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[(ew * N[Sin[t], $MachinePrecision]), $MachinePrecision] * N[Cos[t$95$1], $MachinePrecision]), $MachinePrecision] + N[(N[(eh * N[Cos[t], $MachinePrecision]), $MachinePrecision] * N[Sin[t$95$1], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]]

Initial Program: 99.8% accurate, 1.0× speedup

Math

\[\begin{array}{l} \\ \begin{array}{l} t_1 := \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)\\ \left|\left(ew \cdot \sin t\right) \cdot \cos t\_1 + \left(eh \cdot \cos t\right) \cdot \sin t\_1\right| \end{array} \end{array} \]

FPCore

(FPCore (eh ew t)
 :precision binary64
 (let* ((t_1 (atan (/ (/ eh ew) (tan t)))))
   (fabs (+ (* (* ew (sin t)) (cos t_1)) (* (* eh (cos t)) (sin t_1))))))

C

double code(double eh, double ew, double t) {
	double t_1 = atan(((eh / ew) / tan(t)));
	return fabs((((ew * sin(t)) * cos(t_1)) + ((eh * cos(t)) * sin(t_1))));
}

Fortran

module fmin_fmax_functions
    implicit none
    private
    public fmax
    public fmin

    interface fmax
        module procedure fmax88
        module procedure fmax44
        module procedure fmax84
        module procedure fmax48
    end interface
    interface fmin
        module procedure fmin88
        module procedure fmin44
        module procedure fmin84
        module procedure fmin48
    end interface
contains
    real(8) function fmax88(x, y) result (res)
        real(8), intent (in) :: x
        real(8), intent (in) :: y
        res = merge(y, merge(x, max(x, y), y /= y), x /= x)
    end function
    real(4) function fmax44(x, y) result (res)
        real(4), intent (in) :: x
        real(4), intent (in) :: y
        res = merge(y, merge(x, max(x, y), y /= y), x /= x)
    end function
    real(8) function fmax84(x, y) result(res)
        real(8), intent (in) :: x
        real(4), intent (in) :: y
        res = merge(dble(y), merge(x, max(x, dble(y)), y /= y), x /= x)
    end function
    real(8) function fmax48(x, y) result(res)
        real(4), intent (in) :: x
        real(8), intent (in) :: y
        res = merge(y, merge(dble(x), max(dble(x), y), y /= y), x /= x)
    end function
    real(8) function fmin88(x, y) result (res)
        real(8), intent (in) :: x
        real(8), intent (in) :: y
        res = merge(y, merge(x, min(x, y), y /= y), x /= x)
    end function
    real(4) function fmin44(x, y) result (res)
        real(4), intent (in) :: x
        real(4), intent (in) :: y
        res = merge(y, merge(x, min(x, y), y /= y), x /= x)
    end function
    real(8) function fmin84(x, y) result(res)
        real(8), intent (in) :: x
        real(4), intent (in) :: y
        res = merge(dble(y), merge(x, min(x, dble(y)), y /= y), x /= x)
    end function
    real(8) function fmin48(x, y) result(res)
        real(4), intent (in) :: x
        real(8), intent (in) :: y
        res = merge(y, merge(dble(x), min(dble(x), y), y /= y), x /= x)
    end function
end module

real(8) function code(eh, ew, t)
use fmin_fmax_functions
    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((((ew * sin(t)) * cos(t_1)) + ((eh * cos(t)) * sin(t_1))))
end function

Java

public static double code(double eh, double ew, double t) {
	double t_1 = Math.atan(((eh / ew) / Math.tan(t)));
	return Math.abs((((ew * Math.sin(t)) * Math.cos(t_1)) + ((eh * Math.cos(t)) * Math.sin(t_1))));
}

Python

def code(eh, ew, t):
	t_1 = math.atan(((eh / ew) / math.tan(t)))
	return math.fabs((((ew * math.sin(t)) * math.cos(t_1)) + ((eh * math.cos(t)) * math.sin(t_1))))

Julia

function code(eh, ew, t)
	t_1 = atan(Float64(Float64(eh / ew) / tan(t)))
	return abs(Float64(Float64(Float64(ew * sin(t)) * cos(t_1)) + Float64(Float64(eh * cos(t)) * sin(t_1))))
end

MATLAB

function tmp = code(eh, ew, t)
	t_1 = atan(((eh / ew) / tan(t)));
	tmp = abs((((ew * sin(t)) * cos(t_1)) + ((eh * cos(t)) * sin(t_1))));
end

Wolfram

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[(ew * N[Sin[t], $MachinePrecision]), $MachinePrecision] * N[Cos[t$95$1], $MachinePrecision]), $MachinePrecision] + N[(N[(eh * N[Cos[t], $MachinePrecision]), $MachinePrecision] * N[Sin[t$95$1], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]]

Alternative 1: 99.8% accurate, 1.2× speedup

Math

\[\begin{array}{l} \\ \begin{array}{l} t_1 := \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right)\\ \left|\mathsf{fma}\left(\frac{\sin t}{\cosh t\_1}, ew, \tanh t\_1 \cdot \left(\cos t \cdot eh\right)\right)\right| \end{array} \end{array} \]

FPCore

(FPCore (eh ew t)
 :precision binary64
 (let* ((t_1 (asinh (/ eh (* (tan t) ew)))))
   (fabs (fma (/ (sin t) (cosh t_1)) ew (* (tanh t_1) (* (cos t) eh))))))

C

double code(double eh, double ew, double t) {
	double t_1 = asinh((eh / (tan(t) * ew)));
	return fabs(fma((sin(t) / cosh(t_1)), ew, (tanh(t_1) * (cos(t) * eh))));
}

Julia

function code(eh, ew, t)
	t_1 = asinh(Float64(eh / Float64(tan(t) * ew)))
	return abs(fma(Float64(sin(t) / cosh(t_1)), ew, Float64(tanh(t_1) * Float64(cos(t) * eh))))
end

Wolfram

code[eh_, ew_, t_] := Block[{t$95$1 = N[ArcSinh[N[(eh / N[(N[Tan[t], $MachinePrecision] * ew), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]}, N[Abs[N[(N[(N[Sin[t], $MachinePrecision] / N[Cosh[t$95$1], $MachinePrecision]), $MachinePrecision] * ew + N[(N[Tanh[t$95$1], $MachinePrecision] * N[(N[Cos[t], $MachinePrecision] * eh), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]]

Derivation

1. Initial program 99.8%

   \[\left|\left(ew \cdot \sin t\right) \cdot \cos \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right) + \left(eh \cdot \cos t\right) \cdot \sin \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)\right| \]

3. Applied rewrites 99.8%

   \[\leadsto \left|\color{blue}{\mathsf{fma}\left(\frac{\sin t}{\cosh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right)}, ew, \tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot \left(\cos t \cdot eh\right)\right)}\right| \]
4. Add Preprocessing

Alternative 2: 98.7% accurate, 1.8× speedup

Math

\[\begin{array}{l} \\ \left|\mathsf{fma}\left(\sin t, ew, \tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot \left(\cos t \cdot eh\right)\right)\right| \end{array} \]

FPCore

(FPCore (eh ew t)
 :precision binary64
 (fabs
  (fma (sin t) ew (* (tanh (asinh (/ eh (* (tan t) ew)))) (* (cos t) eh)))))

C

double code(double eh, double ew, double t) {
	return fabs(fma(sin(t), ew, (tanh(asinh((eh / (tan(t) * ew)))) * (cos(t) * eh))));
}

Julia

function code(eh, ew, t)
	return abs(fma(sin(t), ew, Float64(tanh(asinh(Float64(eh / Float64(tan(t) * ew)))) * Float64(cos(t) * eh))))
end

Wolfram

code[eh_, ew_, t_] := N[Abs[N[(N[Sin[t], $MachinePrecision] * ew + N[(N[Tanh[N[ArcSinh[N[(eh / N[(N[Tan[t], $MachinePrecision] * ew), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]], $MachinePrecision] * N[(N[Cos[t], $MachinePrecision] * eh), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]

Derivation

1. Initial program 99.8%

   \[\left|\left(ew \cdot \sin t\right) \cdot \cos \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right) + \left(eh \cdot \cos t\right) \cdot \sin \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)\right| \]

3. Applied rewrites 99.8%

   \[\leadsto \left|\color{blue}{\mathsf{fma}\left(\frac{\sin t}{\cosh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right)}, ew, \tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot \left(\cos t \cdot eh\right)\right)}\right| \]

4. Taylor expanded in eh around 0

   \[\leadsto \left|\mathsf{fma}\left(\color{blue}{\sin t}, ew, \tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot \left(\cos t \cdot eh\right)\right)\right| \]
5. Step-by-step derivation

   1. lower-sin.f64 98.7

      \[\leadsto \left|\mathsf{fma}\left(\sin t, ew, \tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot \left(\cos t \cdot eh\right)\right)\right| \]

6. Applied rewrites 98.7%

   \[\leadsto \left|\mathsf{fma}\left(\color{blue}{\sin t}, ew, \tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot \left(\cos t \cdot eh\right)\right)\right| \]
7. Add Preprocessing

Alternative 3: 89.9% accurate, 1.9× speedup

Math

\[\begin{array}{l} \\ \begin{array}{l} t_1 := \sinh^{-1} \left(\frac{eh}{ew \cdot t}\right)\\ \left|\mathsf{fma}\left(\frac{\sin t}{\cosh t\_1}, ew, \tanh t\_1 \cdot \left(\cos t \cdot eh\right)\right)\right| \end{array} \end{array} \]

FPCore

(FPCore (eh ew t)
 :precision binary64
 (let* ((t_1 (asinh (/ eh (* ew t)))))
   (fabs (fma (/ (sin t) (cosh t_1)) ew (* (tanh t_1) (* (cos t) eh))))))

C

double code(double eh, double ew, double t) {
	double t_1 = asinh((eh / (ew * t)));
	return fabs(fma((sin(t) / cosh(t_1)), ew, (tanh(t_1) * (cos(t) * eh))));
}

Julia

function code(eh, ew, t)
	t_1 = asinh(Float64(eh / Float64(ew * t)))
	return abs(fma(Float64(sin(t) / cosh(t_1)), ew, Float64(tanh(t_1) * Float64(cos(t) * eh))))
end

Wolfram

code[eh_, ew_, t_] := Block[{t$95$1 = N[ArcSinh[N[(eh / N[(ew * t), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]}, N[Abs[N[(N[(N[Sin[t], $MachinePrecision] / N[Cosh[t$95$1], $MachinePrecision]), $MachinePrecision] * ew + N[(N[Tanh[t$95$1], $MachinePrecision] * N[(N[Cos[t], $MachinePrecision] * eh), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]]

Derivation

1. Initial program 99.8%

   \[\left|\left(ew \cdot \sin t\right) \cdot \cos \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right) + \left(eh \cdot \cos t\right) \cdot \sin \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)\right| \]

3. Applied rewrites 99.8%

   \[\leadsto \left|\color{blue}{\mathsf{fma}\left(\frac{\sin t}{\cosh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right)}, ew, \tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot \left(\cos t \cdot eh\right)\right)}\right| \]

4. Taylor expanded in t around 0

   \[\leadsto \left|\mathsf{fma}\left(\frac{\sin t}{\cosh \sinh^{-1} \left(\frac{eh}{\color{blue}{ew \cdot t}}\right)}, ew, \tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot \left(\cos t \cdot eh\right)\right)\right| \]
5. Step-by-step derivation

   1. lower-*.f64 99.2

      \[\leadsto \left|\mathsf{fma}\left(\frac{\sin t}{\cosh \sinh^{-1} \left(\frac{eh}{ew \cdot \color{blue}{t}}\right)}, ew, \tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot \left(\cos t \cdot eh\right)\right)\right| \]

6. Applied rewrites 99.2%

   \[\leadsto \left|\mathsf{fma}\left(\frac{\sin t}{\cosh \sinh^{-1} \left(\frac{eh}{\color{blue}{ew \cdot t}}\right)}, ew, \tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot \left(\cos t \cdot eh\right)\right)\right| \]

7. Taylor expanded in t around 0

   \[\leadsto \left|\mathsf{fma}\left(\frac{\sin t}{\cosh \sinh^{-1} \left(\frac{eh}{ew \cdot t}\right)}, ew, \tanh \sinh^{-1} \left(\frac{eh}{\color{blue}{ew \cdot t}}\right) \cdot \left(\cos t \cdot eh\right)\right)\right| \]
8. Step-by-step derivation

   1. lower-*.f64 89.9

      \[\leadsto \left|\mathsf{fma}\left(\frac{\sin t}{\cosh \sinh^{-1} \left(\frac{eh}{ew \cdot t}\right)}, ew, \tanh \sinh^{-1} \left(\frac{eh}{ew \cdot \color{blue}{t}}\right) \cdot \left(\cos t \cdot eh\right)\right)\right| \]

9. Applied rewrites 89.9%

   \[\leadsto \left|\mathsf{fma}\left(\frac{\sin t}{\cosh \sinh^{-1} \left(\frac{eh}{ew \cdot t}\right)}, ew, \tanh \sinh^{-1} \left(\frac{eh}{\color{blue}{ew \cdot t}}\right) \cdot \left(\cos t \cdot eh\right)\right)\right| \]
10. Add Preprocessing

Alternative 4: 80.6% accurate, 2.1× speedup

Math

\[\begin{array}{l} \\ \begin{array}{l} t_1 := \frac{eh}{ew \cdot t}\\ t_2 := \cos t \cdot eh\\ t_3 := \left|t\_2 \cdot \tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right)\right|\\ \mathbf{if}\;eh \leq -1.7 \cdot 10^{-54}:\\ \;\;\;\;t\_3\\ \mathbf{elif}\;eh \leq 4.2 \cdot 10^{+72}:\\ \;\;\;\;\left|\frac{\mathsf{fma}\left(t\_1, t\_2, \sin t \cdot ew\right)}{\cosh \sinh^{-1} t\_1}\right|\\ \mathbf{else}:\\ \;\;\;\;t\_3\\ \end{array} \end{array} \]

FPCore

(FPCore (eh ew t)
 :precision binary64
 (let* ((t_1 (/ eh (* ew t)))
        (t_2 (* (cos t) eh))
        (t_3 (fabs (* t_2 (tanh (asinh (/ eh (* (tan t) ew))))))))
   (if (<= eh -1.7e-54)
     t_3
     (if (<= eh 4.2e+72)
       (fabs (/ (fma t_1 t_2 (* (sin t) ew)) (cosh (asinh t_1))))
       t_3))))

C

double code(double eh, double ew, double t) {
	double t_1 = eh / (ew * t);
	double t_2 = cos(t) * eh;
	double t_3 = fabs((t_2 * tanh(asinh((eh / (tan(t) * ew))))));
	double tmp;
	if (eh <= -1.7e-54) {
		tmp = t_3;
	} else if (eh <= 4.2e+72) {
		tmp = fabs((fma(t_1, t_2, (sin(t) * ew)) / cosh(asinh(t_1))));
	} else {
		tmp = t_3;
	}
	return tmp;
}

Julia

function code(eh, ew, t)
	t_1 = Float64(eh / Float64(ew * t))
	t_2 = Float64(cos(t) * eh)
	t_3 = abs(Float64(t_2 * tanh(asinh(Float64(eh / Float64(tan(t) * ew))))))
	tmp = 0.0
	if (eh <= -1.7e-54)
		tmp = t_3;
	elseif (eh <= 4.2e+72)
		tmp = abs(Float64(fma(t_1, t_2, Float64(sin(t) * ew)) / cosh(asinh(t_1))));
	else
		tmp = t_3;
	end
	return tmp
end

Wolfram

code[eh_, ew_, t_] := Block[{t$95$1 = N[(eh / N[(ew * t), $MachinePrecision]), $MachinePrecision]}, Block[{t$95$2 = N[(N[Cos[t], $MachinePrecision] * eh), $MachinePrecision]}, Block[{t$95$3 = N[Abs[N[(t$95$2 * N[Tanh[N[ArcSinh[N[(eh / N[(N[Tan[t], $MachinePrecision] * ew), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]], $MachinePrecision]), $MachinePrecision]], $MachinePrecision]}, If[LessEqual[eh, -1.7e-54], t$95$3, If[LessEqual[eh, 4.2e+72], N[Abs[N[(N[(t$95$1 * t$95$2 + N[(N[Sin[t], $MachinePrecision] * ew), $MachinePrecision]), $MachinePrecision] / N[Cosh[N[ArcSinh[t$95$1], $MachinePrecision]], $MachinePrecision]), $MachinePrecision]], $MachinePrecision], t$95$3]]]]]

Derivation

1. Split input into 2 regimes

2. if eh < -1.69999999999999994e-54 or 4.2000000000000003e72 < eh

   1. Initial program 99.8%

      \[\left|\left(ew \cdot \sin t\right) \cdot \cos \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right) + \left(eh \cdot \cos t\right) \cdot \sin \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)\right| \]

   2. Taylor expanded in t around 0

      \[\leadsto \left|\color{blue}{eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)}\right| \]
   3. Step-by-step derivation

      1. lower-*.f64 N/A

         \[\leadsto \left|eh \cdot \color{blue}{\sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)}\right| \]

      2. lower-sin.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      3. lower-atan.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      4. lower-/.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      5. lower-*.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      6. lower-cos.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      7. lower-*.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      8. lower-sin.f64 42.2

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

   4. Applied rewrites 42.2%

      \[\leadsto \left|\color{blue}{eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)}\right| \]

   6. Applied rewrites 21.0%

      \[\leadsto \color{blue}{\sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh}} \]

   7. Taylor expanded in ew around 0

      \[\leadsto \color{blue}{{\left(\sqrt{eh \cdot \left(\cos t \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right)}\right)}^{2}} \]
   8. Step-by-step derivation

      1. lower-pow.f64 N/A

         \[\leadsto {\left(\sqrt{eh \cdot \left(\cos t \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right)}\right)}^{\color{blue}{2}} \]

   9. Applied rewrites 30.7%

      \[\leadsto \color{blue}{{\left(\sqrt{eh \cdot \left(\cos t \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right)}\right)}^{2}} \]

   11. Applied rewrites 62.2%

       \[\leadsto \left|\left(\cos t \cdot eh\right) \cdot \tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right)\right| \]

   if -1.69999999999999994e-54 < eh < 4.2000000000000003e72

   1. Initial program 99.8%

      \[\left|\left(ew \cdot \sin t\right) \cdot \cos \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right) + \left(eh \cdot \cos t\right) \cdot \sin \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)\right| \]
   2. Step-by-step derivation

      1. lift-+.f64 N/A

         \[\leadsto \left|\color{blue}{\left(ew \cdot \sin t\right) \cdot \cos \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right) + \left(eh \cdot \cos t\right) \cdot \sin \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)}\right| \]

      2. +-commutative N/A

         \[\leadsto \left|\color{blue}{\left(eh \cdot \cos t\right) \cdot \sin \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right) + \left(ew \cdot \sin t\right) \cdot \cos \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)}\right| \]

      3. lift-*.f64 N/A

         \[\leadsto \left|\color{blue}{\left(eh \cdot \cos t\right) \cdot \sin \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)} + \left(ew \cdot \sin t\right) \cdot \cos \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)\right| \]

      4. *-commutative N/A

         \[\leadsto \left|\color{blue}{\sin \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right) \cdot \left(eh \cdot \cos t\right)} + \left(ew \cdot \sin t\right) \cdot \cos \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)\right| \]

      5. lift-sin.f64 N/A

         \[\leadsto \left|\color{blue}{\sin \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)} \cdot \left(eh \cdot \cos t\right) + \left(ew \cdot \sin t\right) \cdot \cos \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)\right| \]

      6. lift-atan.f64 N/A

         \[\leadsto \left|\sin \color{blue}{\tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)} \cdot \left(eh \cdot \cos t\right) + \left(ew \cdot \sin t\right) \cdot \cos \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)\right| \]

      7. sin-atan N/A

         \[\leadsto \left|\color{blue}{\frac{\frac{\frac{eh}{ew}}{\tan t}}{\sqrt{1 + \frac{\frac{eh}{ew}}{\tan t} \cdot \frac{\frac{eh}{ew}}{\tan t}}}} \cdot \left(eh \cdot \cos t\right) + \left(ew \cdot \sin t\right) \cdot \cos \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)\right| \]

      8. associate-*l/ N/A

         \[\leadsto \left|\color{blue}{\frac{\frac{\frac{eh}{ew}}{\tan t} \cdot \left(eh \cdot \cos t\right)}{\sqrt{1 + \frac{\frac{eh}{ew}}{\tan t} \cdot \frac{\frac{eh}{ew}}{\tan t}}}} + \left(ew \cdot \sin t\right) \cdot \cos \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)\right| \]

      9. lift-*.f64 N/A

         \[\leadsto \left|\frac{\frac{\frac{eh}{ew}}{\tan t} \cdot \left(eh \cdot \cos t\right)}{\sqrt{1 + \frac{\frac{eh}{ew}}{\tan t} \cdot \frac{\frac{eh}{ew}}{\tan t}}} + \color{blue}{\left(ew \cdot \sin t\right) \cdot \cos \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)}\right| \]

      10. lift-cos.f64 N/A

          \[\leadsto \left|\frac{\frac{\frac{eh}{ew}}{\tan t} \cdot \left(eh \cdot \cos t\right)}{\sqrt{1 + \frac{\frac{eh}{ew}}{\tan t} \cdot \frac{\frac{eh}{ew}}{\tan t}}} + \left(ew \cdot \sin t\right) \cdot \color{blue}{\cos \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)}\right| \]

      11. lift-atan.f64 N/A

          \[\leadsto \left|\frac{\frac{\frac{eh}{ew}}{\tan t} \cdot \left(eh \cdot \cos t\right)}{\sqrt{1 + \frac{\frac{eh}{ew}}{\tan t} \cdot \frac{\frac{eh}{ew}}{\tan t}}} + \left(ew \cdot \sin t\right) \cdot \cos \color{blue}{\tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)}\right| \]

      12. cos-atan N/A

          \[\leadsto \left|\frac{\frac{\frac{eh}{ew}}{\tan t} \cdot \left(eh \cdot \cos t\right)}{\sqrt{1 + \frac{\frac{eh}{ew}}{\tan t} \cdot \frac{\frac{eh}{ew}}{\tan t}}} + \left(ew \cdot \sin t\right) \cdot \color{blue}{\frac{1}{\sqrt{1 + \frac{\frac{eh}{ew}}{\tan t} \cdot \frac{\frac{eh}{ew}}{\tan t}}}}\right| \]

   3. Applied rewrites 62.3%

      \[\leadsto \left|\color{blue}{\frac{\mathsf{fma}\left(\frac{eh}{\tan t \cdot ew}, \cos t \cdot eh, \sin t \cdot ew\right)}{\cosh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right)}}\right| \]

   4. Taylor expanded in t around 0

      \[\leadsto \left|\frac{\mathsf{fma}\left(\frac{eh}{\color{blue}{ew \cdot t}}, \cos t \cdot eh, \sin t \cdot ew\right)}{\cosh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right)}\right| \]
   5. Step-by-step derivation

      1. lower-*.f64 50.8

         \[\leadsto \left|\frac{\mathsf{fma}\left(\frac{eh}{ew \cdot \color{blue}{t}}, \cos t \cdot eh, \sin t \cdot ew\right)}{\cosh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right)}\right| \]

   6. Applied rewrites 50.8%

      \[\leadsto \left|\frac{\mathsf{fma}\left(\frac{eh}{\color{blue}{ew \cdot t}}, \cos t \cdot eh, \sin t \cdot ew\right)}{\cosh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right)}\right| \]

   7. Taylor expanded in t around 0

      \[\leadsto \left|\frac{\mathsf{fma}\left(\frac{eh}{ew \cdot t}, \cos t \cdot eh, \sin t \cdot ew\right)}{\cosh \sinh^{-1} \left(\frac{eh}{\color{blue}{ew \cdot t}}\right)}\right| \]
   8. Step-by-step derivation

      1. lower-*.f64 58.0

         \[\leadsto \left|\frac{\mathsf{fma}\left(\frac{eh}{ew \cdot t}, \cos t \cdot eh, \sin t \cdot ew\right)}{\cosh \sinh^{-1} \left(\frac{eh}{ew \cdot \color{blue}{t}}\right)}\right| \]

   9. Applied rewrites 58.0%

      \[\leadsto \left|\frac{\mathsf{fma}\left(\frac{eh}{ew \cdot t}, \cos t \cdot eh, \sin t \cdot ew\right)}{\cosh \sinh^{-1} \left(\frac{eh}{\color{blue}{ew \cdot t}}\right)}\right| \]
3. Recombined 2 regimes into one program.
4. Add Preprocessing

Alternative 5: 77.5% accurate, 2.3× speedup

Math

\[\begin{array}{l} \\ \begin{array}{l} t_1 := \frac{eh}{ew \cdot t}\\ t_2 := \frac{\left|\left({t\_1}^{2} - -1\right) \cdot \left(\sin t \cdot ew\right)\right|}{\cosh \sinh^{-1} t\_1}\\ \mathbf{if}\;ew \leq -4.2 \cdot 10^{+171}:\\ \;\;\;\;t\_2\\ \mathbf{elif}\;ew \leq 3.3 \cdot 10^{+53}:\\ \;\;\;\;\left|\left(\cos t \cdot eh\right) \cdot \tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right)\right|\\ \mathbf{else}:\\ \;\;\;\;t\_2\\ \end{array} \end{array} \]

FPCore

(FPCore (eh ew t)
 :precision binary64
 (let* ((t_1 (/ eh (* ew t)))
        (t_2
         (/
          (fabs (* (- (pow t_1 2.0) -1.0) (* (sin t) ew)))
          (cosh (asinh t_1)))))
   (if (<= ew -4.2e+171)
     t_2
     (if (<= ew 3.3e+53)
       (fabs (* (* (cos t) eh) (tanh (asinh (/ eh (* (tan t) ew))))))
       t_2))))

C

double code(double eh, double ew, double t) {
	double t_1 = eh / (ew * t);
	double t_2 = fabs(((pow(t_1, 2.0) - -1.0) * (sin(t) * ew))) / cosh(asinh(t_1));
	double tmp;
	if (ew <= -4.2e+171) {
		tmp = t_2;
	} else if (ew <= 3.3e+53) {
		tmp = fabs(((cos(t) * eh) * tanh(asinh((eh / (tan(t) * ew))))));
	} else {
		tmp = t_2;
	}
	return tmp;
}

Python

def code(eh, ew, t):
	t_1 = eh / (ew * t)
	t_2 = math.fabs(((math.pow(t_1, 2.0) - -1.0) * (math.sin(t) * ew))) / math.cosh(math.asinh(t_1))
	tmp = 0
	if ew <= -4.2e+171:
		tmp = t_2
	elif ew <= 3.3e+53:
		tmp = math.fabs(((math.cos(t) * eh) * math.tanh(math.asinh((eh / (math.tan(t) * ew))))))
	else:
		tmp = t_2
	return tmp

Julia

function code(eh, ew, t)
	t_1 = Float64(eh / Float64(ew * t))
	t_2 = Float64(abs(Float64(Float64((t_1 ^ 2.0) - -1.0) * Float64(sin(t) * ew))) / cosh(asinh(t_1)))
	tmp = 0.0
	if (ew <= -4.2e+171)
		tmp = t_2;
	elseif (ew <= 3.3e+53)
		tmp = abs(Float64(Float64(cos(t) * eh) * tanh(asinh(Float64(eh / Float64(tan(t) * ew))))));
	else
		tmp = t_2;
	end
	return tmp
end

MATLAB

function tmp_2 = code(eh, ew, t)
	t_1 = eh / (ew * t);
	t_2 = abs((((t_1 ^ 2.0) - -1.0) * (sin(t) * ew))) / cosh(asinh(t_1));
	tmp = 0.0;
	if (ew <= -4.2e+171)
		tmp = t_2;
	elseif (ew <= 3.3e+53)
		tmp = abs(((cos(t) * eh) * tanh(asinh((eh / (tan(t) * ew))))));
	else
		tmp = t_2;
	end
	tmp_2 = tmp;
end

Wolfram

code[eh_, ew_, t_] := Block[{t$95$1 = N[(eh / N[(ew * t), $MachinePrecision]), $MachinePrecision]}, Block[{t$95$2 = N[(N[Abs[N[(N[(N[Power[t$95$1, 2.0], $MachinePrecision] - -1.0), $MachinePrecision] * N[(N[Sin[t], $MachinePrecision] * ew), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / N[Cosh[N[ArcSinh[t$95$1], $MachinePrecision]], $MachinePrecision]), $MachinePrecision]}, If[LessEqual[ew, -4.2e+171], t$95$2, If[LessEqual[ew, 3.3e+53], N[Abs[N[(N[(N[Cos[t], $MachinePrecision] * eh), $MachinePrecision] * N[Tanh[N[ArcSinh[N[(eh / N[(N[Tan[t], $MachinePrecision] * ew), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]], $MachinePrecision]), $MachinePrecision]], $MachinePrecision], t$95$2]]]]

Derivation

1. Split input into 2 regimes

2. if ew < -4.2000000000000003e171 or 3.3000000000000002e53 < ew

   1. Initial program 99.8%

      \[\left|\left(ew \cdot \sin t\right) \cdot \cos \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right) + \left(eh \cdot \cos t\right) \cdot \sin \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)\right| \]

   3. Applied rewrites 99.8%

      \[\leadsto \left|\color{blue}{\mathsf{fma}\left(\frac{\sin t}{\cosh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right)}, ew, \tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot \left(\cos t \cdot eh\right)\right)}\right| \]

   5. Applied rewrites 56.4%

      \[\leadsto \color{blue}{\frac{\left|\left({\left(\frac{eh}{\tan t \cdot ew}\right)}^{2} - -1\right) \cdot \left(\sin t \cdot ew\right)\right|}{\cosh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right)}} \]

   6. Taylor expanded in t around 0

      \[\leadsto \frac{\left|\left({\left(\frac{eh}{\color{blue}{ew \cdot t}}\right)}^{2} - -1\right) \cdot \left(\sin t \cdot ew\right)\right|}{\cosh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right)} \]
   7. Step-by-step derivation

      1. lower-*.f64 47.8

         \[\leadsto \frac{\left|\left({\left(\frac{eh}{ew \cdot \color{blue}{t}}\right)}^{2} - -1\right) \cdot \left(\sin t \cdot ew\right)\right|}{\cosh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right)} \]

   8. Applied rewrites 47.8%

      \[\leadsto \frac{\left|\left({\left(\frac{eh}{\color{blue}{ew \cdot t}}\right)}^{2} - -1\right) \cdot \left(\sin t \cdot ew\right)\right|}{\cosh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right)} \]

   9. Taylor expanded in t around 0

      \[\leadsto \frac{\left|\left({\left(\frac{eh}{ew \cdot t}\right)}^{2} - -1\right) \cdot \left(\sin t \cdot ew\right)\right|}{\cosh \sinh^{-1} \left(\frac{eh}{\color{blue}{ew \cdot t}}\right)} \]
   10. Step-by-step derivation

       1. lower-*.f64 48.2

          \[\leadsto \frac{\left|\left({\left(\frac{eh}{ew \cdot t}\right)}^{2} - -1\right) \cdot \left(\sin t \cdot ew\right)\right|}{\cosh \sinh^{-1} \left(\frac{eh}{ew \cdot \color{blue}{t}}\right)} \]

   11. Applied rewrites 48.2%

       \[\leadsto \frac{\left|\left({\left(\frac{eh}{ew \cdot t}\right)}^{2} - -1\right) \cdot \left(\sin t \cdot ew\right)\right|}{\cosh \sinh^{-1} \left(\frac{eh}{\color{blue}{ew \cdot t}}\right)} \]

   if -4.2000000000000003e171 < ew < 3.3000000000000002e53

   1. Initial program 99.8%

      \[\left|\left(ew \cdot \sin t\right) \cdot \cos \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right) + \left(eh \cdot \cos t\right) \cdot \sin \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)\right| \]

   2. Taylor expanded in t around 0

      \[\leadsto \left|\color{blue}{eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)}\right| \]
   3. Step-by-step derivation

      1. lower-*.f64 N/A

         \[\leadsto \left|eh \cdot \color{blue}{\sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)}\right| \]

      2. lower-sin.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      3. lower-atan.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      4. lower-/.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      5. lower-*.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      6. lower-cos.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      7. lower-*.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      8. lower-sin.f64 42.2

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

   4. Applied rewrites 42.2%

      \[\leadsto \left|\color{blue}{eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)}\right| \]

   6. Applied rewrites 21.0%

      \[\leadsto \color{blue}{\sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh}} \]

   7. Taylor expanded in ew around 0

      \[\leadsto \color{blue}{{\left(\sqrt{eh \cdot \left(\cos t \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right)}\right)}^{2}} \]
   8. Step-by-step derivation

      1. lower-pow.f64 N/A

         \[\leadsto {\left(\sqrt{eh \cdot \left(\cos t \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right)}\right)}^{\color{blue}{2}} \]

   9. Applied rewrites 30.7%

      \[\leadsto \color{blue}{{\left(\sqrt{eh \cdot \left(\cos t \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right)}\right)}^{2}} \]

   11. Applied rewrites 62.2%

       \[\leadsto \left|\left(\cos t \cdot eh\right) \cdot \tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right)\right| \]
3. Recombined 2 regimes into one program.
4. Add Preprocessing

Alternative 6: 62.2% accurate, 2.4× speedup

Math

\[\begin{array}{l} \\ \begin{array}{l} t_1 := \left|\tanh \sinh^{-1} \left(\frac{\frac{\mathsf{fma}\left(\left(t \cdot t\right) \cdot eh, -0.3333333333333333, eh\right)}{ew}}{t}\right) \cdot eh\right|\\ t_2 := \frac{eh}{ew \cdot t}\\ \mathbf{if}\;eh \leq -1.7 \cdot 10^{-54}:\\ \;\;\;\;t\_1\\ \mathbf{elif}\;eh \leq 8.6 \cdot 10^{+52}:\\ \;\;\;\;\frac{\left|\left({t\_2}^{2} - -1\right) \cdot \left(\sin t \cdot ew\right)\right|}{\cosh \sinh^{-1} t\_2}\\ \mathbf{else}:\\ \;\;\;\;t\_1\\ \end{array} \end{array} \]

FPCore

(FPCore (eh ew t)
 :precision binary64
 (let* ((t_1
         (fabs
          (*
           (tanh
            (asinh (/ (/ (fma (* (* t t) eh) -0.3333333333333333 eh) ew) t)))
           eh)))
        (t_2 (/ eh (* ew t))))
   (if (<= eh -1.7e-54)
     t_1
     (if (<= eh 8.6e+52)
       (/ (fabs (* (- (pow t_2 2.0) -1.0) (* (sin t) ew))) (cosh (asinh t_2)))
       t_1))))

C

double code(double eh, double ew, double t) {
	double t_1 = fabs((tanh(asinh(((fma(((t * t) * eh), -0.3333333333333333, eh) / ew) / t))) * eh));
	double t_2 = eh / (ew * t);
	double tmp;
	if (eh <= -1.7e-54) {
		tmp = t_1;
	} else if (eh <= 8.6e+52) {
		tmp = fabs(((pow(t_2, 2.0) - -1.0) * (sin(t) * ew))) / cosh(asinh(t_2));
	} else {
		tmp = t_1;
	}
	return tmp;
}

Julia

function code(eh, ew, t)
	t_1 = abs(Float64(tanh(asinh(Float64(Float64(fma(Float64(Float64(t * t) * eh), -0.3333333333333333, eh) / ew) / t))) * eh))
	t_2 = Float64(eh / Float64(ew * t))
	tmp = 0.0
	if (eh <= -1.7e-54)
		tmp = t_1;
	elseif (eh <= 8.6e+52)
		tmp = Float64(abs(Float64(Float64((t_2 ^ 2.0) - -1.0) * Float64(sin(t) * ew))) / cosh(asinh(t_2)));
	else
		tmp = t_1;
	end
	return tmp
end

Wolfram

code[eh_, ew_, t_] := Block[{t$95$1 = N[Abs[N[(N[Tanh[N[ArcSinh[N[(N[(N[(N[(N[(t * t), $MachinePrecision] * eh), $MachinePrecision] * -0.3333333333333333 + eh), $MachinePrecision] / ew), $MachinePrecision] / t), $MachinePrecision]], $MachinePrecision]], $MachinePrecision] * eh), $MachinePrecision]], $MachinePrecision]}, Block[{t$95$2 = N[(eh / N[(ew * t), $MachinePrecision]), $MachinePrecision]}, If[LessEqual[eh, -1.7e-54], t$95$1, If[LessEqual[eh, 8.6e+52], N[(N[Abs[N[(N[(N[Power[t$95$2, 2.0], $MachinePrecision] - -1.0), $MachinePrecision] * N[(N[Sin[t], $MachinePrecision] * ew), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / N[Cosh[N[ArcSinh[t$95$2], $MachinePrecision]], $MachinePrecision]), $MachinePrecision], t$95$1]]]]

Derivation

1. Split input into 2 regimes

2. if eh < -1.69999999999999994e-54 or 8.5999999999999999e52 < eh

   1. Initial program 99.8%

      \[\left|\left(ew \cdot \sin t\right) \cdot \cos \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right) + \left(eh \cdot \cos t\right) \cdot \sin \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)\right| \]

   2. Taylor expanded in t around 0

      \[\leadsto \left|\color{blue}{eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)}\right| \]
   3. Step-by-step derivation

      1. lower-*.f64 N/A

         \[\leadsto \left|eh \cdot \color{blue}{\sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)}\right| \]

      2. lower-sin.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      3. lower-atan.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      4. lower-/.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      5. lower-*.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      6. lower-cos.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      7. lower-*.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      8. lower-sin.f64 42.2

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

   4. Applied rewrites 42.2%

      \[\leadsto \left|\color{blue}{eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)}\right| \]

   6. Applied rewrites 21.0%

      \[\leadsto \color{blue}{\sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh}} \]

   7. Taylor expanded in t around 0

      \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\frac{-1}{3} \cdot \frac{eh \cdot {t}^{2}}{ew} + \frac{eh}{ew}}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh} \]
   8. Step-by-step derivation

      1. lower-/.f64 N/A

         \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\frac{-1}{3} \cdot \frac{eh \cdot {t}^{2}}{ew} + \frac{eh}{ew}}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh} \]

      2. lower-fma.f64 N/A

         \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh} \]

      3. lower-/.f64 N/A

         \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh} \]

      4. lower-*.f64 N/A

         \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh} \]

      5. lower-pow.f64 N/A

         \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh} \]

      6. lower-/.f64 18.7

         \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(-0.3333333333333333, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh} \]

   9. Applied rewrites 18.7%

      \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(-0.3333333333333333, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh} \]

   10. Taylor expanded in t around 0

       \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{\frac{-1}{3} \cdot \frac{eh \cdot {t}^{2}}{ew} + \frac{eh}{ew}}{t}\right) \cdot eh} \]
   11. Step-by-step derivation

       1. lower-/.f64 N/A

          \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{\frac{-1}{3} \cdot \frac{eh \cdot {t}^{2}}{ew} + \frac{eh}{ew}}{t}\right) \cdot eh} \]

       2. lower-fma.f64 N/A

          \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \]

       3. lower-/.f64 N/A

          \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \]

       4. lower-*.f64 N/A

          \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \]

       5. lower-pow.f64 N/A

          \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \]

       6. lower-/.f64 20.1

          \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(-0.3333333333333333, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(-0.3333333333333333, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \]

   12. Applied rewrites 20.1%

       \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(-0.3333333333333333, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(-0.3333333333333333, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \]

   14. Applied rewrites 42.4%

       \[\leadsto \color{blue}{\left|\tanh \sinh^{-1} \left(\frac{\frac{\mathsf{fma}\left(\left(t \cdot t\right) \cdot eh, -0.3333333333333333, eh\right)}{ew}}{t}\right) \cdot eh\right|} \]

   if -1.69999999999999994e-54 < eh < 8.5999999999999999e52

   1. Initial program 99.8%

      \[\left|\left(ew \cdot \sin t\right) \cdot \cos \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right) + \left(eh \cdot \cos t\right) \cdot \sin \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)\right| \]

   3. Applied rewrites 99.8%

      \[\leadsto \left|\color{blue}{\mathsf{fma}\left(\frac{\sin t}{\cosh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right)}, ew, \tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot \left(\cos t \cdot eh\right)\right)}\right| \]

   5. Applied rewrites 56.4%

      \[\leadsto \color{blue}{\frac{\left|\left({\left(\frac{eh}{\tan t \cdot ew}\right)}^{2} - -1\right) \cdot \left(\sin t \cdot ew\right)\right|}{\cosh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right)}} \]

   6. Taylor expanded in t around 0

      \[\leadsto \frac{\left|\left({\left(\frac{eh}{\color{blue}{ew \cdot t}}\right)}^{2} - -1\right) \cdot \left(\sin t \cdot ew\right)\right|}{\cosh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right)} \]
   7. Step-by-step derivation

      1. lower-*.f64 47.8

         \[\leadsto \frac{\left|\left({\left(\frac{eh}{ew \cdot \color{blue}{t}}\right)}^{2} - -1\right) \cdot \left(\sin t \cdot ew\right)\right|}{\cosh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right)} \]

   8. Applied rewrites 47.8%

      \[\leadsto \frac{\left|\left({\left(\frac{eh}{\color{blue}{ew \cdot t}}\right)}^{2} - -1\right) \cdot \left(\sin t \cdot ew\right)\right|}{\cosh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right)} \]

   9. Taylor expanded in t around 0

      \[\leadsto \frac{\left|\left({\left(\frac{eh}{ew \cdot t}\right)}^{2} - -1\right) \cdot \left(\sin t \cdot ew\right)\right|}{\cosh \sinh^{-1} \left(\frac{eh}{\color{blue}{ew \cdot t}}\right)} \]
   10. Step-by-step derivation

       1. lower-*.f64 48.2

          \[\leadsto \frac{\left|\left({\left(\frac{eh}{ew \cdot t}\right)}^{2} - -1\right) \cdot \left(\sin t \cdot ew\right)\right|}{\cosh \sinh^{-1} \left(\frac{eh}{ew \cdot \color{blue}{t}}\right)} \]

   11. Applied rewrites 48.2%

       \[\leadsto \frac{\left|\left({\left(\frac{eh}{ew \cdot t}\right)}^{2} - -1\right) \cdot \left(\sin t \cdot ew\right)\right|}{\cosh \sinh^{-1} \left(\frac{eh}{\color{blue}{ew \cdot t}}\right)} \]
3. Recombined 2 regimes into one program.
4. Add Preprocessing

Alternative 7: 61.0% accurate, 5.2× speedup

Math

\[\begin{array}{l} \\ \begin{array}{l} t_1 := \left|\sin t \cdot ew\right|\\ \mathbf{if}\;t \leq -1.4 \cdot 10^{-51}:\\ \;\;\;\;t\_1\\ \mathbf{elif}\;t \leq 4.3 \cdot 10^{-45}:\\ \;\;\;\;\left|\tanh \sinh^{-1} \left(\frac{\frac{\mathsf{fma}\left(\left(t \cdot t\right) \cdot eh, -0.3333333333333333, eh\right)}{ew}}{t}\right) \cdot eh\right|\\ \mathbf{else}:\\ \;\;\;\;t\_1\\ \end{array} \end{array} \]

FPCore

(FPCore (eh ew t)
 :precision binary64
 (let* ((t_1 (fabs (* (sin t) ew))))
   (if (<= t -1.4e-51)
     t_1
     (if (<= t 4.3e-45)
       (fabs
        (*
         (tanh
          (asinh (/ (/ (fma (* (* t t) eh) -0.3333333333333333 eh) ew) t)))
         eh))
       t_1))))

C

double code(double eh, double ew, double t) {
	double t_1 = fabs((sin(t) * ew));
	double tmp;
	if (t <= -1.4e-51) {
		tmp = t_1;
	} else if (t <= 4.3e-45) {
		tmp = fabs((tanh(asinh(((fma(((t * t) * eh), -0.3333333333333333, eh) / ew) / t))) * eh));
	} else {
		tmp = t_1;
	}
	return tmp;
}

Julia

function code(eh, ew, t)
	t_1 = abs(Float64(sin(t) * ew))
	tmp = 0.0
	if (t <= -1.4e-51)
		tmp = t_1;
	elseif (t <= 4.3e-45)
		tmp = abs(Float64(tanh(asinh(Float64(Float64(fma(Float64(Float64(t * t) * eh), -0.3333333333333333, eh) / ew) / t))) * eh));
	else
		tmp = t_1;
	end
	return tmp
end

Wolfram

code[eh_, ew_, t_] := Block[{t$95$1 = N[Abs[N[(N[Sin[t], $MachinePrecision] * ew), $MachinePrecision]], $MachinePrecision]}, If[LessEqual[t, -1.4e-51], t$95$1, If[LessEqual[t, 4.3e-45], N[Abs[N[(N[Tanh[N[ArcSinh[N[(N[(N[(N[(N[(t * t), $MachinePrecision] * eh), $MachinePrecision] * -0.3333333333333333 + eh), $MachinePrecision] / ew), $MachinePrecision] / t), $MachinePrecision]], $MachinePrecision]], $MachinePrecision] * eh), $MachinePrecision]], $MachinePrecision], t$95$1]]]

Derivation

1. Split input into 2 regimes

2. if t < -1.4e-51 or 4.2999999999999999e-45 < t

   1. Initial program 99.8%

      \[\left|\left(ew \cdot \sin t\right) \cdot \cos \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right) + \left(eh \cdot \cos t\right) \cdot \sin \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)\right| \]

   3. Applied rewrites 99.8%

      \[\leadsto \left|\color{blue}{\mathsf{fma}\left(\frac{\sin t}{\cosh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right)}, ew, \tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot \left(\cos t \cdot eh\right)\right)}\right| \]

   4. Taylor expanded in eh around 0

      \[\leadsto \left|\color{blue}{ew \cdot \sin t}\right| \]
   5. Step-by-step derivation

      1. lower-*.f64 N/A

         \[\leadsto \left|ew \cdot \color{blue}{\sin t}\right| \]

      2. lower-sin.f64 41.3

         \[\leadsto \left|ew \cdot \sin t\right| \]

   6. Applied rewrites 41.3%

      \[\leadsto \left|\color{blue}{ew \cdot \sin t}\right| \]
   7. Step-by-step derivation

      1. lift-*.f64 N/A

         \[\leadsto \left|ew \cdot \color{blue}{\sin t}\right| \]

      2. *-commutative N/A

         \[\leadsto \left|\sin t \cdot \color{blue}{ew}\right| \]

      3. lift-*.f64 41.3

         \[\leadsto \left|\sin t \cdot \color{blue}{ew}\right| \]

   8. Applied rewrites 41.3%

      \[\leadsto \left|\color{blue}{\sin t \cdot ew}\right| \]

   if -1.4e-51 < t < 4.2999999999999999e-45

   1. Initial program 99.8%

      \[\left|\left(ew \cdot \sin t\right) \cdot \cos \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right) + \left(eh \cdot \cos t\right) \cdot \sin \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)\right| \]

   2. Taylor expanded in t around 0

      \[\leadsto \left|\color{blue}{eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)}\right| \]
   3. Step-by-step derivation

      1. lower-*.f64 N/A

         \[\leadsto \left|eh \cdot \color{blue}{\sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)}\right| \]

      2. lower-sin.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      3. lower-atan.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      4. lower-/.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      5. lower-*.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      6. lower-cos.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      7. lower-*.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      8. lower-sin.f64 42.2

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

   4. Applied rewrites 42.2%

      \[\leadsto \left|\color{blue}{eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)}\right| \]

   6. Applied rewrites 21.0%

      \[\leadsto \color{blue}{\sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh}} \]

   7. Taylor expanded in t around 0

      \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\frac{-1}{3} \cdot \frac{eh \cdot {t}^{2}}{ew} + \frac{eh}{ew}}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh} \]
   8. Step-by-step derivation

      1. lower-/.f64 N/A

         \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\frac{-1}{3} \cdot \frac{eh \cdot {t}^{2}}{ew} + \frac{eh}{ew}}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh} \]

      2. lower-fma.f64 N/A

         \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh} \]

      3. lower-/.f64 N/A

         \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh} \]

      4. lower-*.f64 N/A

         \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh} \]

      5. lower-pow.f64 N/A

         \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh} \]

      6. lower-/.f64 18.7

         \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(-0.3333333333333333, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh} \]

   9. Applied rewrites 18.7%

      \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(-0.3333333333333333, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh} \]

   10. Taylor expanded in t around 0

       \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{\frac{-1}{3} \cdot \frac{eh \cdot {t}^{2}}{ew} + \frac{eh}{ew}}{t}\right) \cdot eh} \]
   11. Step-by-step derivation

       1. lower-/.f64 N/A

          \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{\frac{-1}{3} \cdot \frac{eh \cdot {t}^{2}}{ew} + \frac{eh}{ew}}{t}\right) \cdot eh} \]

       2. lower-fma.f64 N/A

          \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \]

       3. lower-/.f64 N/A

          \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \]

       4. lower-*.f64 N/A

          \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \]

       5. lower-pow.f64 N/A

          \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \]

       6. lower-/.f64 20.1

          \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(-0.3333333333333333, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(-0.3333333333333333, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \]

   12. Applied rewrites 20.1%

       \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(-0.3333333333333333, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(-0.3333333333333333, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \]

   14. Applied rewrites 42.4%

       \[\leadsto \color{blue}{\left|\tanh \sinh^{-1} \left(\frac{\frac{\mathsf{fma}\left(\left(t \cdot t\right) \cdot eh, -0.3333333333333333, eh\right)}{ew}}{t}\right) \cdot eh\right|} \]
3. Recombined 2 regimes into one program.
4. Add Preprocessing

Alternative 8: 46.7% accurate, 5.5× speedup

Math

\[\begin{array}{l} \\ \begin{array}{l} \mathbf{if}\;eh \leq -1.12 \cdot 10^{+104}:\\ \;\;\;\;\tanh \sinh^{-1} \left(\frac{\frac{\mathsf{fma}\left(\left(t \cdot t\right) \cdot eh, -0.3333333333333333, eh\right)}{ew}}{t}\right) \cdot eh\\ \mathbf{elif}\;eh \leq 1.45 \cdot 10^{+86}:\\ \;\;\;\;\left|\sin t \cdot ew\right|\\ \mathbf{else}:\\ \;\;\;\;\tanh \sinh^{-1} \left(\frac{eh}{ew \cdot t}\right) \cdot eh\\ \end{array} \end{array} \]

FPCore

(FPCore (eh ew t)
 :precision binary64
 (if (<= eh -1.12e+104)
   (*
    (tanh (asinh (/ (/ (fma (* (* t t) eh) -0.3333333333333333 eh) ew) t)))
    eh)
   (if (<= eh 1.45e+86)
     (fabs (* (sin t) ew))
     (* (tanh (asinh (/ eh (* ew t)))) eh))))

C

double code(double eh, double ew, double t) {
	double tmp;
	if (eh <= -1.12e+104) {
		tmp = tanh(asinh(((fma(((t * t) * eh), -0.3333333333333333, eh) / ew) / t))) * eh;
	} else if (eh <= 1.45e+86) {
		tmp = fabs((sin(t) * ew));
	} else {
		tmp = tanh(asinh((eh / (ew * t)))) * eh;
	}
	return tmp;
}

Julia

function code(eh, ew, t)
	tmp = 0.0
	if (eh <= -1.12e+104)
		tmp = Float64(tanh(asinh(Float64(Float64(fma(Float64(Float64(t * t) * eh), -0.3333333333333333, eh) / ew) / t))) * eh);
	elseif (eh <= 1.45e+86)
		tmp = abs(Float64(sin(t) * ew));
	else
		tmp = Float64(tanh(asinh(Float64(eh / Float64(ew * t)))) * eh);
	end
	return tmp
end

Wolfram

code[eh_, ew_, t_] := If[LessEqual[eh, -1.12e+104], N[(N[Tanh[N[ArcSinh[N[(N[(N[(N[(N[(t * t), $MachinePrecision] * eh), $MachinePrecision] * -0.3333333333333333 + eh), $MachinePrecision] / ew), $MachinePrecision] / t), $MachinePrecision]], $MachinePrecision]], $MachinePrecision] * eh), $MachinePrecision], If[LessEqual[eh, 1.45e+86], N[Abs[N[(N[Sin[t], $MachinePrecision] * ew), $MachinePrecision]], $MachinePrecision], N[(N[Tanh[N[ArcSinh[N[(eh / N[(ew * t), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]], $MachinePrecision] * eh), $MachinePrecision]]]

Derivation

1. Split input into 3 regimes

2. if eh < -1.12000000000000003e104

   1. Initial program 99.8%

      \[\left|\left(ew \cdot \sin t\right) \cdot \cos \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right) + \left(eh \cdot \cos t\right) \cdot \sin \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)\right| \]

   2. Taylor expanded in t around 0

      \[\leadsto \left|\color{blue}{eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)}\right| \]
   3. Step-by-step derivation

      1. lower-*.f64 N/A

         \[\leadsto \left|eh \cdot \color{blue}{\sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)}\right| \]

      2. lower-sin.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      3. lower-atan.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      4. lower-/.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      5. lower-*.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      6. lower-cos.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      7. lower-*.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      8. lower-sin.f64 42.2

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

   4. Applied rewrites 42.2%

      \[\leadsto \left|\color{blue}{eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)}\right| \]

   6. Applied rewrites 21.0%

      \[\leadsto \color{blue}{\sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh}} \]

   7. Taylor expanded in t around 0

      \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\frac{-1}{3} \cdot \frac{eh \cdot {t}^{2}}{ew} + \frac{eh}{ew}}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh} \]
   8. Step-by-step derivation

      1. lower-/.f64 N/A

         \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\frac{-1}{3} \cdot \frac{eh \cdot {t}^{2}}{ew} + \frac{eh}{ew}}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh} \]

      2. lower-fma.f64 N/A

         \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh} \]

      3. lower-/.f64 N/A

         \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh} \]

      4. lower-*.f64 N/A

         \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh} \]

      5. lower-pow.f64 N/A

         \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh} \]

      6. lower-/.f64 18.7

         \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(-0.3333333333333333, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh} \]

   9. Applied rewrites 18.7%

      \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(-0.3333333333333333, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh} \]

   10. Taylor expanded in t around 0

       \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{\frac{-1}{3} \cdot \frac{eh \cdot {t}^{2}}{ew} + \frac{eh}{ew}}{t}\right) \cdot eh} \]
   11. Step-by-step derivation

       1. lower-/.f64 N/A

          \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{\frac{-1}{3} \cdot \frac{eh \cdot {t}^{2}}{ew} + \frac{eh}{ew}}{t}\right) \cdot eh} \]

       2. lower-fma.f64 N/A

          \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \]

       3. lower-/.f64 N/A

          \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \]

       4. lower-*.f64 N/A

          \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \]

       5. lower-pow.f64 N/A

          \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(\frac{-1}{3}, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \]

       6. lower-/.f64 20.1

          \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(-0.3333333333333333, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(-0.3333333333333333, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \]

   12. Applied rewrites 20.1%

       \[\leadsto \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(-0.3333333333333333, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{\mathsf{fma}\left(-0.3333333333333333, \frac{eh \cdot {t}^{2}}{ew}, \frac{eh}{ew}\right)}{t}\right) \cdot eh} \]

   14. Applied rewrites 22.0%

       \[\leadsto \color{blue}{\tanh \sinh^{-1} \left(\frac{\frac{\mathsf{fma}\left(\left(t \cdot t\right) \cdot eh, -0.3333333333333333, eh\right)}{ew}}{t}\right) \cdot eh} \]

   if -1.12000000000000003e104 < eh < 1.44999999999999995e86

   1. Initial program 99.8%

      \[\left|\left(ew \cdot \sin t\right) \cdot \cos \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right) + \left(eh \cdot \cos t\right) \cdot \sin \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)\right| \]

   3. Applied rewrites 99.8%

      \[\leadsto \left|\color{blue}{\mathsf{fma}\left(\frac{\sin t}{\cosh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right)}, ew, \tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot \left(\cos t \cdot eh\right)\right)}\right| \]

   4. Taylor expanded in eh around 0

      \[\leadsto \left|\color{blue}{ew \cdot \sin t}\right| \]
   5. Step-by-step derivation

      1. lower-*.f64 N/A

         \[\leadsto \left|ew \cdot \color{blue}{\sin t}\right| \]

      2. lower-sin.f64 41.3

         \[\leadsto \left|ew \cdot \sin t\right| \]

   6. Applied rewrites 41.3%

      \[\leadsto \left|\color{blue}{ew \cdot \sin t}\right| \]
   7. Step-by-step derivation

      1. lift-*.f64 N/A

         \[\leadsto \left|ew \cdot \color{blue}{\sin t}\right| \]

      2. *-commutative N/A

         \[\leadsto \left|\sin t \cdot \color{blue}{ew}\right| \]

      3. lift-*.f64 41.3

         \[\leadsto \left|\sin t \cdot \color{blue}{ew}\right| \]

   8. Applied rewrites 41.3%

      \[\leadsto \left|\color{blue}{\sin t \cdot ew}\right| \]

   if 1.44999999999999995e86 < eh

   1. Initial program 99.8%

      \[\left|\left(ew \cdot \sin t\right) \cdot \cos \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right) + \left(eh \cdot \cos t\right) \cdot \sin \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)\right| \]

   2. Taylor expanded in t around 0

      \[\leadsto \left|\color{blue}{eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)}\right| \]
   3. Step-by-step derivation

      1. lower-*.f64 N/A

         \[\leadsto \left|eh \cdot \color{blue}{\sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)}\right| \]

      2. lower-sin.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      3. lower-atan.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      4. lower-/.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      5. lower-*.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      6. lower-cos.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      7. lower-*.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      8. lower-sin.f64 42.2

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

   4. Applied rewrites 42.2%

      \[\leadsto \left|\color{blue}{eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)}\right| \]

   6. Applied rewrites 21.0%

      \[\leadsto \color{blue}{\sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh}} \]

   8. Applied rewrites 21.7%

      \[\leadsto \color{blue}{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh} \]

   9. Taylor expanded in t around 0

      \[\leadsto \tanh \sinh^{-1} \left(\frac{eh}{ew \cdot t}\right) \cdot eh \]
   10. Step-by-step derivation

       1. lower-*.f64 20.9

          \[\leadsto \tanh \sinh^{-1} \left(\frac{eh}{ew \cdot t}\right) \cdot eh \]

   11. Applied rewrites 20.9%

       \[\leadsto \tanh \sinh^{-1} \left(\frac{eh}{ew \cdot t}\right) \cdot eh \]
3. Recombined 3 regimes into one program.
4. Add Preprocessing

Alternative 9: 45.9% accurate, 5.5× speedup

Math

\[\begin{array}{l} \\ \begin{array}{l} t_1 := \left|\sin t \cdot ew\right|\\ \mathbf{if}\;t \leq -1.2 \cdot 10^{-111}:\\ \;\;\;\;t\_1\\ \mathbf{elif}\;t \leq 7.2 \cdot 10^{-167}:\\ \;\;\;\;\tanh \sinh^{-1} \left(\frac{eh}{ew \cdot t}\right) \cdot eh\\ \mathbf{else}:\\ \;\;\;\;t\_1\\ \end{array} \end{array} \]

FPCore

(FPCore (eh ew t)
 :precision binary64
 (let* ((t_1 (fabs (* (sin t) ew))))
   (if (<= t -1.2e-111)
     t_1
     (if (<= t 7.2e-167) (* (tanh (asinh (/ eh (* ew t)))) eh) t_1))))

C

double code(double eh, double ew, double t) {
	double t_1 = fabs((sin(t) * ew));
	double tmp;
	if (t <= -1.2e-111) {
		tmp = t_1;
	} else if (t <= 7.2e-167) {
		tmp = tanh(asinh((eh / (ew * t)))) * eh;
	} else {
		tmp = t_1;
	}
	return tmp;
}

Python

def code(eh, ew, t):
	t_1 = math.fabs((math.sin(t) * ew))
	tmp = 0
	if t <= -1.2e-111:
		tmp = t_1
	elif t <= 7.2e-167:
		tmp = math.tanh(math.asinh((eh / (ew * t)))) * eh
	else:
		tmp = t_1
	return tmp

Julia

function code(eh, ew, t)
	t_1 = abs(Float64(sin(t) * ew))
	tmp = 0.0
	if (t <= -1.2e-111)
		tmp = t_1;
	elseif (t <= 7.2e-167)
		tmp = Float64(tanh(asinh(Float64(eh / Float64(ew * t)))) * eh);
	else
		tmp = t_1;
	end
	return tmp
end

MATLAB

function tmp_2 = code(eh, ew, t)
	t_1 = abs((sin(t) * ew));
	tmp = 0.0;
	if (t <= -1.2e-111)
		tmp = t_1;
	elseif (t <= 7.2e-167)
		tmp = tanh(asinh((eh / (ew * t)))) * eh;
	else
		tmp = t_1;
	end
	tmp_2 = tmp;
end

Wolfram

code[eh_, ew_, t_] := Block[{t$95$1 = N[Abs[N[(N[Sin[t], $MachinePrecision] * ew), $MachinePrecision]], $MachinePrecision]}, If[LessEqual[t, -1.2e-111], t$95$1, If[LessEqual[t, 7.2e-167], N[(N[Tanh[N[ArcSinh[N[(eh / N[(ew * t), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]], $MachinePrecision] * eh), $MachinePrecision], t$95$1]]]

Derivation

1. Split input into 2 regimes

2. if t < -1.2e-111 or 7.2000000000000002e-167 < t

   1. Initial program 99.8%

      \[\left|\left(ew \cdot \sin t\right) \cdot \cos \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right) + \left(eh \cdot \cos t\right) \cdot \sin \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)\right| \]

   3. Applied rewrites 99.8%

      \[\leadsto \left|\color{blue}{\mathsf{fma}\left(\frac{\sin t}{\cosh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right)}, ew, \tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot \left(\cos t \cdot eh\right)\right)}\right| \]

   4. Taylor expanded in eh around 0

      \[\leadsto \left|\color{blue}{ew \cdot \sin t}\right| \]
   5. Step-by-step derivation

      1. lower-*.f64 N/A

         \[\leadsto \left|ew \cdot \color{blue}{\sin t}\right| \]

      2. lower-sin.f64 41.3

         \[\leadsto \left|ew \cdot \sin t\right| \]

   6. Applied rewrites 41.3%

      \[\leadsto \left|\color{blue}{ew \cdot \sin t}\right| \]
   7. Step-by-step derivation

      1. lift-*.f64 N/A

         \[\leadsto \left|ew \cdot \color{blue}{\sin t}\right| \]

      2. *-commutative N/A

         \[\leadsto \left|\sin t \cdot \color{blue}{ew}\right| \]

      3. lift-*.f64 41.3

         \[\leadsto \left|\sin t \cdot \color{blue}{ew}\right| \]

   8. Applied rewrites 41.3%

      \[\leadsto \left|\color{blue}{\sin t \cdot ew}\right| \]

   if -1.2e-111 < t < 7.2000000000000002e-167

   1. Initial program 99.8%

      \[\left|\left(ew \cdot \sin t\right) \cdot \cos \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right) + \left(eh \cdot \cos t\right) \cdot \sin \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)\right| \]

   2. Taylor expanded in t around 0

      \[\leadsto \left|\color{blue}{eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)}\right| \]
   3. Step-by-step derivation

      1. lower-*.f64 N/A

         \[\leadsto \left|eh \cdot \color{blue}{\sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)}\right| \]

      2. lower-sin.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      3. lower-atan.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      4. lower-/.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      5. lower-*.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      6. lower-cos.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      7. lower-*.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      8. lower-sin.f64 42.2

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

   4. Applied rewrites 42.2%

      \[\leadsto \left|\color{blue}{eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)}\right| \]

   6. Applied rewrites 21.0%

      \[\leadsto \color{blue}{\sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh}} \]

   8. Applied rewrites 21.7%

      \[\leadsto \color{blue}{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh} \]

   9. Taylor expanded in t around 0

      \[\leadsto \tanh \sinh^{-1} \left(\frac{eh}{ew \cdot t}\right) \cdot eh \]
   10. Step-by-step derivation

       1. lower-*.f64 20.9

          \[\leadsto \tanh \sinh^{-1} \left(\frac{eh}{ew \cdot t}\right) \cdot eh \]

   11. Applied rewrites 20.9%

       \[\leadsto \tanh \sinh^{-1} \left(\frac{eh}{ew \cdot t}\right) \cdot eh \]
3. Recombined 2 regimes into one program.
4. Add Preprocessing

Alternative 10: 28.1% accurate, 6.6× speedup

Math

\[\begin{array}{l} \\ \begin{array}{l} t_1 := \left|t \cdot \left(ew + -0.16666666666666666 \cdot \left(ew \cdot {t}^{2}\right)\right)\right|\\ \mathbf{if}\;ew \leq -2.9 \cdot 10^{+85}:\\ \;\;\;\;t\_1\\ \mathbf{elif}\;ew \leq 6.2 \cdot 10^{+50}:\\ \;\;\;\;\tanh \sinh^{-1} \left(\frac{eh}{ew \cdot t}\right) \cdot eh\\ \mathbf{else}:\\ \;\;\;\;t\_1\\ \end{array} \end{array} \]

FPCore

(FPCore (eh ew t)
 :precision binary64
 (let* ((t_1 (fabs (* t (+ ew (* -0.16666666666666666 (* ew (pow t 2.0))))))))
   (if (<= ew -2.9e+85)
     t_1
     (if (<= ew 6.2e+50) (* (tanh (asinh (/ eh (* ew t)))) eh) t_1))))

C

double code(double eh, double ew, double t) {
	double t_1 = fabs((t * (ew + (-0.16666666666666666 * (ew * pow(t, 2.0))))));
	double tmp;
	if (ew <= -2.9e+85) {
		tmp = t_1;
	} else if (ew <= 6.2e+50) {
		tmp = tanh(asinh((eh / (ew * t)))) * eh;
	} else {
		tmp = t_1;
	}
	return tmp;
}

Python

def code(eh, ew, t):
	t_1 = math.fabs((t * (ew + (-0.16666666666666666 * (ew * math.pow(t, 2.0))))))
	tmp = 0
	if ew <= -2.9e+85:
		tmp = t_1
	elif ew <= 6.2e+50:
		tmp = math.tanh(math.asinh((eh / (ew * t)))) * eh
	else:
		tmp = t_1
	return tmp

Julia

function code(eh, ew, t)
	t_1 = abs(Float64(t * Float64(ew + Float64(-0.16666666666666666 * Float64(ew * (t ^ 2.0))))))
	tmp = 0.0
	if (ew <= -2.9e+85)
		tmp = t_1;
	elseif (ew <= 6.2e+50)
		tmp = Float64(tanh(asinh(Float64(eh / Float64(ew * t)))) * eh);
	else
		tmp = t_1;
	end
	return tmp
end

MATLAB

function tmp_2 = code(eh, ew, t)
	t_1 = abs((t * (ew + (-0.16666666666666666 * (ew * (t ^ 2.0))))));
	tmp = 0.0;
	if (ew <= -2.9e+85)
		tmp = t_1;
	elseif (ew <= 6.2e+50)
		tmp = tanh(asinh((eh / (ew * t)))) * eh;
	else
		tmp = t_1;
	end
	tmp_2 = tmp;
end

Wolfram

code[eh_, ew_, t_] := Block[{t$95$1 = N[Abs[N[(t * N[(ew + N[(-0.16666666666666666 * N[(ew * N[Power[t, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]}, If[LessEqual[ew, -2.9e+85], t$95$1, If[LessEqual[ew, 6.2e+50], N[(N[Tanh[N[ArcSinh[N[(eh / N[(ew * t), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]], $MachinePrecision] * eh), $MachinePrecision], t$95$1]]]

Derivation

1. Split input into 2 regimes

2. if ew < -2.89999999999999997e85 or 6.20000000000000006e50 < ew

   1. Initial program 99.8%

      \[\left|\left(ew \cdot \sin t\right) \cdot \cos \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right) + \left(eh \cdot \cos t\right) \cdot \sin \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)\right| \]

   3. Applied rewrites 99.8%

      \[\leadsto \left|\color{blue}{\mathsf{fma}\left(\frac{\sin t}{\cosh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right)}, ew, \tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot \left(\cos t \cdot eh\right)\right)}\right| \]

   4. Taylor expanded in eh around 0

      \[\leadsto \left|\color{blue}{ew \cdot \sin t}\right| \]
   5. Step-by-step derivation

      1. lower-*.f64 N/A

         \[\leadsto \left|ew \cdot \color{blue}{\sin t}\right| \]

      2. lower-sin.f64 41.3

         \[\leadsto \left|ew \cdot \sin t\right| \]

   6. Applied rewrites 41.3%

      \[\leadsto \left|\color{blue}{ew \cdot \sin t}\right| \]

   7. Taylor expanded in t around 0

      \[\leadsto \left|t \cdot \color{blue}{\left(ew + \frac{-1}{6} \cdot \left(ew \cdot {t}^{2}\right)\right)}\right| \]
   8. Step-by-step derivation

      1. lower-*.f64 N/A

         \[\leadsto \left|t \cdot \left(ew + \color{blue}{\frac{-1}{6} \cdot \left(ew \cdot {t}^{2}\right)}\right)\right| \]

      2. lower-+.f64 N/A

         \[\leadsto \left|t \cdot \left(ew + \frac{-1}{6} \cdot \color{blue}{\left(ew \cdot {t}^{2}\right)}\right)\right| \]

      3. lower-*.f64 N/A

         \[\leadsto \left|t \cdot \left(ew + \frac{-1}{6} \cdot \left(ew \cdot \color{blue}{{t}^{2}}\right)\right)\right| \]

      4. lower-*.f64 N/A

         \[\leadsto \left|t \cdot \left(ew + \frac{-1}{6} \cdot \left(ew \cdot {t}^{\color{blue}{2}}\right)\right)\right| \]

      5. lower-pow.f64 18.5

         \[\leadsto \left|t \cdot \left(ew + -0.16666666666666666 \cdot \left(ew \cdot {t}^{2}\right)\right)\right| \]

   9. Applied rewrites 18.5%

      \[\leadsto \left|t \cdot \color{blue}{\left(ew + -0.16666666666666666 \cdot \left(ew \cdot {t}^{2}\right)\right)}\right| \]

   if -2.89999999999999997e85 < ew < 6.20000000000000006e50

   1. Initial program 99.8%

      \[\left|\left(ew \cdot \sin t\right) \cdot \cos \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right) + \left(eh \cdot \cos t\right) \cdot \sin \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)\right| \]

   2. Taylor expanded in t around 0

      \[\leadsto \left|\color{blue}{eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)}\right| \]
   3. Step-by-step derivation

      1. lower-*.f64 N/A

         \[\leadsto \left|eh \cdot \color{blue}{\sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)}\right| \]

      2. lower-sin.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      3. lower-atan.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      4. lower-/.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      5. lower-*.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      6. lower-cos.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      7. lower-*.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      8. lower-sin.f64 42.2

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

   4. Applied rewrites 42.2%

      \[\leadsto \left|\color{blue}{eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)}\right| \]

   6. Applied rewrites 21.0%

      \[\leadsto \color{blue}{\sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh}} \]

   8. Applied rewrites 21.7%

      \[\leadsto \color{blue}{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh} \]

   9. Taylor expanded in t around 0

      \[\leadsto \tanh \sinh^{-1} \left(\frac{eh}{ew \cdot t}\right) \cdot eh \]
   10. Step-by-step derivation

       1. lower-*.f64 20.9

          \[\leadsto \tanh \sinh^{-1} \left(\frac{eh}{ew \cdot t}\right) \cdot eh \]

   11. Applied rewrites 20.9%

       \[\leadsto \tanh \sinh^{-1} \left(\frac{eh}{ew \cdot t}\right) \cdot eh \]
3. Recombined 2 regimes into one program.
4. Add Preprocessing

Alternative 11: 26.7% accurate, 7.1× speedup

Math

\[\begin{array}{l} \\ \begin{array}{l} t_1 := \tanh \sinh^{-1} \left(\frac{eh}{ew \cdot t}\right) \cdot eh\\ \mathbf{if}\;eh \leq -2.8 \cdot 10^{-127}:\\ \;\;\;\;t\_1\\ \mathbf{elif}\;eh \leq 1.15 \cdot 10^{+86}:\\ \;\;\;\;\left|ew \cdot t\right|\\ \mathbf{else}:\\ \;\;\;\;t\_1\\ \end{array} \end{array} \]

FPCore

(FPCore (eh ew t)
 :precision binary64
 (let* ((t_1 (* (tanh (asinh (/ eh (* ew t)))) eh)))
   (if (<= eh -2.8e-127) t_1 (if (<= eh 1.15e+86) (fabs (* ew t)) t_1))))

C

double code(double eh, double ew, double t) {
	double t_1 = tanh(asinh((eh / (ew * t)))) * eh;
	double tmp;
	if (eh <= -2.8e-127) {
		tmp = t_1;
	} else if (eh <= 1.15e+86) {
		tmp = fabs((ew * t));
	} else {
		tmp = t_1;
	}
	return tmp;
}

Python

def code(eh, ew, t):
	t_1 = math.tanh(math.asinh((eh / (ew * t)))) * eh
	tmp = 0
	if eh <= -2.8e-127:
		tmp = t_1
	elif eh <= 1.15e+86:
		tmp = math.fabs((ew * t))
	else:
		tmp = t_1
	return tmp

Julia

function code(eh, ew, t)
	t_1 = Float64(tanh(asinh(Float64(eh / Float64(ew * t)))) * eh)
	tmp = 0.0
	if (eh <= -2.8e-127)
		tmp = t_1;
	elseif (eh <= 1.15e+86)
		tmp = abs(Float64(ew * t));
	else
		tmp = t_1;
	end
	return tmp
end

MATLAB

function tmp_2 = code(eh, ew, t)
	t_1 = tanh(asinh((eh / (ew * t)))) * eh;
	tmp = 0.0;
	if (eh <= -2.8e-127)
		tmp = t_1;
	elseif (eh <= 1.15e+86)
		tmp = abs((ew * t));
	else
		tmp = t_1;
	end
	tmp_2 = tmp;
end

Wolfram

code[eh_, ew_, t_] := Block[{t$95$1 = N[(N[Tanh[N[ArcSinh[N[(eh / N[(ew * t), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]], $MachinePrecision] * eh), $MachinePrecision]}, If[LessEqual[eh, -2.8e-127], t$95$1, If[LessEqual[eh, 1.15e+86], N[Abs[N[(ew * t), $MachinePrecision]], $MachinePrecision], t$95$1]]]

Derivation

1. Split input into 2 regimes

2. if eh < -2.8e-127 or 1.14999999999999995e86 < eh

   1. Initial program 99.8%

      \[\left|\left(ew \cdot \sin t\right) \cdot \cos \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right) + \left(eh \cdot \cos t\right) \cdot \sin \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)\right| \]

   2. Taylor expanded in t around 0

      \[\leadsto \left|\color{blue}{eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)}\right| \]
   3. Step-by-step derivation

      1. lower-*.f64 N/A

         \[\leadsto \left|eh \cdot \color{blue}{\sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)}\right| \]

      2. lower-sin.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      3. lower-atan.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      4. lower-/.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      5. lower-*.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      6. lower-cos.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      7. lower-*.f64 N/A

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

      8. lower-sin.f64 42.2

         \[\leadsto \left|eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)\right| \]

   4. Applied rewrites 42.2%

      \[\leadsto \left|\color{blue}{eh \cdot \sin \tan^{-1} \left(\frac{eh \cdot \cos t}{ew \cdot \sin t}\right)}\right| \]

   6. Applied rewrites 21.0%

      \[\leadsto \color{blue}{\sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh} \cdot \sqrt{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh}} \]

   8. Applied rewrites 21.7%

      \[\leadsto \color{blue}{\tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot eh} \]

   9. Taylor expanded in t around 0

      \[\leadsto \tanh \sinh^{-1} \left(\frac{eh}{ew \cdot t}\right) \cdot eh \]
   10. Step-by-step derivation

       1. lower-*.f64 20.9

          \[\leadsto \tanh \sinh^{-1} \left(\frac{eh}{ew \cdot t}\right) \cdot eh \]

   11. Applied rewrites 20.9%

       \[\leadsto \tanh \sinh^{-1} \left(\frac{eh}{ew \cdot t}\right) \cdot eh \]

   if -2.8e-127 < eh < 1.14999999999999995e86

   1. Initial program 99.8%

      \[\left|\left(ew \cdot \sin t\right) \cdot \cos \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right) + \left(eh \cdot \cos t\right) \cdot \sin \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)\right| \]

   3. Applied rewrites 99.8%

      \[\leadsto \left|\color{blue}{\mathsf{fma}\left(\frac{\sin t}{\cosh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right)}, ew, \tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot \left(\cos t \cdot eh\right)\right)}\right| \]

   4. Taylor expanded in eh around 0

      \[\leadsto \left|\color{blue}{ew \cdot \sin t}\right| \]
   5. Step-by-step derivation

      1. lower-*.f64 N/A

         \[\leadsto \left|ew \cdot \color{blue}{\sin t}\right| \]

      2. lower-sin.f64 41.3

         \[\leadsto \left|ew \cdot \sin t\right| \]

   6. Applied rewrites 41.3%

      \[\leadsto \left|\color{blue}{ew \cdot \sin t}\right| \]

   7. Taylor expanded in t around 0

      \[\leadsto \left|ew \cdot t\right| \]
   8. Step-by-step derivation

   9. Applied rewrites 18.8%

      \[\leadsto \left|ew \cdot t\right| \]
3. Recombined 2 regimes into one program.
4. Add Preprocessing

Alternative 12: 18.8% accurate, 47.8× speedup

Math

\[\begin{array}{l} \\ \left|ew \cdot t\right| \end{array} \]

FPCore

(FPCore (eh ew t) :precision binary64 (fabs (* ew t)))

C

double code(double eh, double ew, double t) {
	return fabs((ew * t));
}

Fortran

module fmin_fmax_functions
    implicit none
    private
    public fmax
    public fmin

    interface fmax
        module procedure fmax88
        module procedure fmax44
        module procedure fmax84
        module procedure fmax48
    end interface
    interface fmin
        module procedure fmin88
        module procedure fmin44
        module procedure fmin84
        module procedure fmin48
    end interface
contains
    real(8) function fmax88(x, y) result (res)
        real(8), intent (in) :: x
        real(8), intent (in) :: y
        res = merge(y, merge(x, max(x, y), y /= y), x /= x)
    end function
    real(4) function fmax44(x, y) result (res)
        real(4), intent (in) :: x
        real(4), intent (in) :: y
        res = merge(y, merge(x, max(x, y), y /= y), x /= x)
    end function
    real(8) function fmax84(x, y) result(res)
        real(8), intent (in) :: x
        real(4), intent (in) :: y
        res = merge(dble(y), merge(x, max(x, dble(y)), y /= y), x /= x)
    end function
    real(8) function fmax48(x, y) result(res)
        real(4), intent (in) :: x
        real(8), intent (in) :: y
        res = merge(y, merge(dble(x), max(dble(x), y), y /= y), x /= x)
    end function
    real(8) function fmin88(x, y) result (res)
        real(8), intent (in) :: x
        real(8), intent (in) :: y
        res = merge(y, merge(x, min(x, y), y /= y), x /= x)
    end function
    real(4) function fmin44(x, y) result (res)
        real(4), intent (in) :: x
        real(4), intent (in) :: y
        res = merge(y, merge(x, min(x, y), y /= y), x /= x)
    end function
    real(8) function fmin84(x, y) result(res)
        real(8), intent (in) :: x
        real(4), intent (in) :: y
        res = merge(dble(y), merge(x, min(x, dble(y)), y /= y), x /= x)
    end function
    real(8) function fmin48(x, y) result(res)
        real(4), intent (in) :: x
        real(8), intent (in) :: y
        res = merge(y, merge(dble(x), min(dble(x), y), y /= y), x /= x)
    end function
end module

real(8) function code(eh, ew, t)
use fmin_fmax_functions
    real(8), intent (in) :: eh
    real(8), intent (in) :: ew
    real(8), intent (in) :: t
    code = abs((ew * t))
end function

Java

public static double code(double eh, double ew, double t) {
	return Math.abs((ew * t));
}

Python

def code(eh, ew, t):
	return math.fabs((ew * t))

Julia

function code(eh, ew, t)
	return abs(Float64(ew * t))
end

MATLAB

function tmp = code(eh, ew, t)
	tmp = abs((ew * t));
end

Wolfram

code[eh_, ew_, t_] := N[Abs[N[(ew * t), $MachinePrecision]], $MachinePrecision]

Derivation

1. Initial program 99.8%

   \[\left|\left(ew \cdot \sin t\right) \cdot \cos \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right) + \left(eh \cdot \cos t\right) \cdot \sin \tan^{-1} \left(\frac{\frac{eh}{ew}}{\tan t}\right)\right| \]

3. Applied rewrites 99.8%

   \[\leadsto \left|\color{blue}{\mathsf{fma}\left(\frac{\sin t}{\cosh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right)}, ew, \tanh \sinh^{-1} \left(\frac{eh}{\tan t \cdot ew}\right) \cdot \left(\cos t \cdot eh\right)\right)}\right| \]

4. Taylor expanded in eh around 0

   \[\leadsto \left|\color{blue}{ew \cdot \sin t}\right| \]
5. Step-by-step derivation

   1. lower-*.f64 N/A

      \[\leadsto \left|ew \cdot \color{blue}{\sin t}\right| \]

   2. lower-sin.f64 41.3

      \[\leadsto \left|ew \cdot \sin t\right| \]

6. Applied rewrites 41.3%

   \[\leadsto \left|\color{blue}{ew \cdot \sin t}\right| \]

7. Taylor expanded in t around 0

   \[\leadsto \left|ew \cdot t\right| \]
8. Step-by-step derivation

9. Applied rewrites 18.8%

   \[\leadsto \left|ew \cdot t\right| \]
10. Add Preprocessing

Reproduce

herbie shell --seed 2025162 
(FPCore (eh ew t)
  :name "Example from Robby"
  :precision binary64
  (fabs (+ (* (* ew (sin t)) (cos (atan (/ (/ eh ew) (tan t))))) (* (* eh (cos t)) (sin (atan (/ (/ eh ew) (tan t))))))))