| Alternative 1 | |
|---|---|
| Error | 39.8 |
| Cost | 65732 |
(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 (sqrt 8.0)))
(t_1 (* 0.005555555555555556 (* PI angle)))
(t_2 (* (sqrt 2.0) (* a (cos t_1)))))
(if (<= x-scale -1.75e+61)
(*
(*
a
(*
(sqrt 2.0)
(* (sqrt 8.0) (cos (* angle (* PI 0.005555555555555556))))))
(* x-scale -0.25))
(if (<= x-scale -7.2e-25)
(*
(* x-scale 0.25)
(*
(sqrt 2.0)
(* a (* (sqrt 8.0) (cos (* PI (* 0.005555555555555556 angle)))))))
(if (<= x-scale -3.65e-112)
(* -0.25 (* t_0 t_2))
(if (<= x-scale 1.8e-101)
(fabs (* (sqrt 8.0) (* (sqrt 2.0) (* b (* 0.25 y-scale)))))
(* 0.25 (* t_0 (hypot t_2 (* (sqrt 2.0) (* b (sin t_1))))))))))))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 * sqrt(8.0);
double t_1 = 0.005555555555555556 * (((double) M_PI) * angle);
double t_2 = sqrt(2.0) * (a * cos(t_1));
double tmp;
if (x_45_scale <= -1.75e+61) {
tmp = (a * (sqrt(2.0) * (sqrt(8.0) * cos((angle * (((double) M_PI) * 0.005555555555555556)))))) * (x_45_scale * -0.25);
} else if (x_45_scale <= -7.2e-25) {
tmp = (x_45_scale * 0.25) * (sqrt(2.0) * (a * (sqrt(8.0) * cos((((double) M_PI) * (0.005555555555555556 * angle))))));
} else if (x_45_scale <= -3.65e-112) {
tmp = -0.25 * (t_0 * t_2);
} else if (x_45_scale <= 1.8e-101) {
tmp = fabs((sqrt(8.0) * (sqrt(2.0) * (b * (0.25 * y_45_scale)))));
} else {
tmp = 0.25 * (t_0 * hypot(t_2, (sqrt(2.0) * (b * sin(t_1)))));
}
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 * Math.sqrt(8.0);
double t_1 = 0.005555555555555556 * (Math.PI * angle);
double t_2 = Math.sqrt(2.0) * (a * Math.cos(t_1));
double tmp;
if (x_45_scale <= -1.75e+61) {
tmp = (a * (Math.sqrt(2.0) * (Math.sqrt(8.0) * Math.cos((angle * (Math.PI * 0.005555555555555556)))))) * (x_45_scale * -0.25);
} else if (x_45_scale <= -7.2e-25) {
tmp = (x_45_scale * 0.25) * (Math.sqrt(2.0) * (a * (Math.sqrt(8.0) * Math.cos((Math.PI * (0.005555555555555556 * angle))))));
} else if (x_45_scale <= -3.65e-112) {
tmp = -0.25 * (t_0 * t_2);
} else if (x_45_scale <= 1.8e-101) {
tmp = Math.abs((Math.sqrt(8.0) * (Math.sqrt(2.0) * (b * (0.25 * y_45_scale)))));
} else {
tmp = 0.25 * (t_0 * Math.hypot(t_2, (Math.sqrt(2.0) * (b * Math.sin(t_1)))));
}
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 * math.sqrt(8.0) t_1 = 0.005555555555555556 * (math.pi * angle) t_2 = math.sqrt(2.0) * (a * math.cos(t_1)) tmp = 0 if x_45_scale <= -1.75e+61: tmp = (a * (math.sqrt(2.0) * (math.sqrt(8.0) * math.cos((angle * (math.pi * 0.005555555555555556)))))) * (x_45_scale * -0.25) elif x_45_scale <= -7.2e-25: tmp = (x_45_scale * 0.25) * (math.sqrt(2.0) * (a * (math.sqrt(8.0) * math.cos((math.pi * (0.005555555555555556 * angle)))))) elif x_45_scale <= -3.65e-112: tmp = -0.25 * (t_0 * t_2) elif x_45_scale <= 1.8e-101: tmp = math.fabs((math.sqrt(8.0) * (math.sqrt(2.0) * (b * (0.25 * y_45_scale))))) else: tmp = 0.25 * (t_0 * math.hypot(t_2, (math.sqrt(2.0) * (b * math.sin(t_1))))) 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(x_45_scale * sqrt(8.0)) t_1 = Float64(0.005555555555555556 * Float64(pi * angle)) t_2 = Float64(sqrt(2.0) * Float64(a * cos(t_1))) tmp = 0.0 if (x_45_scale <= -1.75e+61) tmp = Float64(Float64(a * Float64(sqrt(2.0) * Float64(sqrt(8.0) * cos(Float64(angle * Float64(pi * 0.005555555555555556)))))) * Float64(x_45_scale * -0.25)); elseif (x_45_scale <= -7.2e-25) tmp = Float64(Float64(x_45_scale * 0.25) * Float64(sqrt(2.0) * Float64(a * Float64(sqrt(8.0) * cos(Float64(pi * Float64(0.005555555555555556 * angle))))))); elseif (x_45_scale <= -3.65e-112) tmp = Float64(-0.25 * Float64(t_0 * t_2)); elseif (x_45_scale <= 1.8e-101) tmp = abs(Float64(sqrt(8.0) * Float64(sqrt(2.0) * Float64(b * Float64(0.25 * y_45_scale))))); else tmp = Float64(0.25 * Float64(t_0 * hypot(t_2, Float64(sqrt(2.0) * Float64(b * sin(t_1)))))); 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 * sqrt(8.0); t_1 = 0.005555555555555556 * (pi * angle); t_2 = sqrt(2.0) * (a * cos(t_1)); tmp = 0.0; if (x_45_scale <= -1.75e+61) tmp = (a * (sqrt(2.0) * (sqrt(8.0) * cos((angle * (pi * 0.005555555555555556)))))) * (x_45_scale * -0.25); elseif (x_45_scale <= -7.2e-25) tmp = (x_45_scale * 0.25) * (sqrt(2.0) * (a * (sqrt(8.0) * cos((pi * (0.005555555555555556 * angle)))))); elseif (x_45_scale <= -3.65e-112) tmp = -0.25 * (t_0 * t_2); elseif (x_45_scale <= 1.8e-101) tmp = abs((sqrt(8.0) * (sqrt(2.0) * (b * (0.25 * y_45_scale))))); else tmp = 0.25 * (t_0 * hypot(t_2, (sqrt(2.0) * (b * sin(t_1))))); 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[(x$45$scale * N[Sqrt[8.0], $MachinePrecision]), $MachinePrecision]}, Block[{t$95$1 = N[(0.005555555555555556 * N[(Pi * angle), $MachinePrecision]), $MachinePrecision]}, Block[{t$95$2 = N[(N[Sqrt[2.0], $MachinePrecision] * N[(a * N[Cos[t$95$1], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]}, If[LessEqual[x$45$scale, -1.75e+61], N[(N[(a * N[(N[Sqrt[2.0], $MachinePrecision] * N[(N[Sqrt[8.0], $MachinePrecision] * N[Cos[N[(angle * N[(Pi * 0.005555555555555556), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * N[(x$45$scale * -0.25), $MachinePrecision]), $MachinePrecision], If[LessEqual[x$45$scale, -7.2e-25], N[(N[(x$45$scale * 0.25), $MachinePrecision] * N[(N[Sqrt[2.0], $MachinePrecision] * N[(a * N[(N[Sqrt[8.0], $MachinePrecision] * N[Cos[N[(Pi * N[(0.005555555555555556 * angle), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision], If[LessEqual[x$45$scale, -3.65e-112], N[(-0.25 * N[(t$95$0 * t$95$2), $MachinePrecision]), $MachinePrecision], If[LessEqual[x$45$scale, 1.8e-101], N[Abs[N[(N[Sqrt[8.0], $MachinePrecision] * N[(N[Sqrt[2.0], $MachinePrecision] * N[(b * N[(0.25 * y$45$scale), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision], N[(0.25 * N[(t$95$0 * N[Sqrt[t$95$2 ^ 2 + N[(N[Sqrt[2.0], $MachinePrecision] * N[(b * N[Sin[t$95$1], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] ^ 2], $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 := x-scale \cdot \sqrt{8}\\
t_1 := 0.005555555555555556 \cdot \left(\pi \cdot angle\right)\\
t_2 := \sqrt{2} \cdot \left(a \cdot \cos t_1\right)\\
\mathbf{if}\;x-scale \leq -1.75 \cdot 10^{+61}:\\
\;\;\;\;\left(a \cdot \left(\sqrt{2} \cdot \left(\sqrt{8} \cdot \cos \left(angle \cdot \left(\pi \cdot 0.005555555555555556\right)\right)\right)\right)\right) \cdot \left(x-scale \cdot -0.25\right)\\
\mathbf{elif}\;x-scale \leq -7.2 \cdot 10^{-25}:\\
\;\;\;\;\left(x-scale \cdot 0.25\right) \cdot \left(\sqrt{2} \cdot \left(a \cdot \left(\sqrt{8} \cdot \cos \left(\pi \cdot \left(0.005555555555555556 \cdot angle\right)\right)\right)\right)\right)\\
\mathbf{elif}\;x-scale \leq -3.65 \cdot 10^{-112}:\\
\;\;\;\;-0.25 \cdot \left(t_0 \cdot t_2\right)\\
\mathbf{elif}\;x-scale \leq 1.8 \cdot 10^{-101}:\\
\;\;\;\;\left|\sqrt{8} \cdot \left(\sqrt{2} \cdot \left(b \cdot \left(0.25 \cdot y-scale\right)\right)\right)\right|\\
\mathbf{else}:\\
\;\;\;\;0.25 \cdot \left(t_0 \cdot \mathsf{hypot}\left(t_2, \sqrt{2} \cdot \left(b \cdot \sin t_1\right)\right)\right)\\
\end{array}
Results
if x-scale < -1.75000000000000009e61Initial program 63.3
Simplified63.1
[Start]63.3 | \[ \frac{-\sqrt{\left(\left(2 \cdot \frac{4 \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}}\right) \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)\right) \cdot \left(\left(\frac{\frac{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{x-scale}}{x-scale} + \frac{\frac{{\left(a \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{y-scale}}{y-scale}\right) + \sqrt{{\left(\frac{\frac{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{x-scale}}{x-scale} - \frac{\frac{{\left(a \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{y-scale}}{y-scale}\right)}^{2} + {\left(\frac{\frac{\left(\left(2 \cdot \left({b}^{2} - {a}^{2}\right)\right) \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right) \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)}{x-scale}}{y-scale}\right)}^{2}}\right)}}{\frac{4 \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}}}
\] |
|---|
Taylor expanded in x-scale around inf 61.1
Simplified61.1
[Start]61.1 | \[ {\left(x-scale \cdot y-scale\right)}^{2} \cdot \left(-0.25 \cdot \left(-1 \cdot \left(\frac{\sqrt{8}}{x-scale \cdot y-scale} \cdot \sqrt{2 \cdot \frac{{a}^{2} \cdot {\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{y-scale}^{2}} + 2 \cdot \frac{{b}^{2} \cdot {\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{y-scale}^{2}}}\right)\right)\right)
\] |
|---|---|
mul-1-neg [=>]61.1 | \[ {\left(x-scale \cdot y-scale\right)}^{2} \cdot \left(-0.25 \cdot \color{blue}{\left(-\frac{\sqrt{8}}{x-scale \cdot y-scale} \cdot \sqrt{2 \cdot \frac{{a}^{2} \cdot {\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{y-scale}^{2}} + 2 \cdot \frac{{b}^{2} \cdot {\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{y-scale}^{2}}}\right)}\right)
\] |
*-commutative [=>]61.1 | \[ {\left(x-scale \cdot y-scale\right)}^{2} \cdot \left(-0.25 \cdot \left(-\color{blue}{\sqrt{2 \cdot \frac{{a}^{2} \cdot {\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{y-scale}^{2}} + 2 \cdot \frac{{b}^{2} \cdot {\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{y-scale}^{2}}} \cdot \frac{\sqrt{8}}{x-scale \cdot y-scale}}\right)\right)
\] |
*-commutative [=>]61.1 | \[ {\left(x-scale \cdot y-scale\right)}^{2} \cdot \left(-0.25 \cdot \left(-\sqrt{2 \cdot \frac{{a}^{2} \cdot {\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{y-scale}^{2}} + 2 \cdot \frac{{b}^{2} \cdot {\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{y-scale}^{2}}} \cdot \frac{\sqrt{8}}{\color{blue}{y-scale \cdot x-scale}}\right)\right)
\] |
Taylor expanded in a around -inf 51.2
Simplified51.2
[Start]51.2 | \[ -0.25 \cdot \left(x-scale \cdot \left(\sqrt{2} \cdot \left(a \cdot \left(\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right) \cdot \sqrt{8}\right)\right)\right)\right)
\] |
|---|---|
associate-*r* [=>]51.1 | \[ \color{blue}{\left(-0.25 \cdot x-scale\right) \cdot \left(\sqrt{2} \cdot \left(a \cdot \left(\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right) \cdot \sqrt{8}\right)\right)\right)}
\] |
*-commutative [=>]51.1 | \[ \color{blue}{\left(\sqrt{2} \cdot \left(a \cdot \left(\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right) \cdot \sqrt{8}\right)\right)\right) \cdot \left(-0.25 \cdot x-scale\right)}
\] |
associate-*r* [=>]51.1 | \[ \color{blue}{\left(\left(\sqrt{2} \cdot a\right) \cdot \left(\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right) \cdot \sqrt{8}\right)\right)} \cdot \left(-0.25 \cdot x-scale\right)
\] |
*-commutative [=>]51.1 | \[ \left(\color{blue}{\left(a \cdot \sqrt{2}\right)} \cdot \left(\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right) \cdot \sqrt{8}\right)\right) \cdot \left(-0.25 \cdot x-scale\right)
\] |
associate-*l* [=>]51.2 | \[ \color{blue}{\left(a \cdot \left(\sqrt{2} \cdot \left(\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right) \cdot \sqrt{8}\right)\right)\right)} \cdot \left(-0.25 \cdot x-scale\right)
\] |
*-commutative [=>]51.2 | \[ \left(a \cdot \left(\sqrt{2} \cdot \color{blue}{\left(\sqrt{8} \cdot \cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)\right)}\right)\right) \cdot \left(-0.25 \cdot x-scale\right)
\] |
associate-*r* [=>]51.2 | \[ \left(a \cdot \left(\sqrt{2} \cdot \left(\sqrt{8} \cdot \cos \color{blue}{\left(\left(0.005555555555555556 \cdot angle\right) \cdot \pi\right)}\right)\right)\right) \cdot \left(-0.25 \cdot x-scale\right)
\] |
*-commutative [=>]51.2 | \[ \left(a \cdot \left(\sqrt{2} \cdot \left(\sqrt{8} \cdot \cos \left(\color{blue}{\left(angle \cdot 0.005555555555555556\right)} \cdot \pi\right)\right)\right)\right) \cdot \left(-0.25 \cdot x-scale\right)
\] |
associate-*l* [=>]51.2 | \[ \left(a \cdot \left(\sqrt{2} \cdot \left(\sqrt{8} \cdot \cos \color{blue}{\left(angle \cdot \left(0.005555555555555556 \cdot \pi\right)\right)}\right)\right)\right) \cdot \left(-0.25 \cdot x-scale\right)
\] |
*-commutative [=>]51.2 | \[ \left(a \cdot \left(\sqrt{2} \cdot \left(\sqrt{8} \cdot \cos \left(angle \cdot \left(0.005555555555555556 \cdot \pi\right)\right)\right)\right)\right) \cdot \color{blue}{\left(x-scale \cdot -0.25\right)}
\] |
if -1.75000000000000009e61 < x-scale < -7.1999999999999998e-25Initial program 62.9
Simplified62.3
[Start]62.9 | \[ \frac{-\sqrt{\left(\left(2 \cdot \frac{4 \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}}\right) \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)\right) \cdot \left(\left(\frac{\frac{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{x-scale}}{x-scale} + \frac{\frac{{\left(a \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{y-scale}}{y-scale}\right) + \sqrt{{\left(\frac{\frac{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{x-scale}}{x-scale} - \frac{\frac{{\left(a \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{y-scale}}{y-scale}\right)}^{2} + {\left(\frac{\frac{\left(\left(2 \cdot \left({b}^{2} - {a}^{2}\right)\right) \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right) \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)}{x-scale}}{y-scale}\right)}^{2}}\right)}}{\frac{4 \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}}}
\] |
|---|
Taylor expanded in x-scale around inf 60.5
Simplified60.5
[Start]60.5 | \[ {\left(x-scale \cdot y-scale\right)}^{2} \cdot \left(-0.25 \cdot \left(-1 \cdot \left(\frac{\sqrt{8}}{x-scale \cdot y-scale} \cdot \sqrt{2 \cdot \frac{{a}^{2} \cdot {\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{y-scale}^{2}} + 2 \cdot \frac{{b}^{2} \cdot {\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{y-scale}^{2}}}\right)\right)\right)
\] |
|---|---|
mul-1-neg [=>]60.5 | \[ {\left(x-scale \cdot y-scale\right)}^{2} \cdot \left(-0.25 \cdot \color{blue}{\left(-\frac{\sqrt{8}}{x-scale \cdot y-scale} \cdot \sqrt{2 \cdot \frac{{a}^{2} \cdot {\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{y-scale}^{2}} + 2 \cdot \frac{{b}^{2} \cdot {\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{y-scale}^{2}}}\right)}\right)
\] |
*-commutative [=>]60.5 | \[ {\left(x-scale \cdot y-scale\right)}^{2} \cdot \left(-0.25 \cdot \left(-\color{blue}{\sqrt{2 \cdot \frac{{a}^{2} \cdot {\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{y-scale}^{2}} + 2 \cdot \frac{{b}^{2} \cdot {\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{y-scale}^{2}}} \cdot \frac{\sqrt{8}}{x-scale \cdot y-scale}}\right)\right)
\] |
*-commutative [=>]60.5 | \[ {\left(x-scale \cdot y-scale\right)}^{2} \cdot \left(-0.25 \cdot \left(-\sqrt{2 \cdot \frac{{a}^{2} \cdot {\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{y-scale}^{2}} + 2 \cdot \frac{{b}^{2} \cdot {\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{y-scale}^{2}}} \cdot \frac{\sqrt{8}}{\color{blue}{y-scale \cdot x-scale}}\right)\right)
\] |
Taylor expanded in b around 0 54.0
Simplified54.0
[Start]54.0 | \[ 0.25 \cdot \left(x-scale \cdot \left(\sqrt{2} \cdot \left(a \cdot \left(\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right) \cdot \sqrt{8}\right)\right)\right)\right)
\] |
|---|---|
associate-*r* [=>]54.0 | \[ \color{blue}{\left(0.25 \cdot x-scale\right) \cdot \left(\sqrt{2} \cdot \left(a \cdot \left(\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right) \cdot \sqrt{8}\right)\right)\right)}
\] |
associate-*r* [=>]54.0 | \[ \left(0.25 \cdot x-scale\right) \cdot \color{blue}{\left(\left(\sqrt{2} \cdot a\right) \cdot \left(\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right) \cdot \sqrt{8}\right)\right)}
\] |
*-commutative [=>]54.0 | \[ \left(0.25 \cdot x-scale\right) \cdot \left(\left(\sqrt{2} \cdot a\right) \cdot \color{blue}{\left(\sqrt{8} \cdot \cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)\right)}\right)
\] |
associate-*r* [=>]54.0 | \[ \left(0.25 \cdot x-scale\right) \cdot \left(\left(\sqrt{2} \cdot a\right) \cdot \left(\sqrt{8} \cdot \cos \color{blue}{\left(\left(0.005555555555555556 \cdot angle\right) \cdot \pi\right)}\right)\right)
\] |
*-commutative [=>]54.0 | \[ \left(0.25 \cdot x-scale\right) \cdot \left(\left(\sqrt{2} \cdot a\right) \cdot \left(\sqrt{8} \cdot \cos \color{blue}{\left(\pi \cdot \left(0.005555555555555556 \cdot angle\right)\right)}\right)\right)
\] |
Taylor expanded in a around 0 54.0
Simplified54.0
[Start]54.0 | \[ \left(0.25 \cdot x-scale\right) \cdot \left(\sqrt{2} \cdot \left(a \cdot \left(\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right) \cdot \sqrt{8}\right)\right)\right)
\] |
|---|---|
*-commutative [=>]54.0 | \[ \left(0.25 \cdot x-scale\right) \cdot \left(\sqrt{2} \cdot \left(a \cdot \color{blue}{\left(\sqrt{8} \cdot \cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)\right)}\right)\right)
\] |
associate-*r* [=>]54.0 | \[ \left(0.25 \cdot x-scale\right) \cdot \left(\sqrt{2} \cdot \left(a \cdot \left(\sqrt{8} \cdot \cos \color{blue}{\left(\left(0.005555555555555556 \cdot angle\right) \cdot \pi\right)}\right)\right)\right)
\] |
*-commutative [<=]54.0 | \[ \left(0.25 \cdot x-scale\right) \cdot \left(\sqrt{2} \cdot \left(a \cdot \left(\sqrt{8} \cdot \cos \color{blue}{\left(\pi \cdot \left(0.005555555555555556 \cdot angle\right)\right)}\right)\right)\right)
\] |
*-commutative [=>]54.0 | \[ \left(0.25 \cdot x-scale\right) \cdot \left(\sqrt{2} \cdot \left(a \cdot \left(\sqrt{8} \cdot \cos \left(\pi \cdot \color{blue}{\left(angle \cdot 0.005555555555555556\right)}\right)\right)\right)\right)
\] |
if -7.1999999999999998e-25 < x-scale < -3.6499999999999999e-112Initial program 63.3
Simplified62.7
[Start]63.3 | \[ \frac{-\sqrt{\left(\left(2 \cdot \frac{4 \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}}\right) \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)\right) \cdot \left(\left(\frac{\frac{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{x-scale}}{x-scale} + \frac{\frac{{\left(a \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{y-scale}}{y-scale}\right) + \sqrt{{\left(\frac{\frac{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{x-scale}}{x-scale} - \frac{\frac{{\left(a \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{y-scale}}{y-scale}\right)}^{2} + {\left(\frac{\frac{\left(\left(2 \cdot \left({b}^{2} - {a}^{2}\right)\right) \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right) \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)}{x-scale}}{y-scale}\right)}^{2}}\right)}}{\frac{4 \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}}}
\] |
|---|
Taylor expanded in y-scale around 0 62.7
Taylor expanded in a around -inf 53.8
if -3.6499999999999999e-112 < x-scale < 1.8e-101Initial program 64.0
Simplified63.7
[Start]64.0 | \[ \frac{-\sqrt{\left(\left(2 \cdot \frac{4 \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}}\right) \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)\right) \cdot \left(\left(\frac{\frac{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{x-scale}}{x-scale} + \frac{\frac{{\left(a \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{y-scale}}{y-scale}\right) + \sqrt{{\left(\frac{\frac{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{x-scale}}{x-scale} - \frac{\frac{{\left(a \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{y-scale}}{y-scale}\right)}^{2} + {\left(\frac{\frac{\left(\left(2 \cdot \left({b}^{2} - {a}^{2}\right)\right) \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right) \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)}{x-scale}}{y-scale}\right)}^{2}}\right)}}{\frac{4 \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}}}
\] |
|---|
Taylor expanded in angle around 0 49.1
Simplified49.1
[Start]49.1 | \[ 0.25 \cdot \left(y-scale \cdot \left(\sqrt{2} \cdot \left(b \cdot \sqrt{8}\right)\right)\right)
\] |
|---|---|
associate-*r* [=>]49.1 | \[ \color{blue}{\left(0.25 \cdot y-scale\right) \cdot \left(\sqrt{2} \cdot \left(b \cdot \sqrt{8}\right)\right)}
\] |
*-commutative [=>]49.1 | \[ \left(0.25 \cdot y-scale\right) \cdot \color{blue}{\left(\left(b \cdot \sqrt{8}\right) \cdot \sqrt{2}\right)}
\] |
*-commutative [=>]49.1 | \[ \left(0.25 \cdot y-scale\right) \cdot \left(\color{blue}{\left(\sqrt{8} \cdot b\right)} \cdot \sqrt{2}\right)
\] |
Applied egg-rr38.0
Taylor expanded in y-scale around 0 38.0
Simplified38.0
[Start]38.0 | \[ \left|0.25 \cdot \left(y-scale \cdot \left(\sqrt{2} \cdot \left(b \cdot \sqrt{8}\right)\right)\right)\right|
\] |
|---|---|
associate-*r* [=>]38.0 | \[ \left|\color{blue}{\left(0.25 \cdot y-scale\right) \cdot \left(\sqrt{2} \cdot \left(b \cdot \sqrt{8}\right)\right)}\right|
\] |
*-commutative [<=]38.0 | \[ \left|\left(0.25 \cdot y-scale\right) \cdot \left(\sqrt{2} \cdot \color{blue}{\left(\sqrt{8} \cdot b\right)}\right)\right|
\] |
*-commutative [<=]38.0 | \[ \left|\left(0.25 \cdot y-scale\right) \cdot \color{blue}{\left(\left(\sqrt{8} \cdot b\right) \cdot \sqrt{2}\right)}\right|
\] |
associate-*r* [=>]38.0 | \[ \left|\color{blue}{\left(\left(0.25 \cdot y-scale\right) \cdot \left(\sqrt{8} \cdot b\right)\right) \cdot \sqrt{2}}\right|
\] |
*-commutative [=>]38.0 | \[ \left|\left(\left(0.25 \cdot y-scale\right) \cdot \color{blue}{\left(b \cdot \sqrt{8}\right)}\right) \cdot \sqrt{2}\right|
\] |
associate-*l* [<=]38.0 | \[ \left|\color{blue}{\left(\left(\left(0.25 \cdot y-scale\right) \cdot b\right) \cdot \sqrt{8}\right)} \cdot \sqrt{2}\right|
\] |
*-commutative [=>]38.0 | \[ \left|\color{blue}{\left(\sqrt{8} \cdot \left(\left(0.25 \cdot y-scale\right) \cdot b\right)\right)} \cdot \sqrt{2}\right|
\] |
associate-*l* [=>]38.0 | \[ \left|\color{blue}{\sqrt{8} \cdot \left(\left(\left(0.25 \cdot y-scale\right) \cdot b\right) \cdot \sqrt{2}\right)}\right|
\] |
*-commutative [=>]38.0 | \[ \left|\sqrt{8} \cdot \left(\color{blue}{\left(b \cdot \left(0.25 \cdot y-scale\right)\right)} \cdot \sqrt{2}\right)\right|
\] |
if 1.8e-101 < x-scale Initial program 63.2
Simplified62.9
[Start]63.2 | \[ \frac{-\sqrt{\left(\left(2 \cdot \frac{4 \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}}\right) \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)\right) \cdot \left(\left(\frac{\frac{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{x-scale}}{x-scale} + \frac{\frac{{\left(a \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{y-scale}}{y-scale}\right) + \sqrt{{\left(\frac{\frac{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{x-scale}}{x-scale} - \frac{\frac{{\left(a \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{y-scale}}{y-scale}\right)}^{2} + {\left(\frac{\frac{\left(\left(2 \cdot \left({b}^{2} - {a}^{2}\right)\right) \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right) \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)}{x-scale}}{y-scale}\right)}^{2}}\right)}}{\frac{4 \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}}}
\] |
|---|
Taylor expanded in y-scale around 0 46.6
Applied egg-rr35.8
Final simplification41.8
| Alternative 1 | |
|---|---|
| Error | 39.8 |
| Cost | 65732 |
| Alternative 2 | |
|---|---|
| Error | 45.8 |
| Cost | 39756 |
| Alternative 3 | |
|---|---|
| Error | 45.8 |
| Cost | 27024 |
| Alternative 4 | |
|---|---|
| Error | 45.8 |
| Cost | 27024 |
| Alternative 5 | |
|---|---|
| Error | 44.8 |
| Cost | 20304 |
| Alternative 6 | |
|---|---|
| Error | 44.8 |
| Cost | 20304 |
| Alternative 7 | |
|---|---|
| Error | 44.9 |
| Cost | 20304 |
| Alternative 8 | |
|---|---|
| Error | 53.3 |
| Cost | 13764 |
| Alternative 9 | |
|---|---|
| Error | 52.8 |
| Cost | 13508 |
| Alternative 10 | |
|---|---|
| Error | 52.8 |
| Cost | 13508 |
| Alternative 11 | |
|---|---|
| Error | 52.8 |
| Cost | 13508 |
| Alternative 12 | |
|---|---|
| Error | 53.6 |
| Cost | 653 |
| Alternative 13 | |
|---|---|
| Error | 53.9 |
| Cost | 192 |
herbie shell --seed 2023011
(FPCore (a b angle x-scale y-scale)
:name "a 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))))