| Alternative 1 | |
|---|---|
| Accuracy | 35.3% |
| Cost | 33480 |
(FPCore (a b angle x-scale y-scale)
:precision binary64
(/
(-
(sqrt
(*
(*
(* 2.0 (/ (* 4.0 (* (* b a) (* b (- a)))) (pow (* x-scale y-scale) 2.0)))
(* (* b a) (* b (- a))))
(-
(+
(/
(/
(+
(pow (* a (sin (* (/ angle 180.0) PI))) 2.0)
(pow (* b (cos (* (/ angle 180.0) PI))) 2.0))
x-scale)
x-scale)
(/
(/
(+
(pow (* a (cos (* (/ angle 180.0) PI))) 2.0)
(pow (* b (sin (* (/ angle 180.0) PI))) 2.0))
y-scale)
y-scale))
(sqrt
(+
(pow
(-
(/
(/
(+
(pow (* a (sin (* (/ angle 180.0) PI))) 2.0)
(pow (* b (cos (* (/ angle 180.0) PI))) 2.0))
x-scale)
x-scale)
(/
(/
(+
(pow (* a (cos (* (/ angle 180.0) PI))) 2.0)
(pow (* b (sin (* (/ angle 180.0) PI))) 2.0))
y-scale)
y-scale))
2.0)
(pow
(/
(/
(*
(*
(* 2.0 (- (pow b 2.0) (pow a 2.0)))
(sin (* (/ angle 180.0) PI)))
(cos (* (/ angle 180.0) PI)))
x-scale)
y-scale)
2.0)))))))
(/ (* 4.0 (* (* b a) (* b (- a)))) (pow (* x-scale y-scale) 2.0))))(FPCore (a b angle x-scale y-scale)
:precision binary64
(let* ((t_0 (* (* x-scale 0.25) 0.0))
(t_1 (cos (* PI (* angle 0.005555555555555556))))
(t_2 (* 0.005555555555555556 (* PI angle))))
(if (<= x-scale -2.1e-29)
t_0
(if (<= x-scale -1.1e-118)
(*
0.25
(fabs
(*
(* (sqrt 8.0) (* x-scale y-scale))
(hypot (* t_1 (/ a y-scale)) (/ a y-scale)))))
(if (<= x-scale 7.5e-134)
t_0
(if (<= x-scale 5.2e-27)
(* (* x-scale 0.25) (fabs (* a 4.0)))
(if (<= x-scale 4e-25)
(*
0.25
(*
(* x-scale (* y-scale (* (sqrt 8.0) b)))
(sqrt
(+
(/ (pow (sin t_2) 2.0) (* y-scale y-scale))
(-
(/ (pow (cos t_2) 2.0) (* x-scale x-scale))
(/ (pow t_1 2.0) (* x-scale x-scale)))))))
(if (<= x-scale 9.5e+107)
t_0
(* (* x-scale 0.25) (sqrt (* a (* a 16.0))))))))))))double code(double a, double b, double angle, double x_45_scale, double y_45_scale) {
return -sqrt((((2.0 * ((4.0 * ((b * a) * (b * -a))) / pow((x_45_scale * y_45_scale), 2.0))) * ((b * a) * (b * -a))) * (((((pow((a * sin(((angle / 180.0) * ((double) M_PI)))), 2.0) + pow((b * cos(((angle / 180.0) * ((double) M_PI)))), 2.0)) / x_45_scale) / x_45_scale) + (((pow((a * cos(((angle / 180.0) * ((double) M_PI)))), 2.0) + pow((b * sin(((angle / 180.0) * ((double) M_PI)))), 2.0)) / y_45_scale) / y_45_scale)) - sqrt((pow(((((pow((a * sin(((angle / 180.0) * ((double) M_PI)))), 2.0) + pow((b * cos(((angle / 180.0) * ((double) M_PI)))), 2.0)) / x_45_scale) / x_45_scale) - (((pow((a * cos(((angle / 180.0) * ((double) M_PI)))), 2.0) + pow((b * sin(((angle / 180.0) * ((double) M_PI)))), 2.0)) / y_45_scale) / y_45_scale)), 2.0) + pow((((((2.0 * (pow(b, 2.0) - pow(a, 2.0))) * sin(((angle / 180.0) * ((double) M_PI)))) * cos(((angle / 180.0) * ((double) M_PI)))) / x_45_scale) / y_45_scale), 2.0)))))) / ((4.0 * ((b * a) * (b * -a))) / pow((x_45_scale * y_45_scale), 2.0));
}
double code(double a, double b, double angle, double x_45_scale, double y_45_scale) {
double t_0 = (x_45_scale * 0.25) * 0.0;
double t_1 = cos((((double) M_PI) * (angle * 0.005555555555555556)));
double t_2 = 0.005555555555555556 * (((double) M_PI) * angle);
double tmp;
if (x_45_scale <= -2.1e-29) {
tmp = t_0;
} else if (x_45_scale <= -1.1e-118) {
tmp = 0.25 * fabs(((sqrt(8.0) * (x_45_scale * y_45_scale)) * hypot((t_1 * (a / y_45_scale)), (a / y_45_scale))));
} else if (x_45_scale <= 7.5e-134) {
tmp = t_0;
} else if (x_45_scale <= 5.2e-27) {
tmp = (x_45_scale * 0.25) * fabs((a * 4.0));
} else if (x_45_scale <= 4e-25) {
tmp = 0.25 * ((x_45_scale * (y_45_scale * (sqrt(8.0) * b))) * sqrt(((pow(sin(t_2), 2.0) / (y_45_scale * y_45_scale)) + ((pow(cos(t_2), 2.0) / (x_45_scale * x_45_scale)) - (pow(t_1, 2.0) / (x_45_scale * x_45_scale))))));
} else if (x_45_scale <= 9.5e+107) {
tmp = t_0;
} else {
tmp = (x_45_scale * 0.25) * sqrt((a * (a * 16.0)));
}
return tmp;
}
public static double code(double a, double b, double angle, double x_45_scale, double y_45_scale) {
return -Math.sqrt((((2.0 * ((4.0 * ((b * a) * (b * -a))) / Math.pow((x_45_scale * y_45_scale), 2.0))) * ((b * a) * (b * -a))) * (((((Math.pow((a * Math.sin(((angle / 180.0) * Math.PI))), 2.0) + Math.pow((b * Math.cos(((angle / 180.0) * Math.PI))), 2.0)) / x_45_scale) / x_45_scale) + (((Math.pow((a * Math.cos(((angle / 180.0) * Math.PI))), 2.0) + Math.pow((b * Math.sin(((angle / 180.0) * Math.PI))), 2.0)) / y_45_scale) / y_45_scale)) - Math.sqrt((Math.pow(((((Math.pow((a * Math.sin(((angle / 180.0) * Math.PI))), 2.0) + Math.pow((b * Math.cos(((angle / 180.0) * Math.PI))), 2.0)) / x_45_scale) / x_45_scale) - (((Math.pow((a * Math.cos(((angle / 180.0) * Math.PI))), 2.0) + Math.pow((b * Math.sin(((angle / 180.0) * Math.PI))), 2.0)) / y_45_scale) / y_45_scale)), 2.0) + Math.pow((((((2.0 * (Math.pow(b, 2.0) - Math.pow(a, 2.0))) * Math.sin(((angle / 180.0) * Math.PI))) * Math.cos(((angle / 180.0) * Math.PI))) / x_45_scale) / y_45_scale), 2.0)))))) / ((4.0 * ((b * a) * (b * -a))) / Math.pow((x_45_scale * y_45_scale), 2.0));
}
public static double code(double a, double b, double angle, double x_45_scale, double y_45_scale) {
double t_0 = (x_45_scale * 0.25) * 0.0;
double t_1 = Math.cos((Math.PI * (angle * 0.005555555555555556)));
double t_2 = 0.005555555555555556 * (Math.PI * angle);
double tmp;
if (x_45_scale <= -2.1e-29) {
tmp = t_0;
} else if (x_45_scale <= -1.1e-118) {
tmp = 0.25 * Math.abs(((Math.sqrt(8.0) * (x_45_scale * y_45_scale)) * Math.hypot((t_1 * (a / y_45_scale)), (a / y_45_scale))));
} else if (x_45_scale <= 7.5e-134) {
tmp = t_0;
} else if (x_45_scale <= 5.2e-27) {
tmp = (x_45_scale * 0.25) * Math.abs((a * 4.0));
} else if (x_45_scale <= 4e-25) {
tmp = 0.25 * ((x_45_scale * (y_45_scale * (Math.sqrt(8.0) * b))) * Math.sqrt(((Math.pow(Math.sin(t_2), 2.0) / (y_45_scale * y_45_scale)) + ((Math.pow(Math.cos(t_2), 2.0) / (x_45_scale * x_45_scale)) - (Math.pow(t_1, 2.0) / (x_45_scale * x_45_scale))))));
} else if (x_45_scale <= 9.5e+107) {
tmp = t_0;
} else {
tmp = (x_45_scale * 0.25) * Math.sqrt((a * (a * 16.0)));
}
return tmp;
}
def code(a, b, angle, x_45_scale, y_45_scale): return -math.sqrt((((2.0 * ((4.0 * ((b * a) * (b * -a))) / math.pow((x_45_scale * y_45_scale), 2.0))) * ((b * a) * (b * -a))) * (((((math.pow((a * math.sin(((angle / 180.0) * math.pi))), 2.0) + math.pow((b * math.cos(((angle / 180.0) * math.pi))), 2.0)) / x_45_scale) / x_45_scale) + (((math.pow((a * math.cos(((angle / 180.0) * math.pi))), 2.0) + math.pow((b * math.sin(((angle / 180.0) * math.pi))), 2.0)) / y_45_scale) / y_45_scale)) - math.sqrt((math.pow(((((math.pow((a * math.sin(((angle / 180.0) * math.pi))), 2.0) + math.pow((b * math.cos(((angle / 180.0) * math.pi))), 2.0)) / x_45_scale) / x_45_scale) - (((math.pow((a * math.cos(((angle / 180.0) * math.pi))), 2.0) + math.pow((b * math.sin(((angle / 180.0) * math.pi))), 2.0)) / y_45_scale) / y_45_scale)), 2.0) + math.pow((((((2.0 * (math.pow(b, 2.0) - math.pow(a, 2.0))) * math.sin(((angle / 180.0) * math.pi))) * math.cos(((angle / 180.0) * math.pi))) / x_45_scale) / y_45_scale), 2.0)))))) / ((4.0 * ((b * a) * (b * -a))) / math.pow((x_45_scale * y_45_scale), 2.0))
def code(a, b, angle, x_45_scale, y_45_scale): t_0 = (x_45_scale * 0.25) * 0.0 t_1 = math.cos((math.pi * (angle * 0.005555555555555556))) t_2 = 0.005555555555555556 * (math.pi * angle) tmp = 0 if x_45_scale <= -2.1e-29: tmp = t_0 elif x_45_scale <= -1.1e-118: tmp = 0.25 * math.fabs(((math.sqrt(8.0) * (x_45_scale * y_45_scale)) * math.hypot((t_1 * (a / y_45_scale)), (a / y_45_scale)))) elif x_45_scale <= 7.5e-134: tmp = t_0 elif x_45_scale <= 5.2e-27: tmp = (x_45_scale * 0.25) * math.fabs((a * 4.0)) elif x_45_scale <= 4e-25: tmp = 0.25 * ((x_45_scale * (y_45_scale * (math.sqrt(8.0) * b))) * math.sqrt(((math.pow(math.sin(t_2), 2.0) / (y_45_scale * y_45_scale)) + ((math.pow(math.cos(t_2), 2.0) / (x_45_scale * x_45_scale)) - (math.pow(t_1, 2.0) / (x_45_scale * x_45_scale)))))) elif x_45_scale <= 9.5e+107: tmp = t_0 else: tmp = (x_45_scale * 0.25) * math.sqrt((a * (a * 16.0))) return tmp
function code(a, b, angle, x_45_scale, y_45_scale) return Float64(Float64(-sqrt(Float64(Float64(Float64(2.0 * Float64(Float64(4.0 * Float64(Float64(b * a) * Float64(b * Float64(-a)))) / (Float64(x_45_scale * y_45_scale) ^ 2.0))) * Float64(Float64(b * a) * Float64(b * Float64(-a)))) * Float64(Float64(Float64(Float64(Float64((Float64(a * sin(Float64(Float64(angle / 180.0) * pi))) ^ 2.0) + (Float64(b * cos(Float64(Float64(angle / 180.0) * pi))) ^ 2.0)) / x_45_scale) / x_45_scale) + Float64(Float64(Float64((Float64(a * cos(Float64(Float64(angle / 180.0) * pi))) ^ 2.0) + (Float64(b * sin(Float64(Float64(angle / 180.0) * pi))) ^ 2.0)) / y_45_scale) / y_45_scale)) - sqrt(Float64((Float64(Float64(Float64(Float64((Float64(a * sin(Float64(Float64(angle / 180.0) * pi))) ^ 2.0) + (Float64(b * cos(Float64(Float64(angle / 180.0) * pi))) ^ 2.0)) / x_45_scale) / x_45_scale) - Float64(Float64(Float64((Float64(a * cos(Float64(Float64(angle / 180.0) * pi))) ^ 2.0) + (Float64(b * sin(Float64(Float64(angle / 180.0) * pi))) ^ 2.0)) / y_45_scale) / y_45_scale)) ^ 2.0) + (Float64(Float64(Float64(Float64(Float64(2.0 * Float64((b ^ 2.0) - (a ^ 2.0))) * sin(Float64(Float64(angle / 180.0) * pi))) * cos(Float64(Float64(angle / 180.0) * pi))) / x_45_scale) / y_45_scale) ^ 2.0))))))) / Float64(Float64(4.0 * Float64(Float64(b * a) * Float64(b * Float64(-a)))) / (Float64(x_45_scale * y_45_scale) ^ 2.0))) end
function code(a, b, angle, x_45_scale, y_45_scale) t_0 = Float64(Float64(x_45_scale * 0.25) * 0.0) t_1 = cos(Float64(pi * Float64(angle * 0.005555555555555556))) t_2 = Float64(0.005555555555555556 * Float64(pi * angle)) tmp = 0.0 if (x_45_scale <= -2.1e-29) tmp = t_0; elseif (x_45_scale <= -1.1e-118) tmp = Float64(0.25 * abs(Float64(Float64(sqrt(8.0) * Float64(x_45_scale * y_45_scale)) * hypot(Float64(t_1 * Float64(a / y_45_scale)), Float64(a / y_45_scale))))); elseif (x_45_scale <= 7.5e-134) tmp = t_0; elseif (x_45_scale <= 5.2e-27) tmp = Float64(Float64(x_45_scale * 0.25) * abs(Float64(a * 4.0))); elseif (x_45_scale <= 4e-25) tmp = Float64(0.25 * Float64(Float64(x_45_scale * Float64(y_45_scale * Float64(sqrt(8.0) * b))) * sqrt(Float64(Float64((sin(t_2) ^ 2.0) / Float64(y_45_scale * y_45_scale)) + Float64(Float64((cos(t_2) ^ 2.0) / Float64(x_45_scale * x_45_scale)) - Float64((t_1 ^ 2.0) / Float64(x_45_scale * x_45_scale))))))); elseif (x_45_scale <= 9.5e+107) tmp = t_0; else tmp = Float64(Float64(x_45_scale * 0.25) * sqrt(Float64(a * Float64(a * 16.0)))); end return tmp end
function tmp = code(a, b, angle, x_45_scale, y_45_scale) tmp = -sqrt((((2.0 * ((4.0 * ((b * a) * (b * -a))) / ((x_45_scale * y_45_scale) ^ 2.0))) * ((b * a) * (b * -a))) * (((((((a * sin(((angle / 180.0) * pi))) ^ 2.0) + ((b * cos(((angle / 180.0) * pi))) ^ 2.0)) / x_45_scale) / x_45_scale) + (((((a * cos(((angle / 180.0) * pi))) ^ 2.0) + ((b * sin(((angle / 180.0) * pi))) ^ 2.0)) / y_45_scale) / y_45_scale)) - sqrt(((((((((a * sin(((angle / 180.0) * pi))) ^ 2.0) + ((b * cos(((angle / 180.0) * pi))) ^ 2.0)) / x_45_scale) / x_45_scale) - (((((a * cos(((angle / 180.0) * pi))) ^ 2.0) + ((b * sin(((angle / 180.0) * pi))) ^ 2.0)) / y_45_scale) / y_45_scale)) ^ 2.0) + ((((((2.0 * ((b ^ 2.0) - (a ^ 2.0))) * sin(((angle / 180.0) * pi))) * cos(((angle / 180.0) * pi))) / x_45_scale) / y_45_scale) ^ 2.0)))))) / ((4.0 * ((b * a) * (b * -a))) / ((x_45_scale * y_45_scale) ^ 2.0)); end
function tmp_2 = code(a, b, angle, x_45_scale, y_45_scale) t_0 = (x_45_scale * 0.25) * 0.0; t_1 = cos((pi * (angle * 0.005555555555555556))); t_2 = 0.005555555555555556 * (pi * angle); tmp = 0.0; if (x_45_scale <= -2.1e-29) tmp = t_0; elseif (x_45_scale <= -1.1e-118) tmp = 0.25 * abs(((sqrt(8.0) * (x_45_scale * y_45_scale)) * hypot((t_1 * (a / y_45_scale)), (a / y_45_scale)))); elseif (x_45_scale <= 7.5e-134) tmp = t_0; elseif (x_45_scale <= 5.2e-27) tmp = (x_45_scale * 0.25) * abs((a * 4.0)); elseif (x_45_scale <= 4e-25) tmp = 0.25 * ((x_45_scale * (y_45_scale * (sqrt(8.0) * b))) * sqrt((((sin(t_2) ^ 2.0) / (y_45_scale * y_45_scale)) + (((cos(t_2) ^ 2.0) / (x_45_scale * x_45_scale)) - ((t_1 ^ 2.0) / (x_45_scale * x_45_scale)))))); elseif (x_45_scale <= 9.5e+107) tmp = t_0; else tmp = (x_45_scale * 0.25) * sqrt((a * (a * 16.0))); end tmp_2 = tmp; end
code[a_, b_, angle_, x$45$scale_, y$45$scale_] := N[((-N[Sqrt[N[(N[(N[(2.0 * N[(N[(4.0 * N[(N[(b * a), $MachinePrecision] * N[(b * (-a)), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[Power[N[(x$45$scale * y$45$scale), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * N[(N[(b * a), $MachinePrecision] * N[(b * (-a)), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * N[(N[(N[(N[(N[(N[Power[N[(a * N[Sin[N[(N[(angle / 180.0), $MachinePrecision] * Pi), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * N[Cos[N[(N[(angle / 180.0), $MachinePrecision] * Pi), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision] / x$45$scale), $MachinePrecision] / x$45$scale), $MachinePrecision] + N[(N[(N[(N[Power[N[(a * N[Cos[N[(N[(angle / 180.0), $MachinePrecision] * Pi), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * N[Sin[N[(N[(angle / 180.0), $MachinePrecision] * Pi), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision] / y$45$scale), $MachinePrecision] / y$45$scale), $MachinePrecision]), $MachinePrecision] - N[Sqrt[N[(N[Power[N[(N[(N[(N[(N[Power[N[(a * N[Sin[N[(N[(angle / 180.0), $MachinePrecision] * Pi), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * N[Cos[N[(N[(angle / 180.0), $MachinePrecision] * Pi), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision] / x$45$scale), $MachinePrecision] / x$45$scale), $MachinePrecision] - N[(N[(N[(N[Power[N[(a * N[Cos[N[(N[(angle / 180.0), $MachinePrecision] * Pi), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * N[Sin[N[(N[(angle / 180.0), $MachinePrecision] * Pi), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision] / y$45$scale), $MachinePrecision] / y$45$scale), $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(N[(N[(N[(N[(2.0 * N[(N[Power[b, 2.0], $MachinePrecision] - N[Power[a, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * N[Sin[N[(N[(angle / 180.0), $MachinePrecision] * Pi), $MachinePrecision]], $MachinePrecision]), $MachinePrecision] * N[Cos[N[(N[(angle / 180.0), $MachinePrecision] * Pi), $MachinePrecision]], $MachinePrecision]), $MachinePrecision] / x$45$scale), $MachinePrecision] / y$45$scale), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]) / N[(N[(4.0 * N[(N[(b * a), $MachinePrecision] * N[(b * (-a)), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[Power[N[(x$45$scale * y$45$scale), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]
code[a_, b_, angle_, x$45$scale_, y$45$scale_] := Block[{t$95$0 = N[(N[(x$45$scale * 0.25), $MachinePrecision] * 0.0), $MachinePrecision]}, Block[{t$95$1 = N[Cos[N[(Pi * N[(angle * 0.005555555555555556), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]}, Block[{t$95$2 = N[(0.005555555555555556 * N[(Pi * angle), $MachinePrecision]), $MachinePrecision]}, If[LessEqual[x$45$scale, -2.1e-29], t$95$0, If[LessEqual[x$45$scale, -1.1e-118], N[(0.25 * N[Abs[N[(N[(N[Sqrt[8.0], $MachinePrecision] * N[(x$45$scale * y$45$scale), $MachinePrecision]), $MachinePrecision] * N[Sqrt[N[(t$95$1 * N[(a / y$45$scale), $MachinePrecision]), $MachinePrecision] ^ 2 + N[(a / y$45$scale), $MachinePrecision] ^ 2], $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], If[LessEqual[x$45$scale, 7.5e-134], t$95$0, If[LessEqual[x$45$scale, 5.2e-27], N[(N[(x$45$scale * 0.25), $MachinePrecision] * N[Abs[N[(a * 4.0), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], If[LessEqual[x$45$scale, 4e-25], N[(0.25 * N[(N[(x$45$scale * N[(y$45$scale * N[(N[Sqrt[8.0], $MachinePrecision] * b), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * N[Sqrt[N[(N[(N[Power[N[Sin[t$95$2], $MachinePrecision], 2.0], $MachinePrecision] / N[(y$45$scale * y$45$scale), $MachinePrecision]), $MachinePrecision] + N[(N[(N[Power[N[Cos[t$95$2], $MachinePrecision], 2.0], $MachinePrecision] / N[(x$45$scale * x$45$scale), $MachinePrecision]), $MachinePrecision] - N[(N[Power[t$95$1, 2.0], $MachinePrecision] / N[(x$45$scale * x$45$scale), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision], If[LessEqual[x$45$scale, 9.5e+107], t$95$0, N[(N[(x$45$scale * 0.25), $MachinePrecision] * N[Sqrt[N[(a * N[(a * 16.0), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]]]]]]]]]]
\frac{-\sqrt{\left(\left(2 \cdot \frac{4 \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}}\right) \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)\right) \cdot \left(\left(\frac{\frac{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{x-scale}}{x-scale} + \frac{\frac{{\left(a \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{y-scale}}{y-scale}\right) - \sqrt{{\left(\frac{\frac{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{x-scale}}{x-scale} - \frac{\frac{{\left(a \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{y-scale}}{y-scale}\right)}^{2} + {\left(\frac{\frac{\left(\left(2 \cdot \left({b}^{2} - {a}^{2}\right)\right) \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right) \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)}{x-scale}}{y-scale}\right)}^{2}}\right)}}{\frac{4 \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}}}
\begin{array}{l}
t_0 := \left(x-scale \cdot 0.25\right) \cdot 0\\
t_1 := \cos \left(\pi \cdot \left(angle \cdot 0.005555555555555556\right)\right)\\
t_2 := 0.005555555555555556 \cdot \left(\pi \cdot angle\right)\\
\mathbf{if}\;x-scale \leq -2.1 \cdot 10^{-29}:\\
\;\;\;\;t_0\\
\mathbf{elif}\;x-scale \leq -1.1 \cdot 10^{-118}:\\
\;\;\;\;0.25 \cdot \left|\left(\sqrt{8} \cdot \left(x-scale \cdot y-scale\right)\right) \cdot \mathsf{hypot}\left(t_1 \cdot \frac{a}{y-scale}, \frac{a}{y-scale}\right)\right|\\
\mathbf{elif}\;x-scale \leq 7.5 \cdot 10^{-134}:\\
\;\;\;\;t_0\\
\mathbf{elif}\;x-scale \leq 5.2 \cdot 10^{-27}:\\
\;\;\;\;\left(x-scale \cdot 0.25\right) \cdot \left|a \cdot 4\right|\\
\mathbf{elif}\;x-scale \leq 4 \cdot 10^{-25}:\\
\;\;\;\;0.25 \cdot \left(\left(x-scale \cdot \left(y-scale \cdot \left(\sqrt{8} \cdot b\right)\right)\right) \cdot \sqrt{\frac{{\sin t_2}^{2}}{y-scale \cdot y-scale} + \left(\frac{{\cos t_2}^{2}}{x-scale \cdot x-scale} - \frac{{t_1}^{2}}{x-scale \cdot x-scale}\right)}\right)\\
\mathbf{elif}\;x-scale \leq 9.5 \cdot 10^{+107}:\\
\;\;\;\;t_0\\
\mathbf{else}:\\
\;\;\;\;\left(x-scale \cdot 0.25\right) \cdot \sqrt{a \cdot \left(a \cdot 16\right)}\\
\end{array}
Results
if x-scale < -2.09999999999999989e-29 or -1.09999999999999992e-118 < x-scale < 7.50000000000000048e-134 or 4.00000000000000015e-25 < x-scale < 9.50000000000000019e107Initial program 0.1%
Simplified1.0%
[Start]0.1 | \[ \frac{-\sqrt{\left(\left(2 \cdot \frac{4 \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}}\right) \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)\right) \cdot \left(\left(\frac{\frac{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{x-scale}}{x-scale} + \frac{\frac{{\left(a \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{y-scale}}{y-scale}\right) - \sqrt{{\left(\frac{\frac{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{x-scale}}{x-scale} - \frac{\frac{{\left(a \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{y-scale}}{y-scale}\right)}^{2} + {\left(\frac{\frac{\left(\left(2 \cdot \left({b}^{2} - {a}^{2}\right)\right) \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right) \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)}{x-scale}}{y-scale}\right)}^{2}}\right)}}{\frac{4 \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}}}
\] |
|---|
Taylor expanded in angle around 0 25.8%
Simplified25.8%
[Start]25.8 | \[ 0.25 \cdot \left(x-scale \cdot \left(\sqrt{2} \cdot \left(a \cdot \sqrt{8}\right)\right)\right)
\] |
|---|---|
associate-*r* [=>]25.8 | \[ \color{blue}{\left(0.25 \cdot x-scale\right) \cdot \left(\sqrt{2} \cdot \left(a \cdot \sqrt{8}\right)\right)}
\] |
*-commutative [=>]25.8 | \[ \left(0.25 \cdot x-scale\right) \cdot \color{blue}{\left(\left(a \cdot \sqrt{8}\right) \cdot \sqrt{2}\right)}
\] |
Applied egg-rr26.8%
[Start]25.8 | \[ \left(0.25 \cdot x-scale\right) \cdot \left(\left(a \cdot \sqrt{8}\right) \cdot \sqrt{2}\right)
\] |
|---|---|
expm1-log1p-u [=>]23.5 | \[ \left(0.25 \cdot x-scale\right) \cdot \color{blue}{\mathsf{expm1}\left(\mathsf{log1p}\left(\left(a \cdot \sqrt{8}\right) \cdot \sqrt{2}\right)\right)}
\] |
expm1-udef [=>]26.8 | \[ \left(0.25 \cdot x-scale\right) \cdot \color{blue}{\left(e^{\mathsf{log1p}\left(\left(a \cdot \sqrt{8}\right) \cdot \sqrt{2}\right)} - 1\right)}
\] |
associate-*l* [=>]26.8 | \[ \left(0.25 \cdot x-scale\right) \cdot \left(e^{\mathsf{log1p}\left(\color{blue}{a \cdot \left(\sqrt{8} \cdot \sqrt{2}\right)}\right)} - 1\right)
\] |
sqrt-unprod [=>]26.8 | \[ \left(0.25 \cdot x-scale\right) \cdot \left(e^{\mathsf{log1p}\left(a \cdot \color{blue}{\sqrt{8 \cdot 2}}\right)} - 1\right)
\] |
metadata-eval [=>]26.8 | \[ \left(0.25 \cdot x-scale\right) \cdot \left(e^{\mathsf{log1p}\left(a \cdot \sqrt{\color{blue}{16}}\right)} - 1\right)
\] |
metadata-eval [=>]26.8 | \[ \left(0.25 \cdot x-scale\right) \cdot \left(e^{\mathsf{log1p}\left(a \cdot \color{blue}{4}\right)} - 1\right)
\] |
Taylor expanded in a around 0 36.0%
if -2.09999999999999989e-29 < x-scale < -1.09999999999999992e-118Initial program 0.1%
Simplified2.1%
[Start]0.1 | \[ \frac{-\sqrt{\left(\left(2 \cdot \frac{4 \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}}\right) \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)\right) \cdot \left(\left(\frac{\frac{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{x-scale}}{x-scale} + \frac{\frac{{\left(a \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{y-scale}}{y-scale}\right) - \sqrt{{\left(\frac{\frac{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{x-scale}}{x-scale} - \frac{\frac{{\left(a \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{y-scale}}{y-scale}\right)}^{2} + {\left(\frac{\frac{\left(\left(2 \cdot \left({b}^{2} - {a}^{2}\right)\right) \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right) \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)}{x-scale}}{y-scale}\right)}^{2}}\right)}}{\frac{4 \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}}}
\] |
|---|
Taylor expanded in angle around 0 4.6%
Simplified4.6%
[Start]4.6 | \[ {\left(x-scale \cdot y-scale\right)}^{2} \cdot \left(\frac{-0.25}{b \cdot a} \cdot \frac{\sqrt{b \cdot \left(\left(a \cdot \left(a \cdot \left(\frac{-8 \cdot \left(b \cdot \left(a \cdot \left(b \cdot a\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}} \cdot \left(-b\right)\right)\right)\right) \cdot \left(\frac{{\left(a \cdot \cos \left(\frac{angle}{\frac{180}{\pi}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{\frac{180}{\pi}}\right)\right)}^{2}}{y-scale \cdot y-scale} + \frac{{a}^{2}}{{y-scale}^{2}}\right)\right)}}{b \cdot \left(-a\right)}\right)
\] |
|---|---|
unpow2 [=>]4.6 | \[ {\left(x-scale \cdot y-scale\right)}^{2} \cdot \left(\frac{-0.25}{b \cdot a} \cdot \frac{\sqrt{b \cdot \left(\left(a \cdot \left(a \cdot \left(\frac{-8 \cdot \left(b \cdot \left(a \cdot \left(b \cdot a\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}} \cdot \left(-b\right)\right)\right)\right) \cdot \left(\frac{{\left(a \cdot \cos \left(\frac{angle}{\frac{180}{\pi}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{\frac{180}{\pi}}\right)\right)}^{2}}{y-scale \cdot y-scale} + \frac{\color{blue}{a \cdot a}}{{y-scale}^{2}}\right)\right)}}{b \cdot \left(-a\right)}\right)
\] |
unpow2 [=>]4.6 | \[ {\left(x-scale \cdot y-scale\right)}^{2} \cdot \left(\frac{-0.25}{b \cdot a} \cdot \frac{\sqrt{b \cdot \left(\left(a \cdot \left(a \cdot \left(\frac{-8 \cdot \left(b \cdot \left(a \cdot \left(b \cdot a\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}} \cdot \left(-b\right)\right)\right)\right) \cdot \left(\frac{{\left(a \cdot \cos \left(\frac{angle}{\frac{180}{\pi}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{\frac{180}{\pi}}\right)\right)}^{2}}{y-scale \cdot y-scale} + \frac{a \cdot a}{\color{blue}{y-scale \cdot y-scale}}\right)\right)}}{b \cdot \left(-a\right)}\right)
\] |
Taylor expanded in b around 0 16.3%
Simplified19.1%
[Start]16.3 | \[ 0.25 \cdot \left(\left(x-scale \cdot \left(y-scale \cdot \sqrt{8}\right)\right) \cdot \sqrt{\frac{{a}^{2} \cdot {\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{y-scale}^{2}} + \frac{{a}^{2}}{{y-scale}^{2}}}\right)
\] |
|---|---|
*-commutative [=>]16.3 | \[ \color{blue}{\left(\left(x-scale \cdot \left(y-scale \cdot \sqrt{8}\right)\right) \cdot \sqrt{\frac{{a}^{2} \cdot {\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{y-scale}^{2}} + \frac{{a}^{2}}{{y-scale}^{2}}}\right) \cdot 0.25}
\] |
associate-*l* [=>]16.3 | \[ \color{blue}{\left(x-scale \cdot \left(y-scale \cdot \sqrt{8}\right)\right) \cdot \left(\sqrt{\frac{{a}^{2} \cdot {\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{y-scale}^{2}} + \frac{{a}^{2}}{{y-scale}^{2}}} \cdot 0.25\right)}
\] |
associate-*r* [=>]16.3 | \[ \color{blue}{\left(\left(x-scale \cdot y-scale\right) \cdot \sqrt{8}\right)} \cdot \left(\sqrt{\frac{{a}^{2} \cdot {\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{y-scale}^{2}} + \frac{{a}^{2}}{{y-scale}^{2}}} \cdot 0.25\right)
\] |
*-commutative [<=]16.3 | \[ \left(\color{blue}{\left(y-scale \cdot x-scale\right)} \cdot \sqrt{8}\right) \cdot \left(\sqrt{\frac{{a}^{2} \cdot {\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{y-scale}^{2}} + \frac{{a}^{2}}{{y-scale}^{2}}} \cdot 0.25\right)
\] |
associate-*r* [<=]16.3 | \[ \color{blue}{\left(y-scale \cdot \left(x-scale \cdot \sqrt{8}\right)\right)} \cdot \left(\sqrt{\frac{{a}^{2} \cdot {\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{y-scale}^{2}} + \frac{{a}^{2}}{{y-scale}^{2}}} \cdot 0.25\right)
\] |
Applied egg-rr32.4%
[Start]19.1 | \[ \left(y-scale \cdot \left(x-scale \cdot \sqrt{8}\right)\right) \cdot \left(\sqrt{\frac{a}{y-scale \cdot \frac{y-scale}{a}} \cdot {\cos \left(\pi \cdot \left(0.005555555555555556 \cdot angle\right)\right)}^{2} + \frac{a}{y-scale \cdot \frac{y-scale}{a}}} \cdot 0.25\right)
\] |
|---|---|
add-sqr-sqrt [=>]18.3 | \[ \color{blue}{\sqrt{\left(y-scale \cdot \left(x-scale \cdot \sqrt{8}\right)\right) \cdot \left(\sqrt{\frac{a}{y-scale \cdot \frac{y-scale}{a}} \cdot {\cos \left(\pi \cdot \left(0.005555555555555556 \cdot angle\right)\right)}^{2} + \frac{a}{y-scale \cdot \frac{y-scale}{a}}} \cdot 0.25\right)} \cdot \sqrt{\left(y-scale \cdot \left(x-scale \cdot \sqrt{8}\right)\right) \cdot \left(\sqrt{\frac{a}{y-scale \cdot \frac{y-scale}{a}} \cdot {\cos \left(\pi \cdot \left(0.005555555555555556 \cdot angle\right)\right)}^{2} + \frac{a}{y-scale \cdot \frac{y-scale}{a}}} \cdot 0.25\right)}}
\] |
sqrt-unprod [=>]22.4 | \[ \color{blue}{\sqrt{\left(\left(y-scale \cdot \left(x-scale \cdot \sqrt{8}\right)\right) \cdot \left(\sqrt{\frac{a}{y-scale \cdot \frac{y-scale}{a}} \cdot {\cos \left(\pi \cdot \left(0.005555555555555556 \cdot angle\right)\right)}^{2} + \frac{a}{y-scale \cdot \frac{y-scale}{a}}} \cdot 0.25\right)\right) \cdot \left(\left(y-scale \cdot \left(x-scale \cdot \sqrt{8}\right)\right) \cdot \left(\sqrt{\frac{a}{y-scale \cdot \frac{y-scale}{a}} \cdot {\cos \left(\pi \cdot \left(0.005555555555555556 \cdot angle\right)\right)}^{2} + \frac{a}{y-scale \cdot \frac{y-scale}{a}}} \cdot 0.25\right)\right)}}
\] |
pow2 [=>]22.4 | \[ \sqrt{\color{blue}{{\left(\left(y-scale \cdot \left(x-scale \cdot \sqrt{8}\right)\right) \cdot \left(\sqrt{\frac{a}{y-scale \cdot \frac{y-scale}{a}} \cdot {\cos \left(\pi \cdot \left(0.005555555555555556 \cdot angle\right)\right)}^{2} + \frac{a}{y-scale \cdot \frac{y-scale}{a}}} \cdot 0.25\right)\right)}^{2}}}
\] |
Simplified37.9%
[Start]32.4 | \[ \sqrt{{\left(\mathsf{hypot}\left(\cos \left(\pi \cdot \left(0.005555555555555556 \cdot angle\right)\right) \cdot \frac{a}{y-scale}, \frac{a}{y-scale}\right) \cdot \left(0.25 \cdot \left(\sqrt{8} \cdot \left(y-scale \cdot x-scale\right)\right)\right)\right)}^{2}}
\] |
|---|---|
unpow2 [=>]32.4 | \[ \sqrt{\color{blue}{\left(\mathsf{hypot}\left(\cos \left(\pi \cdot \left(0.005555555555555556 \cdot angle\right)\right) \cdot \frac{a}{y-scale}, \frac{a}{y-scale}\right) \cdot \left(0.25 \cdot \left(\sqrt{8} \cdot \left(y-scale \cdot x-scale\right)\right)\right)\right) \cdot \left(\mathsf{hypot}\left(\cos \left(\pi \cdot \left(0.005555555555555556 \cdot angle\right)\right) \cdot \frac{a}{y-scale}, \frac{a}{y-scale}\right) \cdot \left(0.25 \cdot \left(\sqrt{8} \cdot \left(y-scale \cdot x-scale\right)\right)\right)\right)}}
\] |
rem-sqrt-square [=>]37.9 | \[ \color{blue}{\left|\mathsf{hypot}\left(\cos \left(\pi \cdot \left(0.005555555555555556 \cdot angle\right)\right) \cdot \frac{a}{y-scale}, \frac{a}{y-scale}\right) \cdot \left(0.25 \cdot \left(\sqrt{8} \cdot \left(y-scale \cdot x-scale\right)\right)\right)\right|}
\] |
*-commutative [=>]37.9 | \[ \left|\color{blue}{\left(0.25 \cdot \left(\sqrt{8} \cdot \left(y-scale \cdot x-scale\right)\right)\right) \cdot \mathsf{hypot}\left(\cos \left(\pi \cdot \left(0.005555555555555556 \cdot angle\right)\right) \cdot \frac{a}{y-scale}, \frac{a}{y-scale}\right)}\right|
\] |
associate-*l* [=>]37.9 | \[ \left|\color{blue}{0.25 \cdot \left(\left(\sqrt{8} \cdot \left(y-scale \cdot x-scale\right)\right) \cdot \mathsf{hypot}\left(\cos \left(\pi \cdot \left(0.005555555555555556 \cdot angle\right)\right) \cdot \frac{a}{y-scale}, \frac{a}{y-scale}\right)\right)}\right|
\] |
*-commutative [=>]37.9 | \[ \left|0.25 \cdot \left(\left(\sqrt{8} \cdot \left(y-scale \cdot x-scale\right)\right) \cdot \mathsf{hypot}\left(\cos \left(\pi \cdot \color{blue}{\left(angle \cdot 0.005555555555555556\right)}\right) \cdot \frac{a}{y-scale}, \frac{a}{y-scale}\right)\right)\right|
\] |
if 7.50000000000000048e-134 < x-scale < 5.20000000000000034e-27Initial program 0.1%
Simplified3.1%
[Start]0.1 | \[ \frac{-\sqrt{\left(\left(2 \cdot \frac{4 \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}}\right) \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)\right) \cdot \left(\left(\frac{\frac{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{x-scale}}{x-scale} + \frac{\frac{{\left(a \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{y-scale}}{y-scale}\right) - \sqrt{{\left(\frac{\frac{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{x-scale}}{x-scale} - \frac{\frac{{\left(a \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{y-scale}}{y-scale}\right)}^{2} + {\left(\frac{\frac{\left(\left(2 \cdot \left({b}^{2} - {a}^{2}\right)\right) \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right) \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)}{x-scale}}{y-scale}\right)}^{2}}\right)}}{\frac{4 \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}}}
\] |
|---|
Taylor expanded in angle around 0 26.2%
Simplified26.2%
[Start]26.2 | \[ 0.25 \cdot \left(x-scale \cdot \left(\sqrt{2} \cdot \left(a \cdot \sqrt{8}\right)\right)\right)
\] |
|---|---|
associate-*r* [=>]26.2 | \[ \color{blue}{\left(0.25 \cdot x-scale\right) \cdot \left(\sqrt{2} \cdot \left(a \cdot \sqrt{8}\right)\right)}
\] |
*-commutative [=>]26.2 | \[ \left(0.25 \cdot x-scale\right) \cdot \color{blue}{\left(\left(a \cdot \sqrt{8}\right) \cdot \sqrt{2}\right)}
\] |
Applied egg-rr26.5%
[Start]26.2 | \[ \left(0.25 \cdot x-scale\right) \cdot \left(\left(a \cdot \sqrt{8}\right) \cdot \sqrt{2}\right)
\] |
|---|---|
expm1-log1p-u [=>]25.5 | \[ \left(0.25 \cdot x-scale\right) \cdot \color{blue}{\mathsf{expm1}\left(\mathsf{log1p}\left(\left(a \cdot \sqrt{8}\right) \cdot \sqrt{2}\right)\right)}
\] |
expm1-udef [=>]26.5 | \[ \left(0.25 \cdot x-scale\right) \cdot \color{blue}{\left(e^{\mathsf{log1p}\left(\left(a \cdot \sqrt{8}\right) \cdot \sqrt{2}\right)} - 1\right)}
\] |
associate-*l* [=>]26.5 | \[ \left(0.25 \cdot x-scale\right) \cdot \left(e^{\mathsf{log1p}\left(\color{blue}{a \cdot \left(\sqrt{8} \cdot \sqrt{2}\right)}\right)} - 1\right)
\] |
sqrt-unprod [=>]26.5 | \[ \left(0.25 \cdot x-scale\right) \cdot \left(e^{\mathsf{log1p}\left(a \cdot \color{blue}{\sqrt{8 \cdot 2}}\right)} - 1\right)
\] |
metadata-eval [=>]26.5 | \[ \left(0.25 \cdot x-scale\right) \cdot \left(e^{\mathsf{log1p}\left(a \cdot \sqrt{\color{blue}{16}}\right)} - 1\right)
\] |
metadata-eval [=>]26.5 | \[ \left(0.25 \cdot x-scale\right) \cdot \left(e^{\mathsf{log1p}\left(a \cdot \color{blue}{4}\right)} - 1\right)
\] |
Applied egg-rr32.4%
[Start]26.5 | \[ \left(0.25 \cdot x-scale\right) \cdot \left(e^{\mathsf{log1p}\left(a \cdot 4\right)} - 1\right)
\] |
|---|---|
expm1-def [=>]25.5 | \[ \left(0.25 \cdot x-scale\right) \cdot \color{blue}{\mathsf{expm1}\left(\mathsf{log1p}\left(a \cdot 4\right)\right)}
\] |
expm1-log1p-u [<=]26.3 | \[ \left(0.25 \cdot x-scale\right) \cdot \color{blue}{\left(a \cdot 4\right)}
\] |
add-sqr-sqrt [=>]19.7 | \[ \left(0.25 \cdot x-scale\right) \cdot \color{blue}{\left(\sqrt{a \cdot 4} \cdot \sqrt{a \cdot 4}\right)}
\] |
sqrt-unprod [=>]32.3 | \[ \left(0.25 \cdot x-scale\right) \cdot \color{blue}{\sqrt{\left(a \cdot 4\right) \cdot \left(a \cdot 4\right)}}
\] |
*-commutative [=>]32.3 | \[ \left(0.25 \cdot x-scale\right) \cdot \sqrt{\color{blue}{\left(4 \cdot a\right)} \cdot \left(a \cdot 4\right)}
\] |
*-commutative [=>]32.3 | \[ \left(0.25 \cdot x-scale\right) \cdot \sqrt{\left(4 \cdot a\right) \cdot \color{blue}{\left(4 \cdot a\right)}}
\] |
swap-sqr [=>]32.4 | \[ \left(0.25 \cdot x-scale\right) \cdot \sqrt{\color{blue}{\left(4 \cdot 4\right) \cdot \left(a \cdot a\right)}}
\] |
metadata-eval [=>]32.4 | \[ \left(0.25 \cdot x-scale\right) \cdot \sqrt{\color{blue}{16} \cdot \left(a \cdot a\right)}
\] |
Simplified36.7%
[Start]32.4 | \[ \left(0.25 \cdot x-scale\right) \cdot \sqrt{16 \cdot \left(a \cdot a\right)}
\] |
|---|---|
*-commutative [=>]32.4 | \[ \left(0.25 \cdot x-scale\right) \cdot \sqrt{\color{blue}{\left(a \cdot a\right) \cdot 16}}
\] |
metadata-eval [<=]32.4 | \[ \left(0.25 \cdot x-scale\right) \cdot \sqrt{\left(a \cdot a\right) \cdot \color{blue}{\left(4 \cdot 4\right)}}
\] |
swap-sqr [<=]32.3 | \[ \left(0.25 \cdot x-scale\right) \cdot \sqrt{\color{blue}{\left(a \cdot 4\right) \cdot \left(a \cdot 4\right)}}
\] |
rem-sqrt-square [=>]36.7 | \[ \left(0.25 \cdot x-scale\right) \cdot \color{blue}{\left|a \cdot 4\right|}
\] |
*-commutative [<=]36.7 | \[ \left(0.25 \cdot x-scale\right) \cdot \left|\color{blue}{4 \cdot a}\right|
\] |
if 5.20000000000000034e-27 < x-scale < 4.00000000000000015e-25Initial program 0.3%
Simplified0.3%
[Start]0.3 | \[ \frac{-\sqrt{\left(\left(2 \cdot \frac{4 \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}}\right) \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)\right) \cdot \left(\left(\frac{\frac{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{x-scale}}{x-scale} + \frac{\frac{{\left(a \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{y-scale}}{y-scale}\right) - \sqrt{{\left(\frac{\frac{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{x-scale}}{x-scale} - \frac{\frac{{\left(a \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{y-scale}}{y-scale}\right)}^{2} + {\left(\frac{\frac{\left(\left(2 \cdot \left({b}^{2} - {a}^{2}\right)\right) \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right) \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)}{x-scale}}{y-scale}\right)}^{2}}\right)}}{\frac{4 \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}}}
\] |
|---|
Taylor expanded in b around inf 4.4%
Simplified3.9%
[Start]4.4 | \[ 0.25 \cdot \left(\left(x-scale \cdot \left(y-scale \cdot \left(b \cdot \sqrt{8}\right)\right)\right) \cdot \sqrt{\left(\frac{{\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{x-scale}^{2}} + \frac{{\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{y-scale}^{2}}\right) - \sqrt{4 \cdot \frac{{\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2} \cdot {\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{y-scale}^{2} \cdot {x-scale}^{2}} + {\left(\frac{{\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{x-scale}^{2}} - \frac{{\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{y-scale}^{2}}\right)}^{2}}}\right)
\] |
|---|
Taylor expanded in x-scale around 0 4.0%
Simplified3.8%
[Start]4.0 | \[ 0.25 \cdot \left(\left(x-scale \cdot \left(y-scale \cdot \left(b \cdot \sqrt{8}\right)\right)\right) \cdot \sqrt{\frac{{\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{y-scale \cdot y-scale} + \left(\frac{{\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{x-scale \cdot x-scale} - \frac{{\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{x-scale}^{2}}\right)}\right)
\] |
|---|---|
unpow2 [=>]4.0 | \[ 0.25 \cdot \left(\left(x-scale \cdot \left(y-scale \cdot \left(b \cdot \sqrt{8}\right)\right)\right) \cdot \sqrt{\frac{{\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{y-scale \cdot y-scale} + \left(\frac{{\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{x-scale \cdot x-scale} - \frac{{\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{\color{blue}{x-scale \cdot x-scale}}\right)}\right)
\] |
associate-*r* [=>]3.8 | \[ 0.25 \cdot \left(\left(x-scale \cdot \left(y-scale \cdot \left(b \cdot \sqrt{8}\right)\right)\right) \cdot \sqrt{\frac{{\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{y-scale \cdot y-scale} + \left(\frac{{\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{x-scale \cdot x-scale} - \frac{{\cos \color{blue}{\left(\left(0.005555555555555556 \cdot angle\right) \cdot \pi\right)}}^{2}}{x-scale \cdot x-scale}\right)}\right)
\] |
if 9.50000000000000019e107 < x-scale Initial program 0.0%
Simplified0.8%
[Start]0.0 | \[ \frac{-\sqrt{\left(\left(2 \cdot \frac{4 \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}}\right) \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)\right) \cdot \left(\left(\frac{\frac{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{x-scale}}{x-scale} + \frac{\frac{{\left(a \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{y-scale}}{y-scale}\right) - \sqrt{{\left(\frac{\frac{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{x-scale}}{x-scale} - \frac{\frac{{\left(a \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{y-scale}}{y-scale}\right)}^{2} + {\left(\frac{\frac{\left(\left(2 \cdot \left({b}^{2} - {a}^{2}\right)\right) \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right) \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)}{x-scale}}{y-scale}\right)}^{2}}\right)}}{\frac{4 \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}}}
\] |
|---|
Taylor expanded in angle around 0 7.3%
Simplified7.3%
[Start]7.3 | \[ 0.25 \cdot \left(x-scale \cdot \left(\sqrt{2} \cdot \left(a \cdot \sqrt{8}\right)\right)\right)
\] |
|---|---|
associate-*r* [=>]7.3 | \[ \color{blue}{\left(0.25 \cdot x-scale\right) \cdot \left(\sqrt{2} \cdot \left(a \cdot \sqrt{8}\right)\right)}
\] |
*-commutative [=>]7.3 | \[ \left(0.25 \cdot x-scale\right) \cdot \color{blue}{\left(\left(a \cdot \sqrt{8}\right) \cdot \sqrt{2}\right)}
\] |
Applied egg-rr13.1%
[Start]7.3 | \[ \left(0.25 \cdot x-scale\right) \cdot \left(\left(a \cdot \sqrt{8}\right) \cdot \sqrt{2}\right)
\] |
|---|---|
expm1-log1p-u [=>]7.1 | \[ \left(0.25 \cdot x-scale\right) \cdot \color{blue}{\mathsf{expm1}\left(\mathsf{log1p}\left(\left(a \cdot \sqrt{8}\right) \cdot \sqrt{2}\right)\right)}
\] |
expm1-udef [=>]13.1 | \[ \left(0.25 \cdot x-scale\right) \cdot \color{blue}{\left(e^{\mathsf{log1p}\left(\left(a \cdot \sqrt{8}\right) \cdot \sqrt{2}\right)} - 1\right)}
\] |
associate-*l* [=>]13.1 | \[ \left(0.25 \cdot x-scale\right) \cdot \left(e^{\mathsf{log1p}\left(\color{blue}{a \cdot \left(\sqrt{8} \cdot \sqrt{2}\right)}\right)} - 1\right)
\] |
sqrt-unprod [=>]13.1 | \[ \left(0.25 \cdot x-scale\right) \cdot \left(e^{\mathsf{log1p}\left(a \cdot \color{blue}{\sqrt{8 \cdot 2}}\right)} - 1\right)
\] |
metadata-eval [=>]13.1 | \[ \left(0.25 \cdot x-scale\right) \cdot \left(e^{\mathsf{log1p}\left(a \cdot \sqrt{\color{blue}{16}}\right)} - 1\right)
\] |
metadata-eval [=>]13.1 | \[ \left(0.25 \cdot x-scale\right) \cdot \left(e^{\mathsf{log1p}\left(a \cdot \color{blue}{4}\right)} - 1\right)
\] |
Applied egg-rr13.6%
[Start]13.1 | \[ \left(0.25 \cdot x-scale\right) \cdot \left(e^{\mathsf{log1p}\left(a \cdot 4\right)} - 1\right)
\] |
|---|---|
expm1-def [=>]7.2 | \[ \left(0.25 \cdot x-scale\right) \cdot \color{blue}{\mathsf{expm1}\left(\mathsf{log1p}\left(a \cdot 4\right)\right)}
\] |
expm1-log1p-u [<=]7.3 | \[ \left(0.25 \cdot x-scale\right) \cdot \color{blue}{\left(a \cdot 4\right)}
\] |
add-sqr-sqrt [=>]6.7 | \[ \left(0.25 \cdot x-scale\right) \cdot \color{blue}{\left(\sqrt{a \cdot 4} \cdot \sqrt{a \cdot 4}\right)}
\] |
sqrt-unprod [=>]13.6 | \[ \left(0.25 \cdot x-scale\right) \cdot \color{blue}{\sqrt{\left(a \cdot 4\right) \cdot \left(a \cdot 4\right)}}
\] |
*-commutative [=>]13.6 | \[ \left(0.25 \cdot x-scale\right) \cdot \sqrt{\color{blue}{\left(4 \cdot a\right)} \cdot \left(a \cdot 4\right)}
\] |
*-commutative [=>]13.6 | \[ \left(0.25 \cdot x-scale\right) \cdot \sqrt{\left(4 \cdot a\right) \cdot \color{blue}{\left(4 \cdot a\right)}}
\] |
swap-sqr [=>]13.6 | \[ \left(0.25 \cdot x-scale\right) \cdot \sqrt{\color{blue}{\left(4 \cdot 4\right) \cdot \left(a \cdot a\right)}}
\] |
metadata-eval [=>]13.6 | \[ \left(0.25 \cdot x-scale\right) \cdot \sqrt{\color{blue}{16} \cdot \left(a \cdot a\right)}
\] |
Simplified13.6%
[Start]13.6 | \[ \left(0.25 \cdot x-scale\right) \cdot \sqrt{16 \cdot \left(a \cdot a\right)}
\] |
|---|---|
*-commutative [=>]13.6 | \[ \left(0.25 \cdot x-scale\right) \cdot \sqrt{\color{blue}{\left(a \cdot a\right) \cdot 16}}
\] |
associate-*l* [=>]13.6 | \[ \left(0.25 \cdot x-scale\right) \cdot \sqrt{\color{blue}{a \cdot \left(a \cdot 16\right)}}
\] |
Final simplification32.6%
| Alternative 1 | |
|---|---|
| Accuracy | 35.3% |
| Cost | 33480 |
| Alternative 2 | |
|---|---|
| Accuracy | 35.3% |
| Cost | 33480 |
| Alternative 3 | |
|---|---|
| Accuracy | 33.3% |
| Cost | 7113 |
| Alternative 4 | |
|---|---|
| Accuracy | 34.4% |
| Cost | 580 |
| Alternative 5 | |
|---|---|
| Accuracy | 23.0% |
| Cost | 448 |
herbie shell --seed 2023135
(FPCore (a b angle x-scale y-scale)
:name "b from scale-rotated-ellipse"
:precision binary64
(/ (- (sqrt (* (* (* 2.0 (/ (* 4.0 (* (* b a) (* b (- a)))) (pow (* x-scale y-scale) 2.0))) (* (* b a) (* b (- a)))) (- (+ (/ (/ (+ (pow (* a (sin (* (/ angle 180.0) PI))) 2.0) (pow (* b (cos (* (/ angle 180.0) PI))) 2.0)) x-scale) x-scale) (/ (/ (+ (pow (* a (cos (* (/ angle 180.0) PI))) 2.0) (pow (* b (sin (* (/ angle 180.0) PI))) 2.0)) y-scale) y-scale)) (sqrt (+ (pow (- (/ (/ (+ (pow (* a (sin (* (/ angle 180.0) PI))) 2.0) (pow (* b (cos (* (/ angle 180.0) PI))) 2.0)) x-scale) x-scale) (/ (/ (+ (pow (* a (cos (* (/ angle 180.0) PI))) 2.0) (pow (* b (sin (* (/ angle 180.0) PI))) 2.0)) y-scale) y-scale)) 2.0) (pow (/ (/ (* (* (* 2.0 (- (pow b 2.0) (pow a 2.0))) (sin (* (/ angle 180.0) PI))) (cos (* (/ angle 180.0) PI))) x-scale) y-scale) 2.0))))))) (/ (* 4.0 (* (* b a) (* b (- a)))) (pow (* x-scale y-scale) 2.0))))