| Alternative 1 | |
|---|---|
| Error | 26.1 |
| Cost | 1485 |
(FPCore (a b angle x-scale y-scale)
:precision binary64
(-
(*
(/
(/
(*
(* (* 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 (- (pow b 2.0) (pow a 2.0))) (sin (* (/ angle 180.0) PI)))
(cos (* (/ angle 180.0) PI)))
x-scale)
y-scale))
(*
(*
4.0
(/
(/
(+
(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))))(FPCore (a b angle x-scale y-scale)
:precision binary64
(if (<= x-scale -8.2e-160)
(* -4.0 (/ (* (/ a y-scale) (/ b x-scale)) (/ (/ x-scale b) (/ a y-scale))))
(if (<= x-scale -1.1e-292)
(* (/ (pow (* a b) 2.0) (* x-scale y-scale)) (/ -4.0 (* x-scale y-scale)))
(*
-4.0
(* (/ (/ a y-scale) (/ x-scale b)) (/ (/ b x-scale) (/ y-scale a)))))))double code(double a, double b, double angle, double x_45_scale, double y_45_scale) {
return ((((((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 * (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)) - ((4.0 * (((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));
}
double code(double a, double b, double angle, double x_45_scale, double y_45_scale) {
double tmp;
if (x_45_scale <= -8.2e-160) {
tmp = -4.0 * (((a / y_45_scale) * (b / x_45_scale)) / ((x_45_scale / b) / (a / y_45_scale)));
} else if (x_45_scale <= -1.1e-292) {
tmp = (pow((a * b), 2.0) / (x_45_scale * y_45_scale)) * (-4.0 / (x_45_scale * y_45_scale));
} else {
tmp = -4.0 * (((a / y_45_scale) / (x_45_scale / b)) * ((b / x_45_scale) / (y_45_scale / a)));
}
return tmp;
}
public static double code(double a, double b, double angle, double x_45_scale, double y_45_scale) {
return ((((((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 * (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)) - ((4.0 * (((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));
}
public static double code(double a, double b, double angle, double x_45_scale, double y_45_scale) {
double tmp;
if (x_45_scale <= -8.2e-160) {
tmp = -4.0 * (((a / y_45_scale) * (b / x_45_scale)) / ((x_45_scale / b) / (a / y_45_scale)));
} else if (x_45_scale <= -1.1e-292) {
tmp = (Math.pow((a * b), 2.0) / (x_45_scale * y_45_scale)) * (-4.0 / (x_45_scale * y_45_scale));
} else {
tmp = -4.0 * (((a / y_45_scale) / (x_45_scale / b)) * ((b / x_45_scale) / (y_45_scale / a)));
}
return tmp;
}
def code(a, b, angle, x_45_scale, y_45_scale): return ((((((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 * (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)) - ((4.0 * (((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))
def code(a, b, angle, x_45_scale, y_45_scale): tmp = 0 if x_45_scale <= -8.2e-160: tmp = -4.0 * (((a / y_45_scale) * (b / x_45_scale)) / ((x_45_scale / b) / (a / y_45_scale))) elif x_45_scale <= -1.1e-292: tmp = (math.pow((a * b), 2.0) / (x_45_scale * y_45_scale)) * (-4.0 / (x_45_scale * y_45_scale)) else: tmp = -4.0 * (((a / y_45_scale) / (x_45_scale / b)) * ((b / x_45_scale) / (y_45_scale / a))) return tmp
function code(a, b, angle, x_45_scale, y_45_scale) return Float64(Float64(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) * 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)) - Float64(Float64(4.0 * 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))) end
function code(a, b, angle, x_45_scale, y_45_scale) tmp = 0.0 if (x_45_scale <= -8.2e-160) tmp = Float64(-4.0 * Float64(Float64(Float64(a / y_45_scale) * Float64(b / x_45_scale)) / Float64(Float64(x_45_scale / b) / Float64(a / y_45_scale)))); elseif (x_45_scale <= -1.1e-292) tmp = Float64(Float64((Float64(a * b) ^ 2.0) / Float64(x_45_scale * y_45_scale)) * Float64(-4.0 / Float64(x_45_scale * y_45_scale))); else tmp = Float64(-4.0 * Float64(Float64(Float64(a / y_45_scale) / Float64(x_45_scale / b)) * Float64(Float64(b / x_45_scale) / Float64(y_45_scale / a)))); end return tmp end
function tmp = code(a, b, angle, x_45_scale, y_45_scale) tmp = ((((((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 * ((b ^ 2.0) - (a ^ 2.0))) * sin(((angle / 180.0) * pi))) * cos(((angle / 180.0) * pi))) / x_45_scale) / y_45_scale)) - ((4.0 * (((((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)); end
function tmp_2 = code(a, b, angle, x_45_scale, y_45_scale) tmp = 0.0; if (x_45_scale <= -8.2e-160) tmp = -4.0 * (((a / y_45_scale) * (b / x_45_scale)) / ((x_45_scale / b) / (a / y_45_scale))); elseif (x_45_scale <= -1.1e-292) tmp = (((a * b) ^ 2.0) / (x_45_scale * y_45_scale)) * (-4.0 / (x_45_scale * y_45_scale)); else tmp = -4.0 * (((a / y_45_scale) / (x_45_scale / b)) * ((b / x_45_scale) / (y_45_scale / a))); end tmp_2 = tmp; end
code[a_, b_, angle_, x$45$scale_, y$45$scale_] := N[(N[(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] * 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]), $MachinePrecision] - N[(N[(4.0 * 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]), $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]), $MachinePrecision]
code[a_, b_, angle_, x$45$scale_, y$45$scale_] := If[LessEqual[x$45$scale, -8.2e-160], N[(-4.0 * N[(N[(N[(a / y$45$scale), $MachinePrecision] * N[(b / x$45$scale), $MachinePrecision]), $MachinePrecision] / N[(N[(x$45$scale / b), $MachinePrecision] / N[(a / y$45$scale), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision], If[LessEqual[x$45$scale, -1.1e-292], N[(N[(N[Power[N[(a * b), $MachinePrecision], 2.0], $MachinePrecision] / N[(x$45$scale * y$45$scale), $MachinePrecision]), $MachinePrecision] * N[(-4.0 / N[(x$45$scale * y$45$scale), $MachinePrecision]), $MachinePrecision]), $MachinePrecision], N[(-4.0 * N[(N[(N[(a / y$45$scale), $MachinePrecision] / N[(x$45$scale / b), $MachinePrecision]), $MachinePrecision] * N[(N[(b / x$45$scale), $MachinePrecision] / N[(y$45$scale / a), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]]]
\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} \cdot \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} - \left(4 \cdot \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}\right) \cdot \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}
\begin{array}{l}
\mathbf{if}\;x-scale \leq -8.2 \cdot 10^{-160}:\\
\;\;\;\;-4 \cdot \frac{\frac{a}{y-scale} \cdot \frac{b}{x-scale}}{\frac{\frac{x-scale}{b}}{\frac{a}{y-scale}}}\\
\mathbf{elif}\;x-scale \leq -1.1 \cdot 10^{-292}:\\
\;\;\;\;\frac{{\left(a \cdot b\right)}^{2}}{x-scale \cdot y-scale} \cdot \frac{-4}{x-scale \cdot y-scale}\\
\mathbf{else}:\\
\;\;\;\;-4 \cdot \left(\frac{\frac{a}{y-scale}}{\frac{x-scale}{b}} \cdot \frac{\frac{b}{x-scale}}{\frac{y-scale}{a}}\right)\\
\end{array}
Results
if x-scale < -8.20000000000000003e-160Initial program 38.8
Taylor expanded in angle around 0 34.7
Simplified17.7
[Start]34.7 | \[ -4 \cdot \frac{{a}^{2} \cdot {b}^{2}}{{y-scale}^{2} \cdot {x-scale}^{2}}
\] |
|---|---|
*-commutative [=>]34.7 | \[ \color{blue}{\frac{{a}^{2} \cdot {b}^{2}}{{y-scale}^{2} \cdot {x-scale}^{2}} \cdot -4}
\] |
times-frac [=>]34.9 | \[ \color{blue}{\left(\frac{{a}^{2}}{{y-scale}^{2}} \cdot \frac{{b}^{2}}{{x-scale}^{2}}\right)} \cdot -4
\] |
associate-*l* [=>]34.9 | \[ \color{blue}{\frac{{a}^{2}}{{y-scale}^{2}} \cdot \left(\frac{{b}^{2}}{{x-scale}^{2}} \cdot -4\right)}
\] |
unpow2 [=>]34.9 | \[ \frac{\color{blue}{a \cdot a}}{{y-scale}^{2}} \cdot \left(\frac{{b}^{2}}{{x-scale}^{2}} \cdot -4\right)
\] |
unpow2 [=>]34.9 | \[ \frac{a \cdot a}{\color{blue}{y-scale \cdot y-scale}} \cdot \left(\frac{{b}^{2}}{{x-scale}^{2}} \cdot -4\right)
\] |
times-frac [=>]25.9 | \[ \color{blue}{\left(\frac{a}{y-scale} \cdot \frac{a}{y-scale}\right)} \cdot \left(\frac{{b}^{2}}{{x-scale}^{2}} \cdot -4\right)
\] |
unpow2 [=>]25.9 | \[ \left(\frac{a}{y-scale} \cdot \frac{a}{y-scale}\right) \cdot \left(\frac{\color{blue}{b \cdot b}}{{x-scale}^{2}} \cdot -4\right)
\] |
unpow2 [=>]25.9 | \[ \left(\frac{a}{y-scale} \cdot \frac{a}{y-scale}\right) \cdot \left(\frac{b \cdot b}{\color{blue}{x-scale \cdot x-scale}} \cdot -4\right)
\] |
times-frac [=>]17.7 | \[ \left(\frac{a}{y-scale} \cdot \frac{a}{y-scale}\right) \cdot \left(\color{blue}{\left(\frac{b}{x-scale} \cdot \frac{b}{x-scale}\right)} \cdot -4\right)
\] |
Taylor expanded in a around 0 34.7
Simplified4.9
[Start]34.7 | \[ -4 \cdot \frac{{a}^{2} \cdot {b}^{2}}{{x-scale}^{2} \cdot {y-scale}^{2}}
\] |
|---|---|
*-commutative [=>]34.7 | \[ -4 \cdot \frac{{a}^{2} \cdot {b}^{2}}{\color{blue}{{y-scale}^{2} \cdot {x-scale}^{2}}}
\] |
times-frac [=>]34.9 | \[ -4 \cdot \color{blue}{\left(\frac{{a}^{2}}{{y-scale}^{2}} \cdot \frac{{b}^{2}}{{x-scale}^{2}}\right)}
\] |
unpow2 [=>]34.9 | \[ -4 \cdot \left(\frac{\color{blue}{a \cdot a}}{{y-scale}^{2}} \cdot \frac{{b}^{2}}{{x-scale}^{2}}\right)
\] |
unpow2 [=>]34.9 | \[ -4 \cdot \left(\frac{a \cdot a}{\color{blue}{y-scale \cdot y-scale}} \cdot \frac{{b}^{2}}{{x-scale}^{2}}\right)
\] |
times-frac [=>]25.9 | \[ -4 \cdot \left(\color{blue}{\left(\frac{a}{y-scale} \cdot \frac{a}{y-scale}\right)} \cdot \frac{{b}^{2}}{{x-scale}^{2}}\right)
\] |
unpow2 [=>]25.9 | \[ -4 \cdot \left(\left(\frac{a}{y-scale} \cdot \frac{a}{y-scale}\right) \cdot \frac{\color{blue}{b \cdot b}}{{x-scale}^{2}}\right)
\] |
unpow2 [=>]25.9 | \[ -4 \cdot \left(\left(\frac{a}{y-scale} \cdot \frac{a}{y-scale}\right) \cdot \frac{b \cdot b}{\color{blue}{x-scale \cdot x-scale}}\right)
\] |
times-frac [=>]17.7 | \[ -4 \cdot \left(\left(\frac{a}{y-scale} \cdot \frac{a}{y-scale}\right) \cdot \color{blue}{\left(\frac{b}{x-scale} \cdot \frac{b}{x-scale}\right)}\right)
\] |
swap-sqr [<=]4.9 | \[ -4 \cdot \color{blue}{\left(\left(\frac{a}{y-scale} \cdot \frac{b}{x-scale}\right) \cdot \left(\frac{a}{y-scale} \cdot \frac{b}{x-scale}\right)\right)}
\] |
unpow2 [<=]4.9 | \[ -4 \cdot \color{blue}{{\left(\frac{a}{y-scale} \cdot \frac{b}{x-scale}\right)}^{2}}
\] |
associate-*r/ [=>]4.9 | \[ -4 \cdot {\color{blue}{\left(\frac{\frac{a}{y-scale} \cdot b}{x-scale}\right)}}^{2}
\] |
associate-/l* [=>]4.9 | \[ -4 \cdot {\color{blue}{\left(\frac{\frac{a}{y-scale}}{\frac{x-scale}{b}}\right)}}^{2}
\] |
Applied egg-rr5.0
if -8.20000000000000003e-160 < x-scale < -1.10000000000000006e-292Initial program 52.2
Taylor expanded in angle around 0 63.3
Simplified63.3
[Start]63.3 | \[ -4 \cdot \frac{{a}^{2} \cdot {b}^{2}}{{y-scale}^{2} \cdot {x-scale}^{2}}
\] |
|---|---|
associate-*r/ [=>]63.3 | \[ \color{blue}{\frac{-4 \cdot \left({a}^{2} \cdot {b}^{2}\right)}{{y-scale}^{2} \cdot {x-scale}^{2}}}
\] |
unpow2 [=>]63.3 | \[ \frac{-4 \cdot \left(\color{blue}{\left(a \cdot a\right)} \cdot {b}^{2}\right)}{{y-scale}^{2} \cdot {x-scale}^{2}}
\] |
unpow2 [=>]63.3 | \[ \frac{-4 \cdot \left(\left(a \cdot a\right) \cdot \color{blue}{\left(b \cdot b\right)}\right)}{{y-scale}^{2} \cdot {x-scale}^{2}}
\] |
unpow2 [=>]63.3 | \[ \frac{-4 \cdot \left(\left(a \cdot a\right) \cdot \left(b \cdot b\right)\right)}{\color{blue}{\left(y-scale \cdot y-scale\right)} \cdot {x-scale}^{2}}
\] |
unpow2 [=>]63.3 | \[ \frac{-4 \cdot \left(\left(a \cdot a\right) \cdot \left(b \cdot b\right)\right)}{\left(y-scale \cdot y-scale\right) \cdot \color{blue}{\left(x-scale \cdot x-scale\right)}}
\] |
Applied egg-rr22.4
if -1.10000000000000006e-292 < x-scale Initial program 41.4
Taylor expanded in angle around 0 39.8
Simplified19.7
[Start]39.8 | \[ -4 \cdot \frac{{a}^{2} \cdot {b}^{2}}{{y-scale}^{2} \cdot {x-scale}^{2}}
\] |
|---|---|
*-commutative [=>]39.8 | \[ \color{blue}{\frac{{a}^{2} \cdot {b}^{2}}{{y-scale}^{2} \cdot {x-scale}^{2}} \cdot -4}
\] |
times-frac [=>]40.0 | \[ \color{blue}{\left(\frac{{a}^{2}}{{y-scale}^{2}} \cdot \frac{{b}^{2}}{{x-scale}^{2}}\right)} \cdot -4
\] |
associate-*l* [=>]40.0 | \[ \color{blue}{\frac{{a}^{2}}{{y-scale}^{2}} \cdot \left(\frac{{b}^{2}}{{x-scale}^{2}} \cdot -4\right)}
\] |
unpow2 [=>]40.0 | \[ \frac{\color{blue}{a \cdot a}}{{y-scale}^{2}} \cdot \left(\frac{{b}^{2}}{{x-scale}^{2}} \cdot -4\right)
\] |
unpow2 [=>]40.0 | \[ \frac{a \cdot a}{\color{blue}{y-scale \cdot y-scale}} \cdot \left(\frac{{b}^{2}}{{x-scale}^{2}} \cdot -4\right)
\] |
times-frac [=>]32.1 | \[ \color{blue}{\left(\frac{a}{y-scale} \cdot \frac{a}{y-scale}\right)} \cdot \left(\frac{{b}^{2}}{{x-scale}^{2}} \cdot -4\right)
\] |
unpow2 [=>]32.1 | \[ \left(\frac{a}{y-scale} \cdot \frac{a}{y-scale}\right) \cdot \left(\frac{\color{blue}{b \cdot b}}{{x-scale}^{2}} \cdot -4\right)
\] |
unpow2 [=>]32.1 | \[ \left(\frac{a}{y-scale} \cdot \frac{a}{y-scale}\right) \cdot \left(\frac{b \cdot b}{\color{blue}{x-scale \cdot x-scale}} \cdot -4\right)
\] |
times-frac [=>]19.7 | \[ \left(\frac{a}{y-scale} \cdot \frac{a}{y-scale}\right) \cdot \left(\color{blue}{\left(\frac{b}{x-scale} \cdot \frac{b}{x-scale}\right)} \cdot -4\right)
\] |
Taylor expanded in a around 0 39.8
Simplified5.8
[Start]39.8 | \[ -4 \cdot \frac{{a}^{2} \cdot {b}^{2}}{{x-scale}^{2} \cdot {y-scale}^{2}}
\] |
|---|---|
*-commutative [=>]39.8 | \[ -4 \cdot \frac{{a}^{2} \cdot {b}^{2}}{\color{blue}{{y-scale}^{2} \cdot {x-scale}^{2}}}
\] |
times-frac [=>]40.0 | \[ -4 \cdot \color{blue}{\left(\frac{{a}^{2}}{{y-scale}^{2}} \cdot \frac{{b}^{2}}{{x-scale}^{2}}\right)}
\] |
unpow2 [=>]40.0 | \[ -4 \cdot \left(\frac{\color{blue}{a \cdot a}}{{y-scale}^{2}} \cdot \frac{{b}^{2}}{{x-scale}^{2}}\right)
\] |
unpow2 [=>]40.0 | \[ -4 \cdot \left(\frac{a \cdot a}{\color{blue}{y-scale \cdot y-scale}} \cdot \frac{{b}^{2}}{{x-scale}^{2}}\right)
\] |
times-frac [=>]32.1 | \[ -4 \cdot \left(\color{blue}{\left(\frac{a}{y-scale} \cdot \frac{a}{y-scale}\right)} \cdot \frac{{b}^{2}}{{x-scale}^{2}}\right)
\] |
unpow2 [=>]32.1 | \[ -4 \cdot \left(\left(\frac{a}{y-scale} \cdot \frac{a}{y-scale}\right) \cdot \frac{\color{blue}{b \cdot b}}{{x-scale}^{2}}\right)
\] |
unpow2 [=>]32.1 | \[ -4 \cdot \left(\left(\frac{a}{y-scale} \cdot \frac{a}{y-scale}\right) \cdot \frac{b \cdot b}{\color{blue}{x-scale \cdot x-scale}}\right)
\] |
times-frac [=>]19.7 | \[ -4 \cdot \left(\left(\frac{a}{y-scale} \cdot \frac{a}{y-scale}\right) \cdot \color{blue}{\left(\frac{b}{x-scale} \cdot \frac{b}{x-scale}\right)}\right)
\] |
swap-sqr [<=]5.8 | \[ -4 \cdot \color{blue}{\left(\left(\frac{a}{y-scale} \cdot \frac{b}{x-scale}\right) \cdot \left(\frac{a}{y-scale} \cdot \frac{b}{x-scale}\right)\right)}
\] |
unpow2 [<=]5.8 | \[ -4 \cdot \color{blue}{{\left(\frac{a}{y-scale} \cdot \frac{b}{x-scale}\right)}^{2}}
\] |
associate-*r/ [=>]6.2 | \[ -4 \cdot {\color{blue}{\left(\frac{\frac{a}{y-scale} \cdot b}{x-scale}\right)}}^{2}
\] |
associate-/l* [=>]5.8 | \[ -4 \cdot {\color{blue}{\left(\frac{\frac{a}{y-scale}}{\frac{x-scale}{b}}\right)}}^{2}
\] |
Applied egg-rr8.2
Applied egg-rr6.0
Final simplification6.6
| Alternative 1 | |
|---|---|
| Error | 26.1 |
| Cost | 1485 |
| Alternative 2 | |
|---|---|
| Error | 20.2 |
| Cost | 1353 |
| Alternative 3 | |
|---|---|
| Error | 5.9 |
| Cost | 1352 |
| Alternative 4 | |
|---|---|
| Error | 8.2 |
| Cost | 1088 |
| Alternative 5 | |
|---|---|
| Error | 8.2 |
| Cost | 1088 |
| Alternative 6 | |
|---|---|
| Error | 5.9 |
| Cost | 1088 |
| Alternative 7 | |
|---|---|
| Error | 30.3 |
| Cost | 64 |
herbie shell --seed 2023066
(FPCore (a b angle x-scale y-scale)
:name "Simplification of discriminant from scale-rotated-ellipse"
:precision binary64
(- (* (/ (/ (* (* (* 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 (- (pow b 2.0) (pow a 2.0))) (sin (* (/ angle 180.0) PI))) (cos (* (/ angle 180.0) PI))) x-scale) y-scale)) (* (* 4.0 (/ (/ (+ (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))))