Example from Robby

Percentage Accurate: 99.8% → 99.8%

Time: 24.7s

Alternatives: 13

Speedup: 1.0×

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, 1.0× 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]]

Derivation

1. Initial program 99.8%

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

Alternative 2: 99.8% accurate, 1.2× speedup

Math

\[\begin{array}{l} \\ \begin{array}{l} t_1 := \frac{eh}{ew \cdot \tan t}\\ \left|\mathsf{fma}\left(\tanh \sinh^{-1} t\_1 \cdot \cos t, eh, \frac{1}{\sqrt{1 + {t\_1}^{2}}} \cdot \left(\sin t \cdot ew\right)\right)\right| \end{array} \end{array} \]

FPCore

(FPCore (eh ew t)
 :precision binary64
 (let* ((t_1 (/ eh (* ew (tan t)))))
   (fabs
    (fma
     (* (tanh (asinh t_1)) (cos t))
     eh
     (* (/ 1.0 (sqrt (+ 1.0 (pow t_1 2.0)))) (* (sin t) ew))))))

C

double code(double eh, double ew, double t) {
	double t_1 = eh / (ew * tan(t));
	return fabs(fma((tanh(asinh(t_1)) * cos(t)), eh, ((1.0 / sqrt((1.0 + pow(t_1, 2.0)))) * (sin(t) * ew))));
}

Julia

function code(eh, ew, t)
	t_1 = Float64(eh / Float64(ew * tan(t)))
	return abs(fma(Float64(tanh(asinh(t_1)) * cos(t)), eh, Float64(Float64(1.0 / sqrt(Float64(1.0 + (t_1 ^ 2.0)))) * Float64(sin(t) * ew))))
end

Wolfram

code[eh_, ew_, t_] := Block[{t$95$1 = N[(eh / N[(ew * N[Tan[t], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]}, N[Abs[N[(N[(N[Tanh[N[ArcSinh[t$95$1], $MachinePrecision]], $MachinePrecision] * N[Cos[t], $MachinePrecision]), $MachinePrecision] * eh + N[(N[(1.0 / N[Sqrt[N[(1.0 + N[Power[t$95$1, 2.0], $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision] * N[(N[Sin[t], $MachinePrecision] * ew), $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%

   \[\leadsto \left|\color{blue}{\mathsf{fma}\left(\tanh \sinh^{-1} \left(\frac{eh}{ew \cdot \tan t}\right) \cdot \cos t, eh, \frac{1}{\sqrt{1 + {\left(\frac{eh}{ew \cdot \tan t}\right)}^{2}}} \cdot \left(\sin t \cdot ew\right)\right)}\right| \]
4. Add Preprocessing

Alternative 3: 98.5% accurate, 1.8× speedup

Math

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

FPCore

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

C

double code(double eh, double ew, double t) {
	return fabs(fma((tanh(asinh((eh / (ew * tan(t))))) * cos(t)), eh, (1.0 * (sin(t) * ew))));
}

Julia

function code(eh, ew, t)
	return abs(fma(Float64(tanh(asinh(Float64(eh / Float64(ew * tan(t))))) * cos(t)), eh, Float64(1.0 * Float64(sin(t) * ew))))
end

Wolfram

code[eh_, ew_, t_] := N[Abs[N[(N[(N[Tanh[N[ArcSinh[N[(eh / N[(ew * N[Tan[t], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]], $MachinePrecision] * N[Cos[t], $MachinePrecision]), $MachinePrecision] * eh + N[(1.0 * N[(N[Sin[t], $MachinePrecision] * ew), $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%

   \[\leadsto \left|\color{blue}{\mathsf{fma}\left(\tanh \sinh^{-1} \left(\frac{eh}{ew \cdot \tan t}\right) \cdot \cos t, eh, \frac{1}{\sqrt{1 + {\left(\frac{eh}{ew \cdot \tan t}\right)}^{2}}} \cdot \left(\sin t \cdot ew\right)\right)}\right| \]

4. Taylor expanded in eh around 0

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

6. Applied rewrites 98.5%

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

Alternative 4: 89.8% accurate, 1.8× speedup

Math

\[\begin{array}{l} \\ \begin{array}{l} t_1 := \sin t \cdot ew\\ t_2 := \frac{eh}{ew \cdot t}\\ \mathbf{if}\;t \leq 1.32 \cdot 10^{+157}:\\ \;\;\;\;\left|\mathsf{fma}\left(\tanh \sinh^{-1} t\_2 \cdot \cos t, eh, \frac{1}{\sqrt{1 + {t\_2}^{2}}} \cdot t\_1\right)\right|\\ \mathbf{else}:\\ \;\;\;\;\left|\mathsf{fma}\left(\tanh \left(\log \left(\sqrt{\frac{eh \cdot eh}{ew \cdot ew}} + \frac{eh}{ew}\right) + -1 \cdot \log t\right) \cdot \cos t, eh, 1 \cdot t\_1\right)\right|\\ \end{array} \end{array} \]

FPCore

(FPCore (eh ew t)
 :precision binary64
 (let* ((t_1 (* (sin t) ew)) (t_2 (/ eh (* ew t))))
   (if (<= t 1.32e+157)
     (fabs
      (fma
       (* (tanh (asinh t_2)) (cos t))
       eh
       (* (/ 1.0 (sqrt (+ 1.0 (pow t_2 2.0)))) t_1)))
     (fabs
      (fma
       (*
        (tanh
         (+
          (log (+ (sqrt (/ (* eh eh) (* ew ew))) (/ eh ew)))
          (* -1.0 (log t))))
        (cos t))
       eh
       (* 1.0 t_1))))))

C

double code(double eh, double ew, double t) {
	double t_1 = sin(t) * ew;
	double t_2 = eh / (ew * t);
	double tmp;
	if (t <= 1.32e+157) {
		tmp = fabs(fma((tanh(asinh(t_2)) * cos(t)), eh, ((1.0 / sqrt((1.0 + pow(t_2, 2.0)))) * t_1)));
	} else {
		tmp = fabs(fma((tanh((log((sqrt(((eh * eh) / (ew * ew))) + (eh / ew))) + (-1.0 * log(t)))) * cos(t)), eh, (1.0 * t_1)));
	}
	return tmp;
}

Julia

function code(eh, ew, t)
	t_1 = Float64(sin(t) * ew)
	t_2 = Float64(eh / Float64(ew * t))
	tmp = 0.0
	if (t <= 1.32e+157)
		tmp = abs(fma(Float64(tanh(asinh(t_2)) * cos(t)), eh, Float64(Float64(1.0 / sqrt(Float64(1.0 + (t_2 ^ 2.0)))) * t_1)));
	else
		tmp = abs(fma(Float64(tanh(Float64(log(Float64(sqrt(Float64(Float64(eh * eh) / Float64(ew * ew))) + Float64(eh / ew))) + Float64(-1.0 * log(t)))) * cos(t)), eh, Float64(1.0 * t_1)));
	end
	return tmp
end

Wolfram

code[eh_, ew_, t_] := Block[{t$95$1 = N[(N[Sin[t], $MachinePrecision] * ew), $MachinePrecision]}, Block[{t$95$2 = N[(eh / N[(ew * t), $MachinePrecision]), $MachinePrecision]}, If[LessEqual[t, 1.32e+157], N[Abs[N[(N[(N[Tanh[N[ArcSinh[t$95$2], $MachinePrecision]], $MachinePrecision] * N[Cos[t], $MachinePrecision]), $MachinePrecision] * eh + N[(N[(1.0 / N[Sqrt[N[(1.0 + N[Power[t$95$2, 2.0], $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision] * t$95$1), $MachinePrecision]), $MachinePrecision]], $MachinePrecision], N[Abs[N[(N[(N[Tanh[N[(N[Log[N[(N[Sqrt[N[(N[(eh * eh), $MachinePrecision] / N[(ew * ew), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] + N[(eh / ew), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] + N[(-1.0 * N[Log[t], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] * N[Cos[t], $MachinePrecision]), $MachinePrecision] * eh + N[(1.0 * t$95$1), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]]]]

Derivation

1. Split input into 2 regimes

2. if t < 1.3199999999999999e157

   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%

      \[\leadsto \left|\color{blue}{\mathsf{fma}\left(\tanh \sinh^{-1} \left(\frac{eh}{ew \cdot \tan t}\right) \cdot \cos t, eh, \frac{1}{\sqrt{1 + {\left(\frac{eh}{ew \cdot \tan t}\right)}^{2}}} \cdot \left(\sin t \cdot ew\right)\right)}\right| \]

   4. Taylor expanded in t around 0

      \[\leadsto \left|\mathsf{fma}\left(\tanh \sinh^{-1} \left(\frac{eh}{ew \cdot \color{blue}{t}}\right) \cdot \cos t, eh, \frac{1}{\sqrt{1 + {\left(\frac{eh}{ew \cdot \tan t}\right)}^{2}}} \cdot \left(\sin t \cdot ew\right)\right)\right| \]
   5. Step-by-step derivation

   6. Applied rewrites 89.5%

      \[\leadsto \left|\mathsf{fma}\left(\tanh \sinh^{-1} \left(\frac{eh}{ew \cdot \color{blue}{t}}\right) \cdot \cos t, eh, \frac{1}{\sqrt{1 + {\left(\frac{eh}{ew \cdot \tan t}\right)}^{2}}} \cdot \left(\sin t \cdot ew\right)\right)\right| \]

   7. Taylor expanded in t around 0

      \[\leadsto \left|\mathsf{fma}\left(\tanh \sinh^{-1} \left(\frac{eh}{ew \cdot t}\right) \cdot \cos t, eh, \frac{1}{\sqrt{1 + {\left(\frac{eh}{ew \cdot \color{blue}{t}}\right)}^{2}}} \cdot \left(\sin t \cdot ew\right)\right)\right| \]
   8. Step-by-step derivation

   9. Applied rewrites 89.6%

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

   if 1.3199999999999999e157 < 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%

      \[\leadsto \left|\color{blue}{\mathsf{fma}\left(\tanh \sinh^{-1} \left(\frac{eh}{ew \cdot \tan t}\right) \cdot \cos t, eh, \frac{1}{\sqrt{1 + {\left(\frac{eh}{ew \cdot \tan t}\right)}^{2}}} \cdot \left(\sin t \cdot ew\right)\right)}\right| \]

   4. Taylor expanded in eh around 0

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

   6. Applied rewrites 98.5%

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

   7. Taylor expanded in t around 0

      \[\leadsto \left|\mathsf{fma}\left(\tanh \color{blue}{\left(\log \left(\sqrt{\frac{{eh}^{2}}{{ew}^{2}}} + \frac{eh}{ew}\right) + -1 \cdot \log t\right)} \cdot \cos t, eh, 1 \cdot \left(\sin t \cdot ew\right)\right)\right| \]
   8. Step-by-step derivation

      1. lower-+.f64 N/A

         \[\leadsto \left|\mathsf{fma}\left(\tanh \left(\log \left(\sqrt{\frac{{eh}^{2}}{{ew}^{2}}} + \frac{eh}{ew}\right) + \color{blue}{-1 \cdot \log t}\right) \cdot \cos t, eh, 1 \cdot \left(\sin t \cdot ew\right)\right)\right| \]

      2. lower-log.f64 N/A

         \[\leadsto \left|\mathsf{fma}\left(\tanh \left(\log \left(\sqrt{\frac{{eh}^{2}}{{ew}^{2}}} + \frac{eh}{ew}\right) + \color{blue}{-1} \cdot \log t\right) \cdot \cos t, eh, 1 \cdot \left(\sin t \cdot ew\right)\right)\right| \]

      3. lower-+.f64 N/A

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

      4. lower-sqrt.f64 N/A

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

      5. lower-/.f64 N/A

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

      6. unpow2 N/A

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

      7. lower-*.f64 N/A

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

      8. unpow2 N/A

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

      9. lower-*.f64 N/A

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

      10. lift-/.f64 N/A

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

      11. lower-*.f64 N/A

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

      12. lower-log.f64 34.1

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

   9. Applied rewrites 34.1%

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

Alternative 5: 89.8% accurate, 1.9× speedup

Math

\[\begin{array}{l} \\ \begin{array}{l} t_1 := \frac{eh}{t \cdot ew}\\ \mathbf{if}\;t \leq 1.32 \cdot 10^{+157}:\\ \;\;\;\;\left|\mathsf{fma}\left(ew \cdot \sin t, \frac{1}{\sqrt{1 + t\_1 \cdot t\_1}}, \left(eh \cdot \cos t\right) \cdot \tanh \sinh^{-1} t\_1\right)\right|\\ \mathbf{else}:\\ \;\;\;\;\left|\mathsf{fma}\left(\tanh \left(\log \left(\sqrt{\frac{eh \cdot eh}{ew \cdot ew}} + \frac{eh}{ew}\right) + -1 \cdot \log t\right) \cdot \cos t, eh, 1 \cdot \left(\sin t \cdot ew\right)\right)\right|\\ \end{array} \end{array} \]

FPCore

(FPCore (eh ew t)
 :precision binary64
 (let* ((t_1 (/ eh (* t ew))))
   (if (<= t 1.32e+157)
     (fabs
      (fma
       (* ew (sin t))
       (/ 1.0 (sqrt (+ 1.0 (* t_1 t_1))))
       (* (* eh (cos t)) (tanh (asinh t_1)))))
     (fabs
      (fma
       (*
        (tanh
         (+
          (log (+ (sqrt (/ (* eh eh) (* ew ew))) (/ eh ew)))
          (* -1.0 (log t))))
        (cos t))
       eh
       (* 1.0 (* (sin t) ew)))))))

C

double code(double eh, double ew, double t) {
	double t_1 = eh / (t * ew);
	double tmp;
	if (t <= 1.32e+157) {
		tmp = fabs(fma((ew * sin(t)), (1.0 / sqrt((1.0 + (t_1 * t_1)))), ((eh * cos(t)) * tanh(asinh(t_1)))));
	} else {
		tmp = fabs(fma((tanh((log((sqrt(((eh * eh) / (ew * ew))) + (eh / ew))) + (-1.0 * log(t)))) * cos(t)), eh, (1.0 * (sin(t) * ew))));
	}
	return tmp;
}

Julia

function code(eh, ew, t)
	t_1 = Float64(eh / Float64(t * ew))
	tmp = 0.0
	if (t <= 1.32e+157)
		tmp = abs(fma(Float64(ew * sin(t)), Float64(1.0 / sqrt(Float64(1.0 + Float64(t_1 * t_1)))), Float64(Float64(eh * cos(t)) * tanh(asinh(t_1)))));
	else
		tmp = abs(fma(Float64(tanh(Float64(log(Float64(sqrt(Float64(Float64(eh * eh) / Float64(ew * ew))) + Float64(eh / ew))) + Float64(-1.0 * log(t)))) * cos(t)), eh, Float64(1.0 * Float64(sin(t) * ew))));
	end
	return tmp
end

Wolfram

code[eh_, ew_, t_] := Block[{t$95$1 = N[(eh / N[(t * ew), $MachinePrecision]), $MachinePrecision]}, If[LessEqual[t, 1.32e+157], N[Abs[N[(N[(ew * N[Sin[t], $MachinePrecision]), $MachinePrecision] * N[(1.0 / N[Sqrt[N[(1.0 + N[(t$95$1 * t$95$1), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision] + N[(N[(eh * N[Cos[t], $MachinePrecision]), $MachinePrecision] * N[Tanh[N[ArcSinh[t$95$1], $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision], N[Abs[N[(N[(N[Tanh[N[(N[Log[N[(N[Sqrt[N[(N[(eh * eh), $MachinePrecision] / N[(ew * ew), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] + N[(eh / ew), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] + N[(-1.0 * N[Log[t], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] * N[Cos[t], $MachinePrecision]), $MachinePrecision] * eh + N[(1.0 * N[(N[Sin[t], $MachinePrecision] * ew), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]]]

Derivation

1. Split input into 2 regimes

2. if t < 1.3199999999999999e157

   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

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

      1. lower-/.f64 N/A

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

      2. *-commutative N/A

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

      3. lower-*.f64 99.0

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

   4. Applied rewrites 99.0%

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

   5. Taylor expanded in t around 0

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

      1. lower-/.f64 N/A

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

      2. *-commutative N/A

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

      3. lower-*.f64 89.6

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

   7. Applied rewrites 89.6%

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

      1. lift-+.f64 N/A

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

      2. lift-*.f64 N/A

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

      3. lift-*.f64 N/A

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

      4. lift-sin.f64 N/A

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

      5. lower-fma.f64 N/A

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

   9. Applied rewrites 56.7%

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

       1. lift-/.f64 N/A

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

       2. lift-sqrt.f64 N/A

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

       3. lift-+.f64 N/A

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

       4. lift-*.f64 N/A

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

       5. tanh-asinh-rev N/A

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

       6. lower-tanh.f64 N/A

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

       7. lower-asinh.f64 89.6

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

   11. Applied rewrites 89.6%

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

   if 1.3199999999999999e157 < 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%

      \[\leadsto \left|\color{blue}{\mathsf{fma}\left(\tanh \sinh^{-1} \left(\frac{eh}{ew \cdot \tan t}\right) \cdot \cos t, eh, \frac{1}{\sqrt{1 + {\left(\frac{eh}{ew \cdot \tan t}\right)}^{2}}} \cdot \left(\sin t \cdot ew\right)\right)}\right| \]

   4. Taylor expanded in eh around 0

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

   6. Applied rewrites 98.5%

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

   7. Taylor expanded in t around 0

      \[\leadsto \left|\mathsf{fma}\left(\tanh \color{blue}{\left(\log \left(\sqrt{\frac{{eh}^{2}}{{ew}^{2}}} + \frac{eh}{ew}\right) + -1 \cdot \log t\right)} \cdot \cos t, eh, 1 \cdot \left(\sin t \cdot ew\right)\right)\right| \]
   8. Step-by-step derivation

      1. lower-+.f64 N/A

         \[\leadsto \left|\mathsf{fma}\left(\tanh \left(\log \left(\sqrt{\frac{{eh}^{2}}{{ew}^{2}}} + \frac{eh}{ew}\right) + \color{blue}{-1 \cdot \log t}\right) \cdot \cos t, eh, 1 \cdot \left(\sin t \cdot ew\right)\right)\right| \]

      2. lower-log.f64 N/A

         \[\leadsto \left|\mathsf{fma}\left(\tanh \left(\log \left(\sqrt{\frac{{eh}^{2}}{{ew}^{2}}} + \frac{eh}{ew}\right) + \color{blue}{-1} \cdot \log t\right) \cdot \cos t, eh, 1 \cdot \left(\sin t \cdot ew\right)\right)\right| \]

      3. lower-+.f64 N/A

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

      4. lower-sqrt.f64 N/A

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

      5. lower-/.f64 N/A

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

      6. unpow2 N/A

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

      7. lower-*.f64 N/A

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

      8. unpow2 N/A

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

      9. lower-*.f64 N/A

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

      10. lift-/.f64 N/A

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

      11. lower-*.f64 N/A

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

      12. lower-log.f64 34.1

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

   9. Applied rewrites 34.1%

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

Alternative 6: 89.3% accurate, 2.0× speedup

Math

\[\begin{array}{l} \\ \begin{array}{l} t_1 := 1 \cdot \left(\sin t \cdot ew\right)\\ \mathbf{if}\;t \leq 1.32 \cdot 10^{+157}:\\ \;\;\;\;\left|\mathsf{fma}\left(\tanh \sinh^{-1} \left(\frac{eh}{ew \cdot t}\right) \cdot \cos t, eh, t\_1\right)\right|\\ \mathbf{else}:\\ \;\;\;\;\left|\mathsf{fma}\left(\tanh \left(\log \left(\sqrt{\frac{eh \cdot eh}{ew \cdot ew}} + \frac{eh}{ew}\right) + -1 \cdot \log t\right) \cdot \cos t, eh, t\_1\right)\right|\\ \end{array} \end{array} \]

FPCore

(FPCore (eh ew t)
 :precision binary64
 (let* ((t_1 (* 1.0 (* (sin t) ew))))
   (if (<= t 1.32e+157)
     (fabs (fma (* (tanh (asinh (/ eh (* ew t)))) (cos t)) eh t_1))
     (fabs
      (fma
       (*
        (tanh
         (+
          (log (+ (sqrt (/ (* eh eh) (* ew ew))) (/ eh ew)))
          (* -1.0 (log t))))
        (cos t))
       eh
       t_1)))))

C

double code(double eh, double ew, double t) {
	double t_1 = 1.0 * (sin(t) * ew);
	double tmp;
	if (t <= 1.32e+157) {
		tmp = fabs(fma((tanh(asinh((eh / (ew * t)))) * cos(t)), eh, t_1));
	} else {
		tmp = fabs(fma((tanh((log((sqrt(((eh * eh) / (ew * ew))) + (eh / ew))) + (-1.0 * log(t)))) * cos(t)), eh, t_1));
	}
	return tmp;
}

Julia

function code(eh, ew, t)
	t_1 = Float64(1.0 * Float64(sin(t) * ew))
	tmp = 0.0
	if (t <= 1.32e+157)
		tmp = abs(fma(Float64(tanh(asinh(Float64(eh / Float64(ew * t)))) * cos(t)), eh, t_1));
	else
		tmp = abs(fma(Float64(tanh(Float64(log(Float64(sqrt(Float64(Float64(eh * eh) / Float64(ew * ew))) + Float64(eh / ew))) + Float64(-1.0 * log(t)))) * cos(t)), eh, t_1));
	end
	return tmp
end

Wolfram

code[eh_, ew_, t_] := Block[{t$95$1 = N[(1.0 * N[(N[Sin[t], $MachinePrecision] * ew), $MachinePrecision]), $MachinePrecision]}, If[LessEqual[t, 1.32e+157], N[Abs[N[(N[(N[Tanh[N[ArcSinh[N[(eh / N[(ew * t), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]], $MachinePrecision] * N[Cos[t], $MachinePrecision]), $MachinePrecision] * eh + t$95$1), $MachinePrecision]], $MachinePrecision], N[Abs[N[(N[(N[Tanh[N[(N[Log[N[(N[Sqrt[N[(N[(eh * eh), $MachinePrecision] / N[(ew * ew), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] + N[(eh / ew), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] + N[(-1.0 * N[Log[t], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] * N[Cos[t], $MachinePrecision]), $MachinePrecision] * eh + t$95$1), $MachinePrecision]], $MachinePrecision]]]

Derivation

1. Split input into 2 regimes

2. if t < 1.3199999999999999e157

   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%

      \[\leadsto \left|\color{blue}{\mathsf{fma}\left(\tanh \sinh^{-1} \left(\frac{eh}{ew \cdot \tan t}\right) \cdot \cos t, eh, \frac{1}{\sqrt{1 + {\left(\frac{eh}{ew \cdot \tan t}\right)}^{2}}} \cdot \left(\sin t \cdot ew\right)\right)}\right| \]

   4. Taylor expanded in eh around 0

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

   6. Applied rewrites 98.5%

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

   7. Taylor expanded in t around 0

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

   9. Applied rewrites 89.0%

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

   if 1.3199999999999999e157 < 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%

      \[\leadsto \left|\color{blue}{\mathsf{fma}\left(\tanh \sinh^{-1} \left(\frac{eh}{ew \cdot \tan t}\right) \cdot \cos t, eh, \frac{1}{\sqrt{1 + {\left(\frac{eh}{ew \cdot \tan t}\right)}^{2}}} \cdot \left(\sin t \cdot ew\right)\right)}\right| \]

   4. Taylor expanded in eh around 0

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

   6. Applied rewrites 98.5%

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

   7. Taylor expanded in t around 0

      \[\leadsto \left|\mathsf{fma}\left(\tanh \color{blue}{\left(\log \left(\sqrt{\frac{{eh}^{2}}{{ew}^{2}}} + \frac{eh}{ew}\right) + -1 \cdot \log t\right)} \cdot \cos t, eh, 1 \cdot \left(\sin t \cdot ew\right)\right)\right| \]
   8. Step-by-step derivation

      1. lower-+.f64 N/A

         \[\leadsto \left|\mathsf{fma}\left(\tanh \left(\log \left(\sqrt{\frac{{eh}^{2}}{{ew}^{2}}} + \frac{eh}{ew}\right) + \color{blue}{-1 \cdot \log t}\right) \cdot \cos t, eh, 1 \cdot \left(\sin t \cdot ew\right)\right)\right| \]

      2. lower-log.f64 N/A

         \[\leadsto \left|\mathsf{fma}\left(\tanh \left(\log \left(\sqrt{\frac{{eh}^{2}}{{ew}^{2}}} + \frac{eh}{ew}\right) + \color{blue}{-1} \cdot \log t\right) \cdot \cos t, eh, 1 \cdot \left(\sin t \cdot ew\right)\right)\right| \]

      3. lower-+.f64 N/A

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

      4. lower-sqrt.f64 N/A

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

      5. lower-/.f64 N/A

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

      6. unpow2 N/A

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

      7. lower-*.f64 N/A

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

      8. unpow2 N/A

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

      9. lower-*.f64 N/A

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

      10. lift-/.f64 N/A

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

      11. lower-*.f64 N/A

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

      12. lower-log.f64 34.1

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

   9. Applied rewrites 34.1%

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

Alternative 7: 89.0% accurate, 2.4× speedup

Math

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

FPCore

(FPCore (eh ew t)
 :precision binary64
 (fabs
  (fma (* (tanh (asinh (/ eh (* ew t)))) (cos t)) eh (* 1.0 (* (sin t) ew)))))

C

double code(double eh, double ew, double t) {
	return fabs(fma((tanh(asinh((eh / (ew * t)))) * cos(t)), eh, (1.0 * (sin(t) * ew))));
}

Julia

function code(eh, ew, t)
	return abs(fma(Float64(tanh(asinh(Float64(eh / Float64(ew * t)))) * cos(t)), eh, Float64(1.0 * Float64(sin(t) * ew))))
end

Wolfram

code[eh_, ew_, t_] := N[Abs[N[(N[(N[Tanh[N[ArcSinh[N[(eh / N[(ew * t), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]], $MachinePrecision] * N[Cos[t], $MachinePrecision]), $MachinePrecision] * eh + N[(1.0 * N[(N[Sin[t], $MachinePrecision] * ew), $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%

   \[\leadsto \left|\color{blue}{\mathsf{fma}\left(\tanh \sinh^{-1} \left(\frac{eh}{ew \cdot \tan t}\right) \cdot \cos t, eh, \frac{1}{\sqrt{1 + {\left(\frac{eh}{ew \cdot \tan t}\right)}^{2}}} \cdot \left(\sin t \cdot ew\right)\right)}\right| \]

4. Taylor expanded in eh around 0

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

6. Applied rewrites 98.5%

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

7. Taylor expanded in t around 0

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

9. Applied rewrites 89.0%

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

Alternative 8: 64.3% accurate, 2.4× speedup

Math

\[\begin{array}{l} \\ \begin{array}{l} t_1 := \frac{eh}{ew \cdot t}\\ t_2 := \tanh \sinh^{-1} t\_1\\ \mathbf{if}\;t \leq 0.0106:\\ \;\;\;\;\left|\mathsf{fma}\left(\mathsf{fma}\left(ew, \frac{1}{\sqrt{1 + {t\_1}^{2}}}, \left(-0.5 \cdot eh\right) \cdot \left(t\_2 \cdot t\right)\right), t, t\_2 \cdot eh\right)\right|\\ \mathbf{else}:\\ \;\;\;\;\left|ew \cdot \sin t\right|\\ \end{array} \end{array} \]

FPCore

(FPCore (eh ew t)
 :precision binary64
 (let* ((t_1 (/ eh (* ew t))) (t_2 (tanh (asinh t_1))))
   (if (<= t 0.0106)
     (fabs
      (fma
       (fma ew (/ 1.0 (sqrt (+ 1.0 (pow t_1 2.0)))) (* (* -0.5 eh) (* t_2 t)))
       t
       (* t_2 eh)))
     (fabs (* ew (sin t))))))

C

double code(double eh, double ew, double t) {
	double t_1 = eh / (ew * t);
	double t_2 = tanh(asinh(t_1));
	double tmp;
	if (t <= 0.0106) {
		tmp = fabs(fma(fma(ew, (1.0 / sqrt((1.0 + pow(t_1, 2.0)))), ((-0.5 * eh) * (t_2 * t))), t, (t_2 * eh)));
	} else {
		tmp = fabs((ew * sin(t)));
	}
	return tmp;
}

Julia

function code(eh, ew, t)
	t_1 = Float64(eh / Float64(ew * t))
	t_2 = tanh(asinh(t_1))
	tmp = 0.0
	if (t <= 0.0106)
		tmp = abs(fma(fma(ew, Float64(1.0 / sqrt(Float64(1.0 + (t_1 ^ 2.0)))), Float64(Float64(-0.5 * eh) * Float64(t_2 * t))), t, Float64(t_2 * eh)));
	else
		tmp = abs(Float64(ew * sin(t)));
	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[Tanh[N[ArcSinh[t$95$1], $MachinePrecision]], $MachinePrecision]}, If[LessEqual[t, 0.0106], N[Abs[N[(N[(ew * N[(1.0 / N[Sqrt[N[(1.0 + N[Power[t$95$1, 2.0], $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision] + N[(N[(-0.5 * eh), $MachinePrecision] * N[(t$95$2 * t), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * t + N[(t$95$2 * eh), $MachinePrecision]), $MachinePrecision]], $MachinePrecision], N[Abs[N[(ew * N[Sin[t], $MachinePrecision]), $MachinePrecision]], $MachinePrecision]]]]

Derivation

1. Split input into 2 regimes

2. if t < 0.0106

   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

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

   4. Applied rewrites 53.3%

      \[\leadsto \left|\color{blue}{\mathsf{fma}\left(\mathsf{fma}\left(ew, \frac{1}{\sqrt{1 + {\left(\frac{eh}{ew \cdot \tan t}\right)}^{2}}}, \left(-0.5 \cdot eh\right) \cdot \left(\tanh \sinh^{-1} \left(\frac{eh}{ew \cdot \tan t}\right) \cdot t\right)\right), t, \tanh \sinh^{-1} \left(\frac{eh}{ew \cdot \tan t}\right) \cdot eh\right)}\right| \]

   5. Taylor expanded in t around 0

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

   7. Applied rewrites 53.3%

      \[\leadsto \left|\mathsf{fma}\left(\mathsf{fma}\left(ew, \frac{1}{\sqrt{1 + {\left(\frac{eh}{ew \cdot t}\right)}^{2}}}, \left(-0.5 \cdot eh\right) \cdot \left(\tanh \sinh^{-1} \left(\frac{eh}{ew \cdot \tan t}\right) \cdot t\right)\right), t, \tanh \sinh^{-1} \left(\frac{eh}{ew \cdot \tan t}\right) \cdot eh\right)\right| \]

   8. Taylor expanded in t around 0

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

   10. Applied rewrites 53.4%

       \[\leadsto \left|\mathsf{fma}\left(\mathsf{fma}\left(ew, \frac{1}{\sqrt{1 + {\left(\frac{eh}{ew \cdot t}\right)}^{2}}}, \left(-0.5 \cdot eh\right) \cdot \left(\tanh \sinh^{-1} \left(\frac{eh}{ew \cdot t}\right) \cdot t\right)\right), t, \tanh \sinh^{-1} \left(\frac{eh}{ew \cdot \tan t}\right) \cdot eh\right)\right| \]

   11. Taylor expanded in t around 0

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

   13. Applied rewrites 53.4%

       \[\leadsto \left|\mathsf{fma}\left(\mathsf{fma}\left(ew, \frac{1}{\sqrt{1 + {\left(\frac{eh}{ew \cdot t}\right)}^{2}}}, \left(-0.5 \cdot eh\right) \cdot \left(\tanh \sinh^{-1} \left(\frac{eh}{ew \cdot t}\right) \cdot t\right)\right), t, \tanh \sinh^{-1} \left(\frac{eh}{ew \cdot t}\right) \cdot eh\right)\right| \]

   if 0.0106 < 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%

      \[\leadsto \left|\color{blue}{\mathsf{fma}\left(\tanh \sinh^{-1} \left(\frac{eh}{ew \cdot \tan t}\right) \cdot \cos t, eh, \frac{1}{\sqrt{1 + {\left(\frac{eh}{ew \cdot \tan t}\right)}^{2}}} \cdot \left(\sin t \cdot ew\right)\right)}\right| \]

   4. Taylor expanded in eh around 0

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

      1. lift-sin.f64 N/A

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

      2. lift-*.f64 40.9

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

   6. Applied rewrites 40.9%

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

Alternative 9: 64.1% accurate, 5.1× speedup

Math

\[\begin{array}{l} \\ \begin{array}{l} \mathbf{if}\;t \leq 0.0105:\\ \;\;\;\;\left|\mathsf{fma}\left(ew, t, \tanh \sinh^{-1} \left(\frac{eh}{ew \cdot \left(t \cdot \left(1 + 0.3333333333333333 \cdot \left(t \cdot t\right)\right)\right)}\right) \cdot eh\right)\right|\\ \mathbf{else}:\\ \;\;\;\;\left|ew \cdot \sin t\right|\\ \end{array} \end{array} \]

FPCore

(FPCore (eh ew t)
 :precision binary64
 (if (<= t 0.0105)
   (fabs
    (fma
     ew
     t
     (*
      (tanh (asinh (/ eh (* ew (* t (+ 1.0 (* 0.3333333333333333 (* t t))))))))
      eh)))
   (fabs (* ew (sin t)))))

C

double code(double eh, double ew, double t) {
	double tmp;
	if (t <= 0.0105) {
		tmp = fabs(fma(ew, t, (tanh(asinh((eh / (ew * (t * (1.0 + (0.3333333333333333 * (t * t)))))))) * eh)));
	} else {
		tmp = fabs((ew * sin(t)));
	}
	return tmp;
}

Julia

function code(eh, ew, t)
	tmp = 0.0
	if (t <= 0.0105)
		tmp = abs(fma(ew, t, Float64(tanh(asinh(Float64(eh / Float64(ew * Float64(t * Float64(1.0 + Float64(0.3333333333333333 * Float64(t * t)))))))) * eh)));
	else
		tmp = abs(Float64(ew * sin(t)));
	end
	return tmp
end

Wolfram

code[eh_, ew_, t_] := If[LessEqual[t, 0.0105], N[Abs[N[(ew * t + N[(N[Tanh[N[ArcSinh[N[(eh / N[(ew * N[(t * N[(1.0 + N[(0.3333333333333333 * N[(t * t), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]], $MachinePrecision] * eh), $MachinePrecision]), $MachinePrecision]], $MachinePrecision], N[Abs[N[(ew * N[Sin[t], $MachinePrecision]), $MachinePrecision]], $MachinePrecision]]

Derivation

1. Split input into 2 regimes

2. if t < 0.0105000000000000007

   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

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

   4. Applied rewrites 53.3%

      \[\leadsto \left|\color{blue}{\mathsf{fma}\left(\mathsf{fma}\left(ew, \frac{1}{\sqrt{1 + {\left(\frac{eh}{ew \cdot \tan t}\right)}^{2}}}, \left(-0.5 \cdot eh\right) \cdot \left(\tanh \sinh^{-1} \left(\frac{eh}{ew \cdot \tan t}\right) \cdot t\right)\right), t, \tanh \sinh^{-1} \left(\frac{eh}{ew \cdot \tan t}\right) \cdot eh\right)}\right| \]

   5. Taylor expanded in eh around 0

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

   7. Applied rewrites 55.0%

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

   8. Taylor expanded in t around 0

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

      1. lower-*.f64 N/A

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

      2. lower-+.f64 N/A

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

      3. lower-*.f64 N/A

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

      4. unpow2 N/A

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

      5. lower-*.f64 53.6

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

   10. Applied rewrites 53.6%

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

   if 0.0105000000000000007 < 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%

      \[\leadsto \left|\color{blue}{\mathsf{fma}\left(\tanh \sinh^{-1} \left(\frac{eh}{ew \cdot \tan t}\right) \cdot \cos t, eh, \frac{1}{\sqrt{1 + {\left(\frac{eh}{ew \cdot \tan t}\right)}^{2}}} \cdot \left(\sin t \cdot ew\right)\right)}\right| \]

   4. Taylor expanded in eh around 0

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

      1. lift-sin.f64 N/A

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

      2. lift-*.f64 40.9

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

   6. Applied rewrites 40.9%

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

Alternative 10: 51.2% accurate, 6.0× speedup

Math

\[\begin{array}{l} \\ \begin{array}{l} \mathbf{if}\;t \leq 4.1 \cdot 10^{-14}:\\ \;\;\;\;\left|\tanh \sinh^{-1} \left(\frac{eh}{ew \cdot t}\right) \cdot eh\right|\\ \mathbf{else}:\\ \;\;\;\;\left|ew \cdot \sin t\right|\\ \end{array} \end{array} \]

FPCore

(FPCore (eh ew t)
 :precision binary64
 (if (<= t 4.1e-14)
   (fabs (* (tanh (asinh (/ eh (* ew t)))) eh))
   (fabs (* ew (sin t)))))

C

double code(double eh, double ew, double t) {
	double tmp;
	if (t <= 4.1e-14) {
		tmp = fabs((tanh(asinh((eh / (ew * t)))) * eh));
	} else {
		tmp = fabs((ew * sin(t)));
	}
	return tmp;
}

Python

def code(eh, ew, t):
	tmp = 0
	if t <= 4.1e-14:
		tmp = math.fabs((math.tanh(math.asinh((eh / (ew * t)))) * eh))
	else:
		tmp = math.fabs((ew * math.sin(t)))
	return tmp

Julia

function code(eh, ew, t)
	tmp = 0.0
	if (t <= 4.1e-14)
		tmp = abs(Float64(tanh(asinh(Float64(eh / Float64(ew * t)))) * eh));
	else
		tmp = abs(Float64(ew * sin(t)));
	end
	return tmp
end

MATLAB

function tmp_2 = code(eh, ew, t)
	tmp = 0.0;
	if (t <= 4.1e-14)
		tmp = abs((tanh(asinh((eh / (ew * t)))) * eh));
	else
		tmp = abs((ew * sin(t)));
	end
	tmp_2 = tmp;
end

Wolfram

code[eh_, ew_, t_] := If[LessEqual[t, 4.1e-14], N[Abs[N[(N[Tanh[N[ArcSinh[N[(eh / N[(ew * t), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]], $MachinePrecision] * eh), $MachinePrecision]], $MachinePrecision], N[Abs[N[(ew * N[Sin[t], $MachinePrecision]), $MachinePrecision]], $MachinePrecision]]

Derivation

1. Split input into 2 regimes

2. if t < 4.1000000000000002e-14

   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. *-commutative N/A

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

      2. lower-*.f64 N/A

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

   4. Applied rewrites 42.9%

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

   5. Taylor expanded in t around 0

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

   7. Applied rewrites 41.0%

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

   if 4.1000000000000002e-14 < 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%

      \[\leadsto \left|\color{blue}{\mathsf{fma}\left(\tanh \sinh^{-1} \left(\frac{eh}{ew \cdot \tan t}\right) \cdot \cos t, eh, \frac{1}{\sqrt{1 + {\left(\frac{eh}{ew \cdot \tan t}\right)}^{2}}} \cdot \left(\sin t \cdot ew\right)\right)}\right| \]

   4. Taylor expanded in eh around 0

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

      1. lift-sin.f64 N/A

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

      2. lift-*.f64 40.9

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

   6. Applied rewrites 40.9%

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

Alternative 11: 42.3% accurate, 7.7× speedup

Math

\[\begin{array}{l} \\ \begin{array}{l} \mathbf{if}\;ew \leq 2.45 \cdot 10^{+169}:\\ \;\;\;\;\left|\tanh \sinh^{-1} \left(\frac{eh}{ew \cdot t}\right) \cdot eh\right|\\ \mathbf{else}:\\ \;\;\;\;\left|ew \cdot t\right|\\ \end{array} \end{array} \]

FPCore

(FPCore (eh ew t)
 :precision binary64
 (if (<= ew 2.45e+169)
   (fabs (* (tanh (asinh (/ eh (* ew t)))) eh))
   (fabs (* ew t))))

C

double code(double eh, double ew, double t) {
	double tmp;
	if (ew <= 2.45e+169) {
		tmp = fabs((tanh(asinh((eh / (ew * t)))) * eh));
	} else {
		tmp = fabs((ew * t));
	}
	return tmp;
}

Python

def code(eh, ew, t):
	tmp = 0
	if ew <= 2.45e+169:
		tmp = math.fabs((math.tanh(math.asinh((eh / (ew * t)))) * eh))
	else:
		tmp = math.fabs((ew * t))
	return tmp

Julia

function code(eh, ew, t)
	tmp = 0.0
	if (ew <= 2.45e+169)
		tmp = abs(Float64(tanh(asinh(Float64(eh / Float64(ew * t)))) * eh));
	else
		tmp = abs(Float64(ew * t));
	end
	return tmp
end

MATLAB

function tmp_2 = code(eh, ew, t)
	tmp = 0.0;
	if (ew <= 2.45e+169)
		tmp = abs((tanh(asinh((eh / (ew * t)))) * eh));
	else
		tmp = abs((ew * t));
	end
	tmp_2 = tmp;
end

Wolfram

code[eh_, ew_, t_] := If[LessEqual[ew, 2.45e+169], N[Abs[N[(N[Tanh[N[ArcSinh[N[(eh / N[(ew * t), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]], $MachinePrecision] * eh), $MachinePrecision]], $MachinePrecision], N[Abs[N[(ew * t), $MachinePrecision]], $MachinePrecision]]

Derivation

1. Split input into 2 regimes

2. if ew < 2.45000000000000013e169

   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. *-commutative N/A

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

      2. lower-*.f64 N/A

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

   4. Applied rewrites 42.9%

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

   5. Taylor expanded in t around 0

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

   7. Applied rewrites 41.0%

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

   if 2.45000000000000013e169 < ew

   1. Initial program 99.8%

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

   2. Taylor expanded in t around 0

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

   4. Applied rewrites 53.3%

      \[\leadsto \left|\color{blue}{\mathsf{fma}\left(\mathsf{fma}\left(ew, \frac{1}{\sqrt{1 + {\left(\frac{eh}{ew \cdot \tan t}\right)}^{2}}}, \left(-0.5 \cdot eh\right) \cdot \left(\tanh \sinh^{-1} \left(\frac{eh}{ew \cdot \tan t}\right) \cdot t\right)\right), t, \tanh \sinh^{-1} \left(\frac{eh}{ew \cdot \tan t}\right) \cdot eh\right)}\right| \]

   5. Taylor expanded in eh around 0

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

      1. lower-*.f64 18.6

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

   7. Applied rewrites 18.6%

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

Alternative 12: 19.6% accurate, 9.3× speedup

Math

\[\begin{array}{l} \\ \begin{array}{l} \mathbf{if}\;eh \leq 2.35 \cdot 10^{-126}:\\ \;\;\;\;\left|ew \cdot t\right|\\ \mathbf{else}:\\ \;\;\;\;\left|\frac{eh \cdot eh}{ew \cdot \sqrt{\frac{eh \cdot eh}{ew \cdot ew}}}\right|\\ \end{array} \end{array} \]

FPCore

(FPCore (eh ew t)
 :precision binary64
 (if (<= eh 2.35e-126)
   (fabs (* ew t))
   (fabs (/ (* eh eh) (* ew (sqrt (/ (* eh eh) (* ew ew))))))))

C

double code(double eh, double ew, double t) {
	double tmp;
	if (eh <= 2.35e-126) {
		tmp = fabs((ew * t));
	} else {
		tmp = fabs(((eh * eh) / (ew * sqrt(((eh * eh) / (ew * ew))))));
	}
	return tmp;
}

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) :: tmp
    if (eh <= 2.35d-126) then
        tmp = abs((ew * t))
    else
        tmp = abs(((eh * eh) / (ew * sqrt(((eh * eh) / (ew * ew))))))
    end if
    code = tmp
end function

Java

public static double code(double eh, double ew, double t) {
	double tmp;
	if (eh <= 2.35e-126) {
		tmp = Math.abs((ew * t));
	} else {
		tmp = Math.abs(((eh * eh) / (ew * Math.sqrt(((eh * eh) / (ew * ew))))));
	}
	return tmp;
}

Python

def code(eh, ew, t):
	tmp = 0
	if eh <= 2.35e-126:
		tmp = math.fabs((ew * t))
	else:
		tmp = math.fabs(((eh * eh) / (ew * math.sqrt(((eh * eh) / (ew * ew))))))
	return tmp

Julia

function code(eh, ew, t)
	tmp = 0.0
	if (eh <= 2.35e-126)
		tmp = abs(Float64(ew * t));
	else
		tmp = abs(Float64(Float64(eh * eh) / Float64(ew * sqrt(Float64(Float64(eh * eh) / Float64(ew * ew))))));
	end
	return tmp
end

MATLAB

function tmp_2 = code(eh, ew, t)
	tmp = 0.0;
	if (eh <= 2.35e-126)
		tmp = abs((ew * t));
	else
		tmp = abs(((eh * eh) / (ew * sqrt(((eh * eh) / (ew * ew))))));
	end
	tmp_2 = tmp;
end

Wolfram

code[eh_, ew_, t_] := If[LessEqual[eh, 2.35e-126], N[Abs[N[(ew * t), $MachinePrecision]], $MachinePrecision], N[Abs[N[(N[(eh * eh), $MachinePrecision] / N[(ew * N[Sqrt[N[(N[(eh * eh), $MachinePrecision] / N[(ew * ew), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]]

Derivation

1. Split input into 2 regimes

2. if eh < 2.35000000000000009e-126

   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

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

   4. Applied rewrites 53.3%

      \[\leadsto \left|\color{blue}{\mathsf{fma}\left(\mathsf{fma}\left(ew, \frac{1}{\sqrt{1 + {\left(\frac{eh}{ew \cdot \tan t}\right)}^{2}}}, \left(-0.5 \cdot eh\right) \cdot \left(\tanh \sinh^{-1} \left(\frac{eh}{ew \cdot \tan t}\right) \cdot t\right)\right), t, \tanh \sinh^{-1} \left(\frac{eh}{ew \cdot \tan t}\right) \cdot eh\right)}\right| \]

   5. Taylor expanded in eh around 0

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

      1. lower-*.f64 18.6

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

   7. Applied rewrites 18.6%

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

   if 2.35000000000000009e-126 < 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

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

      1. lower-/.f64 N/A

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

      2. *-commutative N/A

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

      3. lower-*.f64 99.0

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

   4. Applied rewrites 99.0%

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

   5. Taylor expanded in t around 0

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

      1. lower-/.f64 N/A

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

      2. *-commutative N/A

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

      3. lower-*.f64 89.6

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

   7. Applied rewrites 89.6%

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

      1. lift-+.f64 N/A

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

      2. lift-*.f64 N/A

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

      3. lift-*.f64 N/A

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

      4. lift-sin.f64 N/A

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

      5. lower-fma.f64 N/A

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

   9. Applied rewrites 56.7%

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

   10. Taylor expanded in t around 0

       \[\leadsto \left|\color{blue}{\frac{{eh}^{2}}{ew \cdot \sqrt{\frac{{eh}^{2}}{{ew}^{2}}}}}\right| \]
   11. Step-by-step derivation

       1. cos-atan-rev N/A

          \[\leadsto \left|\frac{{eh}^{2}}{ew \cdot \sqrt{\frac{{eh}^{2}}{{ew}^{2}}}}\right| \]

       2. sin-atan-rev N/A

          \[\leadsto \left|\frac{{eh}^{2}}{ew \cdot \sqrt{\frac{{eh}^{2}}{{ew}^{2}}}}\right| \]

       3. lower-/.f64 N/A

          \[\leadsto \left|\frac{{eh}^{2}}{\color{blue}{ew \cdot \sqrt{\frac{{eh}^{2}}{{ew}^{2}}}}}\right| \]

       4. unpow2 N/A

          \[\leadsto \left|\frac{eh \cdot eh}{\color{blue}{ew} \cdot \sqrt{\frac{{eh}^{2}}{{ew}^{2}}}}\right| \]

       5. lower-*.f64 N/A

          \[\leadsto \left|\frac{eh \cdot eh}{\color{blue}{ew} \cdot \sqrt{\frac{{eh}^{2}}{{ew}^{2}}}}\right| \]

       6. lower-*.f64 N/A

          \[\leadsto \left|\frac{eh \cdot eh}{ew \cdot \color{blue}{\sqrt{\frac{{eh}^{2}}{{ew}^{2}}}}}\right| \]

       7. lower-sqrt.f64 N/A

          \[\leadsto \left|\frac{eh \cdot eh}{ew \cdot \sqrt{\frac{{eh}^{2}}{{ew}^{2}}}}\right| \]

   12. Applied rewrites 11.7%

       \[\leadsto \left|\color{blue}{\frac{eh \cdot eh}{ew \cdot \sqrt{\frac{eh \cdot eh}{ew \cdot ew}}}}\right| \]
3. Recombined 2 regimes into one program.
4. Add Preprocessing

Alternative 13: 18.6% 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%

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

2. Taylor expanded in t around 0

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

4. Applied rewrites 53.3%

   \[\leadsto \left|\color{blue}{\mathsf{fma}\left(\mathsf{fma}\left(ew, \frac{1}{\sqrt{1 + {\left(\frac{eh}{ew \cdot \tan t}\right)}^{2}}}, \left(-0.5 \cdot eh\right) \cdot \left(\tanh \sinh^{-1} \left(\frac{eh}{ew \cdot \tan t}\right) \cdot t\right)\right), t, \tanh \sinh^{-1} \left(\frac{eh}{ew \cdot \tan t}\right) \cdot eh\right)}\right| \]

5. Taylor expanded in eh around 0

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

   1. lower-*.f64 18.6

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

7. Applied rewrites 18.6%

   \[\leadsto \left|ew \cdot \color{blue}{t}\right| \]
8. Add Preprocessing

Reproduce

herbie shell --seed 2025140 
(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))))))))