\(\int \frac {(d \sec (e+f x))^{5/2}}{(a+b \tan (e+f x))^2} \, dx\) [611]
Optimal result
Integrand size = 25, antiderivative size = 440 \[
\int \frac {(d \sec (e+f x))^{5/2}}{(a+b \tan (e+f x))^2} \, dx=\frac {a d^2 \arctan \left (\frac {\sqrt {b} \sqrt [4]{\sec ^2(e+f x)}}{\sqrt [4]{a^2+b^2}}\right ) \sqrt {d \sec (e+f x)}}{2 b^{3/2} \left (a^2+b^2\right )^{3/4} f \sqrt [4]{\sec ^2(e+f x)}}+\frac {a d^2 \text {arctanh}\left (\frac {\sqrt {b} \sqrt [4]{\sec ^2(e+f x)}}{\sqrt [4]{a^2+b^2}}\right ) \sqrt {d \sec (e+f x)}}{2 b^{3/2} \left (a^2+b^2\right )^{3/4} f \sqrt [4]{\sec ^2(e+f x)}}+\frac {d^2 \operatorname {EllipticF}\left (\frac {1}{2} \arctan (\tan (e+f x)),2\right ) \sqrt {d \sec (e+f x)}}{b^2 f \sqrt [4]{\sec ^2(e+f x)}}-\frac {a^2 d^2 \cot (e+f x) \operatorname {EllipticPi}\left (-\frac {b}{\sqrt {a^2+b^2}},\arcsin \left (\sqrt [4]{\sec ^2(e+f x)}\right ),-1\right ) \sqrt {d \sec (e+f x)} \sqrt {-\tan ^2(e+f x)}}{2 b^2 \left (a^2+b^2\right ) f \sqrt [4]{\sec ^2(e+f x)}}-\frac {a^2 d^2 \cot (e+f x) \operatorname {EllipticPi}\left (\frac {b}{\sqrt {a^2+b^2}},\arcsin \left (\sqrt [4]{\sec ^2(e+f x)}\right ),-1\right ) \sqrt {d \sec (e+f x)} \sqrt {-\tan ^2(e+f x)}}{2 b^2 \left (a^2+b^2\right ) f \sqrt [4]{\sec ^2(e+f x)}}-\frac {d^2 \sqrt {d \sec (e+f x)}}{b f (a+b \tan (e+f x))}
\]
[Out]
1/2*a*d^2*arctan((sec(f*x+e)^2)^(1/4)*b^(1/2)/(a^2+b^2)^(1/4))*(d*sec(f*x+e))^(1/2)/b^(3/2)/(a^2+b^2)^(3/4)/f/
(sec(f*x+e)^2)^(1/4)+1/2*a*d^2*arctanh((sec(f*x+e)^2)^(1/4)*b^(1/2)/(a^2+b^2)^(1/4))*(d*sec(f*x+e))^(1/2)/b^(3
/2)/(a^2+b^2)^(3/4)/f/(sec(f*x+e)^2)^(1/4)+d^2*(cos(1/2*arctan(tan(f*x+e)))^2)^(1/2)/cos(1/2*arctan(tan(f*x+e)
))*EllipticF(sin(1/2*arctan(tan(f*x+e))),2^(1/2))*(d*sec(f*x+e))^(1/2)/b^2/f/(sec(f*x+e)^2)^(1/4)-1/2*a^2*d^2*
cot(f*x+e)*EllipticPi((sec(f*x+e)^2)^(1/4),-b/(a^2+b^2)^(1/2),I)*(d*sec(f*x+e))^(1/2)*(-tan(f*x+e)^2)^(1/2)/b^
2/(a^2+b^2)/f/(sec(f*x+e)^2)^(1/4)-1/2*a^2*d^2*cot(f*x+e)*EllipticPi((sec(f*x+e)^2)^(1/4),b/(a^2+b^2)^(1/2),I)
*(d*sec(f*x+e))^(1/2)*(-tan(f*x+e)^2)^(1/2)/b^2/(a^2+b^2)/f/(sec(f*x+e)^2)^(1/4)-d^2*(d*sec(f*x+e))^(1/2)/b/f/
(a+b*tan(f*x+e))
Rubi [A] (verified)
Time = 0.46 (sec) , antiderivative size = 440, normalized size of antiderivative = 1.00, number of
steps used = 17, number of rules used = 15, \(\frac {\text {number of rules}}{\text {integrand size}}\) = 0.600, Rules used = {3593, 747, 858, 237, 761,
410, 109, 418, 1227, 551, 455, 65, 218, 214, 211} \[
\int \frac {(d \sec (e+f x))^{5/2}}{(a+b \tan (e+f x))^2} \, dx=-\frac {a^2 d^2 \sqrt {-\tan ^2(e+f x)} \cot (e+f x) \sqrt {d \sec (e+f x)} \operatorname {EllipticPi}\left (-\frac {b}{\sqrt {a^2+b^2}},\arcsin \left (\sqrt [4]{\sec ^2(e+f x)}\right ),-1\right )}{2 b^2 f \left (a^2+b^2\right ) \sqrt [4]{\sec ^2(e+f x)}}-\frac {a^2 d^2 \sqrt {-\tan ^2(e+f x)} \cot (e+f x) \sqrt {d \sec (e+f x)} \operatorname {EllipticPi}\left (\frac {b}{\sqrt {a^2+b^2}},\arcsin \left (\sqrt [4]{\sec ^2(e+f x)}\right ),-1\right )}{2 b^2 f \left (a^2+b^2\right ) \sqrt [4]{\sec ^2(e+f x)}}+\frac {a d^2 \sqrt {d \sec (e+f x)} \arctan \left (\frac {\sqrt {b} \sqrt [4]{\sec ^2(e+f x)}}{\sqrt [4]{a^2+b^2}}\right )}{2 b^{3/2} f \left (a^2+b^2\right )^{3/4} \sqrt [4]{\sec ^2(e+f x)}}+\frac {a d^2 \sqrt {d \sec (e+f x)} \text {arctanh}\left (\frac {\sqrt {b} \sqrt [4]{\sec ^2(e+f x)}}{\sqrt [4]{a^2+b^2}}\right )}{2 b^{3/2} f \left (a^2+b^2\right )^{3/4} \sqrt [4]{\sec ^2(e+f x)}}-\frac {d^2 \sqrt {d \sec (e+f x)}}{b f (a+b \tan (e+f x))}+\frac {d^2 \sqrt {d \sec (e+f x)} \operatorname {EllipticF}\left (\frac {1}{2} \arctan (\tan (e+f x)),2\right )}{b^2 f \sqrt [4]{\sec ^2(e+f x)}}
\]
[In]
Int[(d*Sec[e + f*x])^(5/2)/(a + b*Tan[e + f*x])^2,x]
[Out]
(a*d^2*ArcTan[(Sqrt[b]*(Sec[e + f*x]^2)^(1/4))/(a^2 + b^2)^(1/4)]*Sqrt[d*Sec[e + f*x]])/(2*b^(3/2)*(a^2 + b^2)
^(3/4)*f*(Sec[e + f*x]^2)^(1/4)) + (a*d^2*ArcTanh[(Sqrt[b]*(Sec[e + f*x]^2)^(1/4))/(a^2 + b^2)^(1/4)]*Sqrt[d*S
ec[e + f*x]])/(2*b^(3/2)*(a^2 + b^2)^(3/4)*f*(Sec[e + f*x]^2)^(1/4)) + (d^2*EllipticF[ArcTan[Tan[e + f*x]]/2,
2]*Sqrt[d*Sec[e + f*x]])/(b^2*f*(Sec[e + f*x]^2)^(1/4)) - (a^2*d^2*Cot[e + f*x]*EllipticPi[-(b/Sqrt[a^2 + b^2]
), ArcSin[(Sec[e + f*x]^2)^(1/4)], -1]*Sqrt[d*Sec[e + f*x]]*Sqrt[-Tan[e + f*x]^2])/(2*b^2*(a^2 + b^2)*f*(Sec[e
+ f*x]^2)^(1/4)) - (a^2*d^2*Cot[e + f*x]*EllipticPi[b/Sqrt[a^2 + b^2], ArcSin[(Sec[e + f*x]^2)^(1/4)], -1]*Sq
rt[d*Sec[e + f*x]]*Sqrt[-Tan[e + f*x]^2])/(2*b^2*(a^2 + b^2)*f*(Sec[e + f*x]^2)^(1/4)) - (d^2*Sqrt[d*Sec[e + f
*x]])/(b*f*(a + b*Tan[e + f*x]))
Rule 65
Int[((a_.) + (b_.)*(x_))^(m_)*((c_.) + (d_.)*(x_))^(n_), x_Symbol] :> With[{p = Denominator[m]}, Dist[p/b, Sub
st[Int[x^(p*(m + 1) - 1)*(c - a*(d/b) + d*(x^p/b))^n, x], x, (a + b*x)^(1/p)], x]] /; FreeQ[{a, b, c, d}, x] &
& NeQ[b*c - a*d, 0] && LtQ[-1, m, 0] && LeQ[-1, n, 0] && LeQ[Denominator[n], Denominator[m]] && IntLinearQ[a,
b, c, d, m, n, x]
Rule 109
Int[1/(((a_.) + (b_.)*(x_))*Sqrt[(c_.) + (d_.)*(x_)]*((e_.) + (f_.)*(x_))^(3/4)), x_Symbol] :> Dist[-4, Subst[
Int[1/((b*e - a*f - b*x^4)*Sqrt[c - d*(e/f) + d*(x^4/f)]), x], x, (e + f*x)^(1/4)], x] /; FreeQ[{a, b, c, d, e
, f}, x] && GtQ[-f/(d*e - c*f), 0]
Rule 211
Int[((a_) + (b_.)*(x_)^2)^(-1), x_Symbol] :> Simp[(Rt[a/b, 2]/a)*ArcTan[x/Rt[a/b, 2]], x] /; FreeQ[{a, b}, x]
&& PosQ[a/b]
Rule 214
Int[((a_) + (b_.)*(x_)^2)^(-1), x_Symbol] :> Simp[(Rt[-a/b, 2]/a)*ArcTanh[x/Rt[-a/b, 2]], x] /; FreeQ[{a, b},
x] && NegQ[a/b]
Rule 218
Int[((a_) + (b_.)*(x_)^4)^(-1), x_Symbol] :> With[{r = Numerator[Rt[-a/b, 2]], s = Denominator[Rt[-a/b, 2]]},
Dist[r/(2*a), Int[1/(r - s*x^2), x], x] + Dist[r/(2*a), Int[1/(r + s*x^2), x], x]] /; FreeQ[{a, b}, x] && !Gt
Q[a/b, 0]
Rule 237
Int[((a_) + (b_.)*(x_)^2)^(-3/4), x_Symbol] :> Simp[(2/(a^(3/4)*Rt[b/a, 2]))*EllipticF[(1/2)*ArcTan[Rt[b/a, 2]
*x], 2], x] /; FreeQ[{a, b}, x] && GtQ[a, 0] && PosQ[b/a]
Rule 410
Int[1/(((a_) + (b_.)*(x_)^2)^(3/4)*((c_) + (d_.)*(x_)^2)), x_Symbol] :> Dist[Sqrt[(-b)*(x^2/a)]/(2*x), Subst[I
nt[1/(Sqrt[(-b)*(x/a)]*(a + b*x)^(3/4)*(c + d*x)), x], x, x^2], x] /; FreeQ[{a, b, c, d}, x] && NeQ[b*c - a*d,
0]
Rule 418
Int[1/(Sqrt[(a_) + (b_.)*(x_)^4]*((c_) + (d_.)*(x_)^4)), x_Symbol] :> Dist[1/(2*c), Int[1/(Sqrt[a + b*x^4]*(1
- Rt[-d/c, 2]*x^2)), x], x] + Dist[1/(2*c), Int[1/(Sqrt[a + b*x^4]*(1 + Rt[-d/c, 2]*x^2)), x], x] /; FreeQ[{a,
b, c, d}, x] && NeQ[b*c - a*d, 0]
Rule 455
Int[(x_)^(m_.)*((a_) + (b_.)*(x_)^(n_))^(p_.)*((c_) + (d_.)*(x_)^(n_))^(q_.), x_Symbol] :> Dist[1/n, Subst[Int
[(a + b*x)^p*(c + d*x)^q, x], x, x^n], x] /; FreeQ[{a, b, c, d, m, n, p, q}, x] && NeQ[b*c - a*d, 0] && EqQ[m
- n + 1, 0]
Rule 551
Int[1/(((a_) + (b_.)*(x_)^2)*Sqrt[(c_) + (d_.)*(x_)^2]*Sqrt[(e_) + (f_.)*(x_)^2]), x_Symbol] :> Simp[(1/(a*Sqr
t[c]*Sqrt[e]*Rt[-d/c, 2]))*EllipticPi[b*(c/(a*d)), ArcSin[Rt[-d/c, 2]*x], c*(f/(d*e))], x] /; FreeQ[{a, b, c,
d, e, f}, x] && !GtQ[d/c, 0] && GtQ[c, 0] && GtQ[e, 0] && !( !GtQ[f/e, 0] && SimplerSqrtQ[-f/e, -d/c])
Rule 747
Int[((d_) + (e_.)*(x_))^(m_)*((a_) + (c_.)*(x_)^2)^(p_), x_Symbol] :> Simp[(d + e*x)^(m + 1)*((a + c*x^2)^p/(e
*(m + 1))), x] - Dist[2*c*(p/(e*(m + 1))), Int[x*(d + e*x)^(m + 1)*(a + c*x^2)^(p - 1), x], x] /; FreeQ[{a, c,
d, e, m}, x] && NeQ[c*d^2 + a*e^2, 0] && GtQ[p, 0] && (IntegerQ[p] || LtQ[m, -1]) && NeQ[m, -1] && !ILtQ[m +
2*p + 1, 0] && IntQuadraticQ[a, 0, c, d, e, m, p, x]
Rule 761
Int[1/(((d_) + (e_.)*(x_))*((a_) + (c_.)*(x_)^2)^(3/4)), x_Symbol] :> Dist[d, Int[1/((d^2 - e^2*x^2)*(a + c*x^
2)^(3/4)), x], x] - Dist[e, Int[x/((d^2 - e^2*x^2)*(a + c*x^2)^(3/4)), x], x] /; FreeQ[{a, c, d, e}, x] && NeQ
[c*d^2 + a*e^2, 0]
Rule 858
Int[((d_.) + (e_.)*(x_))^(m_)*((f_.) + (g_.)*(x_))*((a_) + (c_.)*(x_)^2)^(p_.), x_Symbol] :> Dist[g/e, Int[(d
+ e*x)^(m + 1)*(a + c*x^2)^p, x], x] + Dist[(e*f - d*g)/e, Int[(d + e*x)^m*(a + c*x^2)^p, x], x] /; FreeQ[{a,
c, d, e, f, g, m, p}, x] && NeQ[c*d^2 + a*e^2, 0] && !IGtQ[m, 0]
Rule 1227
Int[1/(((d_) + (e_.)*(x_)^2)*Sqrt[(a_) + (c_.)*(x_)^4]), x_Symbol] :> With[{q = Rt[(-a)*c, 2]}, Dist[Sqrt[-c],
Int[1/((d + e*x^2)*Sqrt[q + c*x^2]*Sqrt[q - c*x^2]), x], x]] /; FreeQ[{a, c, d, e}, x] && GtQ[a, 0] && LtQ[c,
0]
Rule 3593
Int[((d_.)*sec[(e_.) + (f_.)*(x_)])^(m_.)*((a_) + (b_.)*tan[(e_.) + (f_.)*(x_)])^(n_), x_Symbol] :> Dist[d^(2*
IntPart[m/2])*((d*Sec[e + f*x])^(2*FracPart[m/2])/(b*f*(Sec[e + f*x]^2)^FracPart[m/2])), Subst[Int[(a + x)^n*(
1 + x^2/b^2)^(m/2 - 1), x], x, b*Tan[e + f*x]], x] /; FreeQ[{a, b, d, e, f, m, n}, x] && NeQ[a^2 + b^2, 0] &&
!IntegerQ[m/2]
Rubi steps \begin{align*}
\text {integral}& = \frac {\left (d^2 \sqrt {d \sec (e+f x)}\right ) \text {Subst}\left (\int \frac {\sqrt [4]{1+\frac {x^2}{b^2}}}{(a+x)^2} \, dx,x,b \tan (e+f x)\right )}{b f \sqrt [4]{\sec ^2(e+f x)}} \\ & = -\frac {d^2 \sqrt {d \sec (e+f x)}}{b f (a+b \tan (e+f x))}+\frac {\left (d^2 \sqrt {d \sec (e+f x)}\right ) \text {Subst}\left (\int \frac {x}{(a+x) \left (1+\frac {x^2}{b^2}\right )^{3/4}} \, dx,x,b \tan (e+f x)\right )}{2 b^3 f \sqrt [4]{\sec ^2(e+f x)}} \\ & = -\frac {d^2 \sqrt {d \sec (e+f x)}}{b f (a+b \tan (e+f x))}+\frac {\left (d^2 \sqrt {d \sec (e+f x)}\right ) \text {Subst}\left (\int \frac {1}{\left (1+\frac {x^2}{b^2}\right )^{3/4}} \, dx,x,b \tan (e+f x)\right )}{2 b^3 f \sqrt [4]{\sec ^2(e+f x)}}-\frac {\left (a d^2 \sqrt {d \sec (e+f x)}\right ) \text {Subst}\left (\int \frac {1}{(a+x) \left (1+\frac {x^2}{b^2}\right )^{3/4}} \, dx,x,b \tan (e+f x)\right )}{2 b^3 f \sqrt [4]{\sec ^2(e+f x)}} \\ & = \frac {d^2 \operatorname {EllipticF}\left (\frac {1}{2} \arctan (\tan (e+f x)),2\right ) \sqrt {d \sec (e+f x)}}{b^2 f \sqrt [4]{\sec ^2(e+f x)}}-\frac {d^2 \sqrt {d \sec (e+f x)}}{b f (a+b \tan (e+f x))}+\frac {\left (a d^2 \sqrt {d \sec (e+f x)}\right ) \text {Subst}\left (\int \frac {x}{\left (a^2-x^2\right ) \left (1+\frac {x^2}{b^2}\right )^{3/4}} \, dx,x,b \tan (e+f x)\right )}{2 b^3 f \sqrt [4]{\sec ^2(e+f x)}}-\frac {\left (a^2 d^2 \sqrt {d \sec (e+f x)}\right ) \text {Subst}\left (\int \frac {1}{\left (a^2-x^2\right ) \left (1+\frac {x^2}{b^2}\right )^{3/4}} \, dx,x,b \tan (e+f x)\right )}{2 b^3 f \sqrt [4]{\sec ^2(e+f x)}} \\ & = \frac {d^2 \operatorname {EllipticF}\left (\frac {1}{2} \arctan (\tan (e+f x)),2\right ) \sqrt {d \sec (e+f x)}}{b^2 f \sqrt [4]{\sec ^2(e+f x)}}-\frac {d^2 \sqrt {d \sec (e+f x)}}{b f (a+b \tan (e+f x))}+\frac {\left (a d^2 \sqrt {d \sec (e+f x)}\right ) \text {Subst}\left (\int \frac {1}{\left (a^2-x\right ) \left (1+\frac {x}{b^2}\right )^{3/4}} \, dx,x,b^2 \tan ^2(e+f x)\right )}{4 b^3 f \sqrt [4]{\sec ^2(e+f x)}}-\frac {\left (a^2 d^2 \cot (e+f x) \sqrt {d \sec (e+f x)} \sqrt {-\tan ^2(e+f x)}\right ) \text {Subst}\left (\int \frac {1}{\left (a^2-x\right ) \sqrt {-\frac {x}{b^2}} \left (1+\frac {x}{b^2}\right )^{3/4}} \, dx,x,b^2 \tan ^2(e+f x)\right )}{4 b^4 f \sqrt [4]{\sec ^2(e+f x)}} \\ & = \frac {d^2 \operatorname {EllipticF}\left (\frac {1}{2} \arctan (\tan (e+f x)),2\right ) \sqrt {d \sec (e+f x)}}{b^2 f \sqrt [4]{\sec ^2(e+f x)}}-\frac {d^2 \sqrt {d \sec (e+f x)}}{b f (a+b \tan (e+f x))}+\frac {\left (a d^2 \sqrt {d \sec (e+f x)}\right ) \text {Subst}\left (\int \frac {1}{a^2+b^2-b^2 x^4} \, dx,x,\sqrt [4]{\sec ^2(e+f x)}\right )}{b f \sqrt [4]{\sec ^2(e+f x)}}+\frac {\left (a^2 d^2 \cot (e+f x) \sqrt {d \sec (e+f x)} \sqrt {-\tan ^2(e+f x)}\right ) \text {Subst}\left (\int \frac {1}{\sqrt {1-x^4} \left (-1-\frac {a^2}{b^2}+x^4\right )} \, dx,x,\sqrt [4]{\sec ^2(e+f x)}\right )}{b^4 f \sqrt [4]{\sec ^2(e+f x)}} \\ & = \frac {d^2 \operatorname {EllipticF}\left (\frac {1}{2} \arctan (\tan (e+f x)),2\right ) \sqrt {d \sec (e+f x)}}{b^2 f \sqrt [4]{\sec ^2(e+f x)}}-\frac {d^2 \sqrt {d \sec (e+f x)}}{b f (a+b \tan (e+f x))}+\frac {\left (a d^2 \sqrt {d \sec (e+f x)}\right ) \text {Subst}\left (\int \frac {1}{\sqrt {a^2+b^2}-b x^2} \, dx,x,\sqrt [4]{\sec ^2(e+f x)}\right )}{2 b \sqrt {a^2+b^2} f \sqrt [4]{\sec ^2(e+f x)}}+\frac {\left (a d^2 \sqrt {d \sec (e+f x)}\right ) \text {Subst}\left (\int \frac {1}{\sqrt {a^2+b^2}+b x^2} \, dx,x,\sqrt [4]{\sec ^2(e+f x)}\right )}{2 b \sqrt {a^2+b^2} f \sqrt [4]{\sec ^2(e+f x)}}-\frac {\left (a^2 d^2 \cot (e+f x) \sqrt {d \sec (e+f x)} \sqrt {-\tan ^2(e+f x)}\right ) \text {Subst}\left (\int \frac {1}{\left (1-\frac {b x^2}{\sqrt {a^2+b^2}}\right ) \sqrt {1-x^4}} \, dx,x,\sqrt [4]{\sec ^2(e+f x)}\right )}{2 b^2 \left (a^2+b^2\right ) f \sqrt [4]{\sec ^2(e+f x)}}-\frac {\left (a^2 d^2 \cot (e+f x) \sqrt {d \sec (e+f x)} \sqrt {-\tan ^2(e+f x)}\right ) \text {Subst}\left (\int \frac {1}{\left (1+\frac {b x^2}{\sqrt {a^2+b^2}}\right ) \sqrt {1-x^4}} \, dx,x,\sqrt [4]{\sec ^2(e+f x)}\right )}{2 b^2 \left (a^2+b^2\right ) f \sqrt [4]{\sec ^2(e+f x)}} \\ & = \frac {a d^2 \arctan \left (\frac {\sqrt {b} \sqrt [4]{\sec ^2(e+f x)}}{\sqrt [4]{a^2+b^2}}\right ) \sqrt {d \sec (e+f x)}}{2 b^{3/2} \left (a^2+b^2\right )^{3/4} f \sqrt [4]{\sec ^2(e+f x)}}+\frac {a d^2 \text {arctanh}\left (\frac {\sqrt {b} \sqrt [4]{\sec ^2(e+f x)}}{\sqrt [4]{a^2+b^2}}\right ) \sqrt {d \sec (e+f x)}}{2 b^{3/2} \left (a^2+b^2\right )^{3/4} f \sqrt [4]{\sec ^2(e+f x)}}+\frac {d^2 \operatorname {EllipticF}\left (\frac {1}{2} \arctan (\tan (e+f x)),2\right ) \sqrt {d \sec (e+f x)}}{b^2 f \sqrt [4]{\sec ^2(e+f x)}}-\frac {d^2 \sqrt {d \sec (e+f x)}}{b f (a+b \tan (e+f x))}-\frac {\left (a^2 d^2 \cot (e+f x) \sqrt {d \sec (e+f x)} \sqrt {-\tan ^2(e+f x)}\right ) \text {Subst}\left (\int \frac {1}{\sqrt {1-x^2} \sqrt {1+x^2} \left (1-\frac {b x^2}{\sqrt {a^2+b^2}}\right )} \, dx,x,\sqrt [4]{\sec ^2(e+f x)}\right )}{2 b^2 \left (a^2+b^2\right ) f \sqrt [4]{\sec ^2(e+f x)}}-\frac {\left (a^2 d^2 \cot (e+f x) \sqrt {d \sec (e+f x)} \sqrt {-\tan ^2(e+f x)}\right ) \text {Subst}\left (\int \frac {1}{\sqrt {1-x^2} \sqrt {1+x^2} \left (1+\frac {b x^2}{\sqrt {a^2+b^2}}\right )} \, dx,x,\sqrt [4]{\sec ^2(e+f x)}\right )}{2 b^2 \left (a^2+b^2\right ) f \sqrt [4]{\sec ^2(e+f x)}} \\ & = \frac {a d^2 \arctan \left (\frac {\sqrt {b} \sqrt [4]{\sec ^2(e+f x)}}{\sqrt [4]{a^2+b^2}}\right ) \sqrt {d \sec (e+f x)}}{2 b^{3/2} \left (a^2+b^2\right )^{3/4} f \sqrt [4]{\sec ^2(e+f x)}}+\frac {a d^2 \text {arctanh}\left (\frac {\sqrt {b} \sqrt [4]{\sec ^2(e+f x)}}{\sqrt [4]{a^2+b^2}}\right ) \sqrt {d \sec (e+f x)}}{2 b^{3/2} \left (a^2+b^2\right )^{3/4} f \sqrt [4]{\sec ^2(e+f x)}}+\frac {d^2 \operatorname {EllipticF}\left (\frac {1}{2} \arctan (\tan (e+f x)),2\right ) \sqrt {d \sec (e+f x)}}{b^2 f \sqrt [4]{\sec ^2(e+f x)}}-\frac {a^2 d^2 \cot (e+f x) \operatorname {EllipticPi}\left (-\frac {b}{\sqrt {a^2+b^2}},\arcsin \left (\sqrt [4]{\sec ^2(e+f x)}\right ),-1\right ) \sqrt {d \sec (e+f x)} \sqrt {-\tan ^2(e+f x)}}{2 b^2 \left (a^2+b^2\right ) f \sqrt [4]{\sec ^2(e+f x)}}-\frac {a^2 d^2 \cot (e+f x) \operatorname {EllipticPi}\left (\frac {b}{\sqrt {a^2+b^2}},\arcsin \left (\sqrt [4]{\sec ^2(e+f x)}\right ),-1\right ) \sqrt {d \sec (e+f x)} \sqrt {-\tan ^2(e+f x)}}{2 b^2 \left (a^2+b^2\right ) f \sqrt [4]{\sec ^2(e+f x)}}-\frac {d^2 \sqrt {d \sec (e+f x)}}{b f (a+b \tan (e+f x))} \\
\end{align*}
Mathematica [C] (verified)
Result contains higher order function than in optimal. Order 5 vs. order 4 in optimal.
Time = 12.02 (sec) , antiderivative size = 378, normalized size of antiderivative = 0.86
\[
\int \frac {(d \sec (e+f x))^{5/2}}{(a+b \tan (e+f x))^2} \, dx=\frac {(d \sec (e+f x))^{5/2} (a \cos (e+f x)+b \sin (e+f x))^2 \left (-\frac {1}{a b}+\frac {\sin (e+f x)}{a (a \cos (e+f x)+b \sin (e+f x))}\right )}{f (a+b \tan (e+f x))^2}+\frac {\cos ^2(e+f x) (d \sec (e+f x))^{5/2} \sec ^2(e+f x)^{3/4} (a \cos (e+f x)+b \sin (e+f x))^2 \left (\operatorname {Hypergeometric2F1}\left (\frac {1}{2},\frac {3}{4},\frac {3}{2},-\tan ^2(e+f x)\right ) \tan (e+f x)+\frac {a \left (a \operatorname {EllipticPi}\left (-\frac {b}{\sqrt {a^2+b^2}},\arcsin \left (\sqrt [4]{\sec ^2(e+f x)}\right ),-1\right ) \tan (e+f x)+a \operatorname {EllipticPi}\left (\frac {b}{\sqrt {a^2+b^2}},\arcsin \left (\sqrt [4]{\sec ^2(e+f x)}\right ),-1\right ) \tan (e+f x)+\sqrt {b} \sqrt [4]{a^2+b^2} \left (\arctan \left (\frac {\sqrt {b} \sqrt [4]{\sec ^2(e+f x)}}{\sqrt [4]{a^2+b^2}}\right )+\text {arctanh}\left (\frac {\sqrt {b} \sqrt [4]{\sec ^2(e+f x)}}{\sqrt [4]{a^2+b^2}}\right )\right ) \sqrt {-\tan ^2(e+f x)}\right )}{\left (a^2+b^2\right ) \sqrt {-\tan ^2(e+f x)}}\right )}{2 b^2 f (a+b \tan (e+f x))^2}
\]
[In]
Integrate[(d*Sec[e + f*x])^(5/2)/(a + b*Tan[e + f*x])^2,x]
[Out]
((d*Sec[e + f*x])^(5/2)*(a*Cos[e + f*x] + b*Sin[e + f*x])^2*(-(1/(a*b)) + Sin[e + f*x]/(a*(a*Cos[e + f*x] + b*
Sin[e + f*x]))))/(f*(a + b*Tan[e + f*x])^2) + (Cos[e + f*x]^2*(d*Sec[e + f*x])^(5/2)*(Sec[e + f*x]^2)^(3/4)*(a
*Cos[e + f*x] + b*Sin[e + f*x])^2*(Hypergeometric2F1[1/2, 3/4, 3/2, -Tan[e + f*x]^2]*Tan[e + f*x] + (a*(a*Elli
pticPi[-(b/Sqrt[a^2 + b^2]), ArcSin[(Sec[e + f*x]^2)^(1/4)], -1]*Tan[e + f*x] + a*EllipticPi[b/Sqrt[a^2 + b^2]
, ArcSin[(Sec[e + f*x]^2)^(1/4)], -1]*Tan[e + f*x] + Sqrt[b]*(a^2 + b^2)^(1/4)*(ArcTan[(Sqrt[b]*(Sec[e + f*x]^
2)^(1/4))/(a^2 + b^2)^(1/4)] + ArcTanh[(Sqrt[b]*(Sec[e + f*x]^2)^(1/4))/(a^2 + b^2)^(1/4)])*Sqrt[-Tan[e + f*x]
^2]))/((a^2 + b^2)*Sqrt[-Tan[e + f*x]^2])))/(2*b^2*f*(a + b*Tan[e + f*x])^2)
Maple [B] (warning: unable to verify)
Both result and optimal contain complex but leaf count of result is larger than twice the leaf
count of optimal. 4811 vs. \(2 (405 ) = 810\).
Time = 128.71 (sec) , antiderivative size = 4812, normalized size of antiderivative =
10.94
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method | result | size |
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\(\text {Expression too large to display}\) |
\(4812\) |
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[In]
int((d*sec(f*x+e))^(5/2)/(a+b*tan(f*x+e))^2,x,method=_RETURNVERBOSE)
[Out]
-1/4*d^2/f*(-d*(csc(f*x+e)^2*(1-cos(f*x+e))^2+1)/(csc(f*x+e)^2*(1-cos(f*x+e))^2-1))^(1/2)*(csc(f*x+e)^2*(1-cos
(f*x+e))^2-1)*(8*I*(b*((a^2+b^2)^(1/2)*a^2+2*(a^2+b^2)^(1/2)*b^2+2*a^2*b+2*b^3)/a^4)^(1/2)*(-b*((a^2+b^2)^(1/2
)*a^2+2*(a^2+b^2)^(1/2)*b^2-2*a^2*b-2*b^3)/a^4)^(1/2)*(csc(f*x+e)^2*(1-cos(f*x+e))^2+1)^(1/2)*(-csc(f*x+e)^2*(
1-cos(f*x+e))^2+1)^(1/2)*EllipticPi(I*(csc(f*x+e)-cot(f*x+e)),-1/(-b+(a^2+b^2)^(1/2))^2*a^2,I)*a*b*(csc(f*x+e)
-cot(f*x+e))+4*I*(b*((a^2+b^2)^(1/2)*a^2+2*(a^2+b^2)^(1/2)*b^2+2*a^2*b+2*b^3)/a^4)^(1/2)*(-b*((a^2+b^2)^(1/2)*
a^2+2*(a^2+b^2)^(1/2)*b^2-2*a^2*b-2*b^3)/a^4)^(1/2)*(csc(f*x+e)^2*(1-cos(f*x+e))^2+1)^(1/2)*(-csc(f*x+e)^2*(1-
cos(f*x+e))^2+1)^(1/2)*EllipticPi(I*(csc(f*x+e)-cot(f*x+e)),-1/(-b+(a^2+b^2)^(1/2))^2*a^2,I)*a^2-4*I*csc(f*x+e
)^2*(b*((a^2+b^2)^(1/2)*a^2+2*(a^2+b^2)^(1/2)*b^2+2*a^2*b+2*b^3)/a^4)^(1/2)*(-b*((a^2+b^2)^(1/2)*a^2+2*(a^2+b^
2)^(1/2)*b^2-2*a^2*b-2*b^3)/a^4)^(1/2)*(csc(f*x+e)^2*(1-cos(f*x+e))^2+1)^(1/2)*(-csc(f*x+e)^2*(1-cos(f*x+e))^2
+1)^(1/2)*EllipticPi(I*(csc(f*x+e)-cot(f*x+e)),-1/(-b+(a^2+b^2)^(1/2))^2*a^2,I)*a^2*(1-cos(f*x+e))^2-4*I*(b*((
a^2+b^2)^(1/2)*a^2+2*(a^2+b^2)^(1/2)*b^2+2*a^2*b+2*b^3)/a^4)^(1/2)*(-b*((a^2+b^2)^(1/2)*a^2+2*(a^2+b^2)^(1/2)*
b^2-2*a^2*b-2*b^3)/a^4)^(1/2)*(csc(f*x+e)^2*(1-cos(f*x+e))^2+1)^(1/2)*(-csc(f*x+e)^2*(1-cos(f*x+e))^2+1)^(1/2)
*EllipticPi(I*(csc(f*x+e)-cot(f*x+e)),-1/(b+(a^2+b^2)^(1/2))^2*a^2,I)*a^2-8*I*(b*((a^2+b^2)^(1/2)*a^2+2*(a^2+b
^2)^(1/2)*b^2+2*a^2*b+2*b^3)/a^4)^(1/2)*(-b*((a^2+b^2)^(1/2)*a^2+2*(a^2+b^2)^(1/2)*b^2-2*a^2*b-2*b^3)/a^4)^(1/
2)*(csc(f*x+e)^2*(1-cos(f*x+e))^2+1)^(1/2)*(-csc(f*x+e)^2*(1-cos(f*x+e))^2+1)^(1/2)*EllipticPi(I*(csc(f*x+e)-c
ot(f*x+e)),-1/(b+(a^2+b^2)^(1/2))^2*a^2,I)*a*b*(csc(f*x+e)-cot(f*x+e))+4*I*csc(f*x+e)^2*(b*((a^2+b^2)^(1/2)*a^
2+2*(a^2+b^2)^(1/2)*b^2+2*a^2*b+2*b^3)/a^4)^(1/2)*(-b*((a^2+b^2)^(1/2)*a^2+2*(a^2+b^2)^(1/2)*b^2-2*a^2*b-2*b^3
)/a^4)^(1/2)*(csc(f*x+e)^2*(1-cos(f*x+e))^2+1)^(1/2)*(-csc(f*x+e)^2*(1-cos(f*x+e))^2+1)^(1/2)*EllipticPi(I*(cs
c(f*x+e)-cot(f*x+e)),-1/(b+(a^2+b^2)^(1/2))^2*a^2,I)*a^2*(1-cos(f*x+e))^2+4*csc(f*x+e)^4*(a^2+b^2)^(1/2)*(b*((
a^2+b^2)^(1/2)*a^2+2*(a^2+b^2)^(1/2)*b^2+2*a^2*b+2*b^3)/a^4)^(1/2)*(-b*((a^2+b^2)^(1/2)*a^2+2*(a^2+b^2)^(1/2)*
b^2-2*a^2*b-2*b^3)/a^4)^(1/2)*a*(1-cos(f*x+e))^4+csc(f*x+e)^2*(a^2+b^2)^(1/2)*(csc(f*x+e)^4*(1-cos(f*x+e))^4-1
)^(1/2)*(b*((a^2+b^2)^(1/2)*a^2+2*(a^2+b^2)^(1/2)*b^2+2*a^2*b+2*b^3)/a^4)^(1/2)*arctanh(1/2*(2*csc(f*x+e)^2*(1
-cos(f*x+e))^2*b*(a^2+b^2)^(1/2)-csc(f*x+e)^2*a^2*(1-cos(f*x+e))^2-2*csc(f*x+e)^2*b^2*(1-cos(f*x+e))^2+a^2)/(-
b*((a^2+b^2)^(1/2)*a^2+2*(a^2+b^2)^(1/2)*b^2-2*a^2*b-2*b^3)/a^4)^(1/2)/(csc(f*x+e)^4*(1-cos(f*x+e))^4-1)^(1/2)
/a^2)*a*(1-cos(f*x+e))^2-csc(f*x+e)^2*(a^2+b^2)^(1/2)*(csc(f*x+e)^4*(1-cos(f*x+e))^4-1)^(1/2)*(-b*((a^2+b^2)^(
1/2)*a^2+2*(a^2+b^2)^(1/2)*b^2-2*a^2*b-2*b^3)/a^4)^(1/2)*arctanh(1/2*(2*csc(f*x+e)^2*(1-cos(f*x+e))^2*b*(a^2+b
^2)^(1/2)+csc(f*x+e)^2*a^2*(1-cos(f*x+e))^2+2*csc(f*x+e)^2*b^2*(1-cos(f*x+e))^2-a^2)/(b*((a^2+b^2)^(1/2)*a^2+2
*(a^2+b^2)^(1/2)*b^2+2*a^2*b+2*b^3)/a^4)^(1/2)/(csc(f*x+e)^4*(1-cos(f*x+e))^4-1)^(1/2)/a^2)*a*(1-cos(f*x+e))^2
-csc(f*x+e)^2*(csc(f*x+e)^4*(1-cos(f*x+e))^4-1)^(1/2)*(b*((a^2+b^2)^(1/2)*a^2+2*(a^2+b^2)^(1/2)*b^2+2*a^2*b+2*
b^3)/a^4)^(1/2)*arctanh(1/2*(2*csc(f*x+e)^2*(1-cos(f*x+e))^2*b*(a^2+b^2)^(1/2)-csc(f*x+e)^2*a^2*(1-cos(f*x+e))
^2-2*csc(f*x+e)^2*b^2*(1-cos(f*x+e))^2+a^2)/(-b*((a^2+b^2)^(1/2)*a^2+2*(a^2+b^2)^(1/2)*b^2-2*a^2*b-2*b^3)/a^4)
^(1/2)/(csc(f*x+e)^4*(1-cos(f*x+e))^4-1)^(1/2)/a^2)*a*b*(1-cos(f*x+e))^2-csc(f*x+e)^2*(csc(f*x+e)^4*(1-cos(f*x
+e))^4-1)^(1/2)*(-b*((a^2+b^2)^(1/2)*a^2+2*(a^2+b^2)^(1/2)*b^2-2*a^2*b-2*b^3)/a^4)^(1/2)*arctanh(1/2*(2*csc(f*
x+e)^2*(1-cos(f*x+e))^2*b*(a^2+b^2)^(1/2)+csc(f*x+e)^2*a^2*(1-cos(f*x+e))^2+2*csc(f*x+e)^2*b^2*(1-cos(f*x+e))^
2-a^2)/(b*((a^2+b^2)^(1/2)*a^2+2*(a^2+b^2)^(1/2)*b^2+2*a^2*b+2*b^3)/a^4)^(1/2)/(csc(f*x+e)^4*(1-cos(f*x+e))^4-
1)^(1/2)/a^2)*a*b*(1-cos(f*x+e))^2-2*(a^2+b^2)^(1/2)*(csc(f*x+e)^4*(1-cos(f*x+e))^4-1)^(1/2)*(b*((a^2+b^2)^(1/
2)*a^2+2*(a^2+b^2)^(1/2)*b^2+2*a^2*b+2*b^3)/a^4)^(1/2)*arctanh(1/2*(2*csc(f*x+e)^2*(1-cos(f*x+e))^2*b*(a^2+b^2
)^(1/2)-csc(f*x+e)^2*a^2*(1-cos(f*x+e))^2-2*csc(f*x+e)^2*b^2*(1-cos(f*x+e))^2+a^2)/(-b*((a^2+b^2)^(1/2)*a^2+2*
(a^2+b^2)^(1/2)*b^2-2*a^2*b-2*b^3)/a^4)^(1/2)/(csc(f*x+e)^4*(1-cos(f*x+e))^4-1)^(1/2)/a^2)*b*(csc(f*x+e)-cot(f
*x+e))+2*(a^2+b^2)^(1/2)*(csc(f*x+e)^4*(1-cos(f*x+e))^4-1)^(1/2)*(-b*((a^2+b^2)^(1/2)*a^2+2*(a^2+b^2)^(1/2)*b^
2-2*a^2*b-2*b^3)/a^4)^(1/2)*arctanh(1/2*(2*csc(f*x+e)^2*(1-cos(f*x+e))^2*b*(a^2+b^2)^(1/2)+csc(f*x+e)^2*a^2*(1
-cos(f*x+e))^2+2*csc(f*x+e)^2*b^2*(1-cos(f*x+e))^2-a^2)/(b*((a^2+b^2)^(1/2)*a^2+2*(a^2+b^2)^(1/2)*b^2+2*a^2*b+
2*b^3)/a^4)^(1/2)/(csc(f*x+e)^4*(1-cos(f*x+e))^4-1)^(1/2)/a^2)*b*(csc(f*x+e)-cot(f*x+e))+2*(csc(f*x+e)^4*(1-co
s(f*x+e))^4-1)^(1/2)*(b*((a^2+b^2)^(1/2)*a^2+2*(a^2+b^2)^(1/2)*b^2+2*a^2*b+2*b^3)/a^4)^(1/2)*arctanh(1/2*(2*cs
c(f*x+e)^2*(1-cos(f*x+e))^2*b*(a^2+b^2)^(1/2)-csc(f*x+e)^2*a^2*(1-cos(f*x+e))^2-2*csc(f*x+e)^2*b^2*(1-cos(f*x+
e))^2+a^2)/(-b*((a^2+b^2)^(1/2)*a^2+2*(a^2+b^2)^(1/2)*b^2-2*a^2*b-2*b^3)/a^4)^(1/2)/(csc(f*x+e)^4*(1-cos(f*x+e
))^4-1)^(1/2)/a^2)*b^2*(csc(f*x+e)-cot(f*x+e))+2*(csc(f*x+e)^4*(1-cos(f*x+e))^4-1)^(1/2)*(-b*((a^2+b^2)^(1/2)*
a^2+2*(a^2+b^2)^(1/2)*b^2-2*a^2*b-2*b^3)/a^4)^(1/2)*arctanh(1/2*(2*csc(f*x+e)^2*(1-cos(f*x+e))^2*b*(a^2+b^2)^(
1/2)+csc(f*x+e)^2*a^2*(1-cos(f*x+e))^2+2*csc(f*x+e)^2*b^2*(1-cos(f*x+e))^2-a^2)/(b*((a^2+b^2)^(1/2)*a^2+2*(a^2
+b^2)^(1/2)*b^2+2*a^2*b+2*b^3)/a^4)^(1/2)/(csc(f*x+e)^4*(1-cos(f*x+e))^4-1)^(1/2)/a^2)*b^2*(csc(f*x+e)-cot(f*x
+e))-(a^2+b^2)^(1/2)*(csc(f*x+e)^4*(1-cos(f*x+e))^4-1)^(1/2)*(b*((a^2+b^2)^(1/2)*a^2+2*(a^2+b^2)^(1/2)*b^2+2*a
^2*b+2*b^3)/a^4)^(1/2)*arctanh(1/2*(2*csc(f*x+e)^2*(1-cos(f*x+e))^2*b*(a^2+b^2)^(1/2)-csc(f*x+e)^2*a^2*(1-cos(
f*x+e))^2-2*csc(f*x+e)^2*b^2*(1-cos(f*x+e))^2+a^2)/(-b*((a^2+b^2)^(1/2)*a^2+2*(a^2+b^2)^(1/2)*b^2-2*a^2*b-2*b^
3)/a^4)^(1/2)/(csc(f*x+e)^4*(1-cos(f*x+e))^4-1)^(1/2)/a^2)*a+(a^2+b^2)^(1/2)*(csc(f*x+e)^4*(1-cos(f*x+e))^4-1)
^(1/2)*(-b*((a^2+b^2)^(1/2)*a^2+2*(a^2+b^2)^(1/2)*b^2-2*a^2*b-2*b^3)/a^4)^(1/2)*arctanh(1/2*(2*csc(f*x+e)^2*(1
-cos(f*x+e))^2*b*(a^2+b^2)^(1/2)+csc(f*x+e)^2*a^2*(1-cos(f*x+e))^2+2*csc(f*x+e)^2*b^2*(1-cos(f*x+e))^2-a^2)/(b
*((a^2+b^2)^(1/2)*a^2+2*(a^2+b^2)^(1/2)*b^2+2*a^2*b+2*b^3)/a^4)^(1/2)/(csc(f*x+e)^4*(1-cos(f*x+e))^4-1)^(1/2)/
a^2)*a+(csc(f*x+e)^4*(1-cos(f*x+e))^4-1)^(1/2)*(b*((a^2+b^2)^(1/2)*a^2+2*(a^2+b^2)^(1/2)*b^2+2*a^2*b+2*b^3)/a^
4)^(1/2)*arctanh(1/2*(2*csc(f*x+e)^2*(1-cos(f*x+e))^2*b*(a^2+b^2)^(1/2)-csc(f*x+e)^2*a^2*(1-cos(f*x+e))^2-2*cs
c(f*x+e)^2*b^2*(1-cos(f*x+e))^2+a^2)/(-b*((a^2+b^2)^(1/2)*a^2+2*(a^2+b^2)^(1/2)*b^2-2*a^2*b-2*b^3)/a^4)^(1/2)/
(csc(f*x+e)^4*(1-cos(f*x+e))^4-1)^(1/2)/a^2)*a*b+(csc(f*x+e)^4*(1-cos(f*x+e))^4-1)^(1/2)*(-b*((a^2+b^2)^(1/2)*
a^2+2*(a^2+b^2)^(1/2)*b^2-2*a^2*b-2*b^3)/a^4)^(1/2)*arctanh(1/2*(2*csc(f*x+e)^2*(1-cos(f*x+e))^2*b*(a^2+b^2)^(
1/2)+csc(f*x+e)^2*a^2*(1-cos(f*x+e))^2+2*csc(f*x+e)^2*b^2*(1-cos(f*x+e))^2-a^2)/(b*((a^2+b^2)^(1/2)*a^2+2*(a^2
+b^2)^(1/2)*b^2+2*a^2*b+2*b^3)/a^4)^(1/2)/(csc(f*x+e)^4*(1-cos(f*x+e))^4-1)^(1/2)/a^2)*a*b-4*(a^2+b^2)^(1/2)*(
b*((a^2+b^2)^(1/2)*a^2+2*(a^2+b^2)^(1/2)*b^2+2*a^2*b+2*b^3)/a^4)^(1/2)*(-b*((a^2+b^2)^(1/2)*a^2+2*(a^2+b^2)^(1
/2)*b^2-2*a^2*b-2*b^3)/a^4)^(1/2)*a)/(csc(f*x+e)^2*a*(1-cos(f*x+e))^2-2*b*(csc(f*x+e)-cot(f*x+e))-a)/(csc(f*x+
e)^4*(1-cos(f*x+e))^4-1)^(1/2)/((csc(f*x+e)^2*(1-cos(f*x+e))^2+1)*(csc(f*x+e)^2*(1-cos(f*x+e))^2-1))^(1/2)/a/b
/(-b*((a^2+b^2)^(1/2)*a^2+2*(a^2+b^2)^(1/2)*b^2-2*a^2*b-2*b^3)/a^4)^(1/2)/(b*((a^2+b^2)^(1/2)*a^2+2*(a^2+b^2)^
(1/2)*b^2+2*a^2*b+2*b^3)/a^4)^(1/2)/(a^2+b^2)^(1/2)
Fricas [F(-2)]
Exception generated. \[
\int \frac {(d \sec (e+f x))^{5/2}}{(a+b \tan (e+f x))^2} \, dx=\text {Exception raised: TypeError}
\]
[In]
integrate((d*sec(f*x+e))^(5/2)/(a+b*tan(f*x+e))^2,x, algorithm="fricas")
[Out]
Exception raised: TypeError >> Error detected within library code: catdef: division by zero
Sympy [F(-1)]
Timed out. \[
\int \frac {(d \sec (e+f x))^{5/2}}{(a+b \tan (e+f x))^2} \, dx=\text {Timed out}
\]
[In]
integrate((d*sec(f*x+e))**(5/2)/(a+b*tan(f*x+e))**2,x)
[Out]
Timed out
Maxima [F]
\[
\int \frac {(d \sec (e+f x))^{5/2}}{(a+b \tan (e+f x))^2} \, dx=\int { \frac {\left (d \sec \left (f x + e\right )\right )^{\frac {5}{2}}}{{\left (b \tan \left (f x + e\right ) + a\right )}^{2}} \,d x }
\]
[In]
integrate((d*sec(f*x+e))^(5/2)/(a+b*tan(f*x+e))^2,x, algorithm="maxima")
[Out]
integrate((d*sec(f*x + e))^(5/2)/(b*tan(f*x + e) + a)^2, x)
Giac [F]
\[
\int \frac {(d \sec (e+f x))^{5/2}}{(a+b \tan (e+f x))^2} \, dx=\int { \frac {\left (d \sec \left (f x + e\right )\right )^{\frac {5}{2}}}{{\left (b \tan \left (f x + e\right ) + a\right )}^{2}} \,d x }
\]
[In]
integrate((d*sec(f*x+e))^(5/2)/(a+b*tan(f*x+e))^2,x, algorithm="giac")
[Out]
integrate((d*sec(f*x + e))^(5/2)/(b*tan(f*x + e) + a)^2, x)
Mupad [F(-1)]
Timed out. \[
\int \frac {(d \sec (e+f x))^{5/2}}{(a+b \tan (e+f x))^2} \, dx=\int \frac {{\left (\frac {d}{\cos \left (e+f\,x\right )}\right )}^{5/2}}{{\left (a+b\,\mathrm {tan}\left (e+f\,x\right )\right )}^2} \,d x
\]
[In]
int((d/cos(e + f*x))^(5/2)/(a + b*tan(e + f*x))^2,x)
[Out]
int((d/cos(e + f*x))^(5/2)/(a + b*tan(e + f*x))^2, x)