Integrand size = 25, antiderivative size = 99 \[ \int \frac {1}{\sqrt {e \csc (c+d x)} (a+a \sec (c+d x))} \, dx=\frac {2 \cot (c+d x)}{a d \sqrt {e \csc (c+d x)}}-\frac {2 \csc (c+d x)}{a d \sqrt {e \csc (c+d x)}}+\frac {4 E\left (\left .\frac {1}{2} \left (c-\frac {\pi }{2}+d x\right )\right |2\right )}{a d \sqrt {e \csc (c+d x)} \sqrt {\sin (c+d x)}} \]
2*cot(d*x+c)/a/d/(e*csc(d*x+c))^(1/2)-2*csc(d*x+c)/a/d/(e*csc(d*x+c))^(1/2 )-4*(sin(1/2*c+1/4*Pi+1/2*d*x)^2)^(1/2)/sin(1/2*c+1/4*Pi+1/2*d*x)*Elliptic E(cos(1/2*c+1/4*Pi+1/2*d*x),2^(1/2))/a/d/(e*csc(d*x+c))^(1/2)/sin(d*x+c)^( 1/2)
Result contains higher order function than in optimal. Order 5 vs. order 4 in optimal.
Time = 1.15 (sec) , antiderivative size = 95, normalized size of antiderivative = 0.96 \[ \int \frac {1}{\sqrt {e \csc (c+d x)} (a+a \sec (c+d x))} \, dx=\frac {6 (2 i+\cot (c+d x)-\csc (c+d x))-4 \sqrt {1-e^{2 i (c+d x)}} (i+\cot (c+d x)) \operatorname {Hypergeometric2F1}\left (\frac {1}{2},\frac {3}{4},\frac {7}{4},e^{2 i (c+d x)}\right )}{3 a d \sqrt {e \csc (c+d x)}} \]
(6*(2*I + Cot[c + d*x] - Csc[c + d*x]) - 4*Sqrt[1 - E^((2*I)*(c + d*x))]*( I + Cot[c + d*x])*Hypergeometric2F1[1/2, 3/4, 7/4, E^((2*I)*(c + d*x))])/( 3*a*d*Sqrt[e*Csc[c + d*x]])
Time = 0.68 (sec) , antiderivative size = 90, normalized size of antiderivative = 0.91, number of steps used = 15, number of rules used = 14, \(\frac {\text {number of rules}}{\text {integrand size}}\) = 0.560, Rules used = {3042, 4366, 3042, 4360, 25, 25, 3042, 3318, 3042, 3044, 15, 3047, 3042, 3119}
Below are the steps used by Rubi to obtain the solution. The rule number used for the transformation is given above next to the arrow. The rules definitions used are listed below.
\(\displaystyle \int \frac {1}{(a \sec (c+d x)+a) \sqrt {e \csc (c+d x)}} \, dx\) |
\(\Big \downarrow \) 3042 |
\(\displaystyle \int \frac {1}{\left (a-a \csc \left (c+d x-\frac {\pi }{2}\right )\right ) \sqrt {e \sec \left (c+d x-\frac {\pi }{2}\right )}}dx\) |
\(\Big \downarrow \) 4366 |
\(\displaystyle \frac {\int \frac {\sqrt {\sin (c+d x)}}{\sec (c+d x) a+a}dx}{\sqrt {\sin (c+d x)} \sqrt {e \csc (c+d x)}}\) |
\(\Big \downarrow \) 3042 |
\(\displaystyle \frac {\int \frac {\sqrt {\cos \left (c+d x-\frac {\pi }{2}\right )}}{a-a \csc \left (c+d x-\frac {\pi }{2}\right )}dx}{\sqrt {\sin (c+d x)} \sqrt {e \csc (c+d x)}}\) |
\(\Big \downarrow \) 4360 |
\(\displaystyle \frac {\int -\frac {\cos (c+d x) \sqrt {\sin (c+d x)}}{-\cos (c+d x) a-a}dx}{\sqrt {\sin (c+d x)} \sqrt {e \csc (c+d x)}}\) |
\(\Big \downarrow \) 25 |
\(\displaystyle -\frac {\int -\frac {\cos (c+d x) \sqrt {\sin (c+d x)}}{\cos (c+d x) a+a}dx}{\sqrt {\sin (c+d x)} \sqrt {e \csc (c+d x)}}\) |
\(\Big \downarrow \) 25 |
\(\displaystyle \frac {\int \frac {\cos (c+d x) \sqrt {\sin (c+d x)}}{\cos (c+d x) a+a}dx}{\sqrt {\sin (c+d x)} \sqrt {e \csc (c+d x)}}\) |
\(\Big \downarrow \) 3042 |
\(\displaystyle \frac {\int \frac {\sqrt {-\cos \left (c+d x+\frac {\pi }{2}\right )} \sin \left (c+d x+\frac {\pi }{2}\right )}{\sin \left (c+d x+\frac {\pi }{2}\right ) a+a}dx}{\sqrt {\sin (c+d x)} \sqrt {e \csc (c+d x)}}\) |
\(\Big \downarrow \) 3318 |
\(\displaystyle \frac {\frac {\int \frac {\cos (c+d x)}{\sin ^{\frac {3}{2}}(c+d x)}dx}{a}-\frac {\int \frac {\cos ^2(c+d x)}{\sin ^{\frac {3}{2}}(c+d x)}dx}{a}}{\sqrt {\sin (c+d x)} \sqrt {e \csc (c+d x)}}\) |
\(\Big \downarrow \) 3042 |
\(\displaystyle \frac {\frac {\int \frac {\cos (c+d x)}{\sin (c+d x)^{3/2}}dx}{a}-\frac {\int \frac {\cos (c+d x)^2}{\sin (c+d x)^{3/2}}dx}{a}}{\sqrt {\sin (c+d x)} \sqrt {e \csc (c+d x)}}\) |
\(\Big \downarrow \) 3044 |
\(\displaystyle \frac {\frac {\int \frac {1}{\sin ^{\frac {3}{2}}(c+d x)}d\sin (c+d x)}{a d}-\frac {\int \frac {\cos (c+d x)^2}{\sin (c+d x)^{3/2}}dx}{a}}{\sqrt {\sin (c+d x)} \sqrt {e \csc (c+d x)}}\) |
\(\Big \downarrow \) 15 |
\(\displaystyle \frac {-\frac {\int \frac {\cos (c+d x)^2}{\sin (c+d x)^{3/2}}dx}{a}-\frac {2}{a d \sqrt {\sin (c+d x)}}}{\sqrt {\sin (c+d x)} \sqrt {e \csc (c+d x)}}\) |
\(\Big \downarrow \) 3047 |
\(\displaystyle \frac {-\frac {-2 \int \sqrt {\sin (c+d x)}dx-\frac {2 \cos (c+d x)}{d \sqrt {\sin (c+d x)}}}{a}-\frac {2}{a d \sqrt {\sin (c+d x)}}}{\sqrt {\sin (c+d x)} \sqrt {e \csc (c+d x)}}\) |
\(\Big \downarrow \) 3042 |
\(\displaystyle \frac {-\frac {-2 \int \sqrt {\sin (c+d x)}dx-\frac {2 \cos (c+d x)}{d \sqrt {\sin (c+d x)}}}{a}-\frac {2}{a d \sqrt {\sin (c+d x)}}}{\sqrt {\sin (c+d x)} \sqrt {e \csc (c+d x)}}\) |
\(\Big \downarrow \) 3119 |
\(\displaystyle \frac {-\frac {2}{a d \sqrt {\sin (c+d x)}}-\frac {-\frac {4 E\left (\left .\frac {1}{2} \left (c+d x-\frac {\pi }{2}\right )\right |2\right )}{d}-\frac {2 \cos (c+d x)}{d \sqrt {\sin (c+d x)}}}{a}}{\sqrt {\sin (c+d x)} \sqrt {e \csc (c+d x)}}\) |
(-(((-4*EllipticE[(c - Pi/2 + d*x)/2, 2])/d - (2*Cos[c + d*x])/(d*Sqrt[Sin [c + d*x]]))/a) - 2/(a*d*Sqrt[Sin[c + d*x]]))/(Sqrt[e*Csc[c + d*x]]*Sqrt[S in[c + d*x]])
3.3.96.3.1 Defintions of rubi rules used
Int[(a_.)*(x_)^(m_.), x_Symbol] :> Simp[a*(x^(m + 1)/(m + 1)), x] /; FreeQ[ {a, m}, x] && NeQ[m, -1]
Int[cos[(e_.) + (f_.)*(x_)]^(n_.)*((a_.)*sin[(e_.) + (f_.)*(x_)])^(m_.), x_ Symbol] :> Simp[1/(a*f) Subst[Int[x^m*(1 - x^2/a^2)^((n - 1)/2), x], x, a *Sin[e + f*x]], x] /; FreeQ[{a, e, f, m}, x] && IntegerQ[(n - 1)/2] && !(I ntegerQ[(m - 1)/2] && LtQ[0, m, n])
Int[(cos[(e_.) + (f_.)*(x_)]*(a_.))^(m_)*((b_.)*sin[(e_.) + (f_.)*(x_)])^(n _), x_Symbol] :> Simp[a*(a*Cos[e + f*x])^(m - 1)*((b*Sin[e + f*x])^(n + 1)/ (b*f*(n + 1))), x] + Simp[a^2*((m - 1)/(b^2*(n + 1))) Int[(a*Cos[e + f*x] )^(m - 2)*(b*Sin[e + f*x])^(n + 2), x], x] /; FreeQ[{a, b, e, f}, x] && GtQ [m, 1] && LtQ[n, -1] && (IntegersQ[2*m, 2*n] || EqQ[m + n, 0])
Int[Sqrt[sin[(c_.) + (d_.)*(x_)]], x_Symbol] :> Simp[(2/d)*EllipticE[(1/2)* (c - Pi/2 + d*x), 2], x] /; FreeQ[{c, d}, x]
Int[((cos[(e_.) + (f_.)*(x_)]*(g_.))^(p_)*((d_.)*sin[(e_.) + (f_.)*(x_)])^( n_.))/((a_) + (b_.)*sin[(e_.) + (f_.)*(x_)]), x_Symbol] :> Simp[g^2/a Int [(g*Cos[e + f*x])^(p - 2)*(d*Sin[e + f*x])^n, x], x] - Simp[g^2/(b*d) Int [(g*Cos[e + f*x])^(p - 2)*(d*Sin[e + f*x])^(n + 1), x], x] /; FreeQ[{a, b, d, e, f, g, n, p}, x] && EqQ[a^2 - b^2, 0]
Int[(cos[(e_.) + (f_.)*(x_)]*(g_.))^(p_.)*(csc[(e_.) + (f_.)*(x_)]*(b_.) + (a_))^(m_.), x_Symbol] :> Int[(g*Cos[e + f*x])^p*((b + a*Sin[e + f*x])^m/Si n[e + f*x]^m), x] /; FreeQ[{a, b, e, f, g, p}, x] && IntegerQ[m]
Int[(csc[(e_.) + (f_.)*(x_)]*(b_.) + (a_))^(m_.)*((g_.)*sec[(e_.) + (f_.)*( x_)])^(p_), x_Symbol] :> Simp[g^IntPart[p]*(g*Sec[e + f*x])^FracPart[p]*Cos [e + f*x]^FracPart[p] Int[(a + b*Csc[e + f*x])^m/Cos[e + f*x]^p, x], x] / ; FreeQ[{a, b, e, f, g, m, p}, x] && !IntegerQ[p]
Result contains complex when optimal does not.
Time = 7.46 (sec) , antiderivative size = 432, normalized size of antiderivative = 4.36
method | result | size |
default | \(-\frac {\sqrt {2}\, \left (4 \sqrt {-i \left (i-\cot \left (d x +c \right )+\csc \left (d x +c \right )\right )}\, \sqrt {-i \left (i+\cot \left (d x +c \right )-\csc \left (d x +c \right )\right )}\, \sqrt {-i \left (\cot \left (d x +c \right )-\csc \left (d x +c \right )\right )}\, \operatorname {EllipticE}\left (\sqrt {-i \left (i-\cot \left (d x +c \right )+\csc \left (d x +c \right )\right )}, \frac {\sqrt {2}}{2}\right ) \cos \left (d x +c \right )-2 \sqrt {-i \left (i-\cot \left (d x +c \right )+\csc \left (d x +c \right )\right )}\, \sqrt {-i \left (i+\cot \left (d x +c \right )-\csc \left (d x +c \right )\right )}\, \sqrt {-i \left (\cot \left (d x +c \right )-\csc \left (d x +c \right )\right )}\, \operatorname {EllipticF}\left (\sqrt {-i \left (i-\cot \left (d x +c \right )+\csc \left (d x +c \right )\right )}, \frac {\sqrt {2}}{2}\right ) \cos \left (d x +c \right )+4 \sqrt {-i \left (i-\cot \left (d x +c \right )+\csc \left (d x +c \right )\right )}\, \sqrt {-i \left (i+\cot \left (d x +c \right )-\csc \left (d x +c \right )\right )}\, \sqrt {-i \left (\cot \left (d x +c \right )-\csc \left (d x +c \right )\right )}\, \operatorname {EllipticE}\left (\sqrt {-i \left (i-\cot \left (d x +c \right )+\csc \left (d x +c \right )\right )}, \frac {\sqrt {2}}{2}\right )-2 \sqrt {-i \left (i-\cot \left (d x +c \right )+\csc \left (d x +c \right )\right )}\, \sqrt {-i \left (i+\cot \left (d x +c \right )-\csc \left (d x +c \right )\right )}\, \sqrt {-i \left (\cot \left (d x +c \right )-\csc \left (d x +c \right )\right )}\, \operatorname {EllipticF}\left (\sqrt {-i \left (i-\cot \left (d x +c \right )+\csc \left (d x +c \right )\right )}, \frac {\sqrt {2}}{2}\right )+\sqrt {2}\, \cos \left (d x +c \right )-\sqrt {2}\right ) \csc \left (d x +c \right )}{a d \sqrt {e \csc \left (d x +c \right )}}\) | \(432\) |
-1/a/d*2^(1/2)*(4*(-I*(I-cot(d*x+c)+csc(d*x+c)))^(1/2)*(-I*(I+cot(d*x+c)-c sc(d*x+c)))^(1/2)*(-I*(cot(d*x+c)-csc(d*x+c)))^(1/2)*EllipticE((-I*(I-cot( d*x+c)+csc(d*x+c)))^(1/2),1/2*2^(1/2))*cos(d*x+c)-2*(-I*(I-cot(d*x+c)+csc( d*x+c)))^(1/2)*(-I*(I+cot(d*x+c)-csc(d*x+c)))^(1/2)*(-I*(cot(d*x+c)-csc(d* x+c)))^(1/2)*EllipticF((-I*(I-cot(d*x+c)+csc(d*x+c)))^(1/2),1/2*2^(1/2))*c os(d*x+c)+4*(-I*(I-cot(d*x+c)+csc(d*x+c)))^(1/2)*(-I*(I+cot(d*x+c)-csc(d*x +c)))^(1/2)*(-I*(cot(d*x+c)-csc(d*x+c)))^(1/2)*EllipticE((-I*(I-cot(d*x+c) +csc(d*x+c)))^(1/2),1/2*2^(1/2))-2*(-I*(I-cot(d*x+c)+csc(d*x+c)))^(1/2)*(- I*(I+cot(d*x+c)-csc(d*x+c)))^(1/2)*(-I*(cot(d*x+c)-csc(d*x+c)))^(1/2)*Elli pticF((-I*(I-cot(d*x+c)+csc(d*x+c)))^(1/2),1/2*2^(1/2))+2^(1/2)*cos(d*x+c) -2^(1/2))/(e*csc(d*x+c))^(1/2)*csc(d*x+c)
Result contains higher order function than in optimal. Order 9 vs. order 4.
Time = 0.09 (sec) , antiderivative size = 87, normalized size of antiderivative = 0.88 \[ \int \frac {1}{\sqrt {e \csc (c+d x)} (a+a \sec (c+d x))} \, dx=\frac {2 \, {\left (\sqrt {\frac {e}{\sin \left (d x + c\right )}} {\left (\cos \left (d x + c\right ) - 1\right )} + \sqrt {2 i \, e} {\rm weierstrassZeta}\left (4, 0, {\rm weierstrassPInverse}\left (4, 0, \cos \left (d x + c\right ) + i \, \sin \left (d x + c\right )\right )\right ) + \sqrt {-2 i \, e} {\rm weierstrassZeta}\left (4, 0, {\rm weierstrassPInverse}\left (4, 0, \cos \left (d x + c\right ) - i \, \sin \left (d x + c\right )\right )\right )\right )}}{a d e} \]
2*(sqrt(e/sin(d*x + c))*(cos(d*x + c) - 1) + sqrt(2*I*e)*weierstrassZeta(4 , 0, weierstrassPInverse(4, 0, cos(d*x + c) + I*sin(d*x + c))) + sqrt(-2*I *e)*weierstrassZeta(4, 0, weierstrassPInverse(4, 0, cos(d*x + c) - I*sin(d *x + c))))/(a*d*e)
\[ \int \frac {1}{\sqrt {e \csc (c+d x)} (a+a \sec (c+d x))} \, dx=\frac {\int \frac {1}{\sqrt {e \csc {\left (c + d x \right )}} \sec {\left (c + d x \right )} + \sqrt {e \csc {\left (c + d x \right )}}}\, dx}{a} \]
\[ \int \frac {1}{\sqrt {e \csc (c+d x)} (a+a \sec (c+d x))} \, dx=\int { \frac {1}{\sqrt {e \csc \left (d x + c\right )} {\left (a \sec \left (d x + c\right ) + a\right )}} \,d x } \]
\[ \int \frac {1}{\sqrt {e \csc (c+d x)} (a+a \sec (c+d x))} \, dx=\int { \frac {1}{\sqrt {e \csc \left (d x + c\right )} {\left (a \sec \left (d x + c\right ) + a\right )}} \,d x } \]
Timed out. \[ \int \frac {1}{\sqrt {e \csc (c+d x)} (a+a \sec (c+d x))} \, dx=\int \frac {\cos \left (c+d\,x\right )}{a\,\sqrt {\frac {e}{\sin \left (c+d\,x\right )}}\,\left (\cos \left (c+d\,x\right )+1\right )} \,d x \]