Integrand size = 23, antiderivative size = 140 \[ \int \sin ^3(e+f x) \left (a+b \tan ^2(e+f x)\right )^p \, dx=\frac {\cos ^3(e+f x) \left (a-b+b \sec ^2(e+f x)\right )^{1+p}}{3 (a-b) f}-\frac {(3 a-2 b (1+p)) \cos (e+f x) \operatorname {Hypergeometric2F1}\left (-\frac {1}{2},-p,\frac {1}{2},-\frac {b \sec ^2(e+f x)}{a-b}\right ) \left (a-b+b \sec ^2(e+f x)\right )^p \left (1+\frac {b \sec ^2(e+f x)}{a-b}\right )^{-p}}{3 (a-b) f} \]
1/3*cos(f*x+e)^3*(a-b+b*sec(f*x+e)^2)^(p+1)/(a-b)/f-1/3*(3*a-2*b*(p+1))*co s(f*x+e)*hypergeom([-1/2, -p],[1/2],-b*sec(f*x+e)^2/(a-b))*(a-b+b*sec(f*x+ e)^2)^p/(a-b)/f/((1+b*sec(f*x+e)^2/(a-b))^p)
Time = 4.84 (sec) , antiderivative size = 184, normalized size of antiderivative = 1.31 \[ \int \sin ^3(e+f x) \left (a+b \tan ^2(e+f x)\right )^p \, dx=\frac {\sin (e+f x) \tan (e+f x) \left (a+b \tan ^2(e+f x)\right )^p \left ((-3 a+2 b (1+p)) \operatorname {Hypergeometric2F1}\left (-\frac {1}{2},-p,\frac {1}{2},-\frac {b \sec ^2(e+f x)}{a-b}\right )+\left (a \cos ^2(e+f x)+b \sin ^2(e+f x)\right ) \left (\frac {a+b \tan ^2(e+f x)}{a-b}\right )^p\right )}{f \left (3 a \sec ^2(e+f x) \left (\frac {a-b+b \sec ^2(e+f x)}{a-b}\right )^p-3 (a-b) \left (\frac {a+b \tan ^2(e+f x)}{a-b}\right )^{1+p}\right )} \]
(Sin[e + f*x]*Tan[e + f*x]*(a + b*Tan[e + f*x]^2)^p*((-3*a + 2*b*(1 + p))* Hypergeometric2F1[-1/2, -p, 1/2, -((b*Sec[e + f*x]^2)/(a - b))] + (a*Cos[e + f*x]^2 + b*Sin[e + f*x]^2)*((a + b*Tan[e + f*x]^2)/(a - b))^p))/(f*(3*a *Sec[e + f*x]^2*((a - b + b*Sec[e + f*x]^2)/(a - b))^p - 3*(a - b)*((a + b *Tan[e + f*x]^2)/(a - b))^(1 + p)))
Time = 0.30 (sec) , antiderivative size = 138, normalized size of antiderivative = 0.99, number of steps used = 7, number of rules used = 6, \(\frac {\text {number of rules}}{\text {integrand size}}\) = 0.261, Rules used = {3042, 4147, 25, 359, 279, 278}
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.
\(\displaystyle \int \sin ^3(e+f x) \left (a+b \tan ^2(e+f x)\right )^p \, dx\) |
\(\Big \downarrow \) 3042 |
\(\displaystyle \int \sin (e+f x)^3 \left (a+b \tan (e+f x)^2\right )^pdx\) |
\(\Big \downarrow \) 4147 |
\(\displaystyle \frac {\int -\cos ^4(e+f x) \left (1-\sec ^2(e+f x)\right ) \left (b \sec ^2(e+f x)+a-b\right )^pd\sec (e+f x)}{f}\) |
\(\Big \downarrow \) 25 |
\(\displaystyle -\frac {\int \cos ^4(e+f x) \left (1-\sec ^2(e+f x)\right ) \left (b \sec ^2(e+f x)+a-b\right )^pd\sec (e+f x)}{f}\) |
\(\Big \downarrow \) 359 |
\(\displaystyle \frac {\frac {(3 a-2 b (p+1)) \int \cos ^2(e+f x) \left (b \sec ^2(e+f x)+a-b\right )^pd\sec (e+f x)}{3 (a-b)}+\frac {\cos ^3(e+f x) \left (a+b \sec ^2(e+f x)-b\right )^{p+1}}{3 (a-b)}}{f}\) |
\(\Big \downarrow \) 279 |
\(\displaystyle \frac {\frac {(3 a-2 b (p+1)) \left (a+b \sec ^2(e+f x)-b\right )^p \left (\frac {b \sec ^2(e+f x)}{a-b}+1\right )^{-p} \int \cos ^2(e+f x) \left (\frac {b \sec ^2(e+f x)}{a-b}+1\right )^pd\sec (e+f x)}{3 (a-b)}+\frac {\cos ^3(e+f x) \left (a+b \sec ^2(e+f x)-b\right )^{p+1}}{3 (a-b)}}{f}\) |
\(\Big \downarrow \) 278 |
\(\displaystyle \frac {\frac {\cos ^3(e+f x) \left (a+b \sec ^2(e+f x)-b\right )^{p+1}}{3 (a-b)}-\frac {(3 a-2 b (p+1)) \cos (e+f x) \left (a+b \sec ^2(e+f x)-b\right )^p \left (\frac {b \sec ^2(e+f x)}{a-b}+1\right )^{-p} \operatorname {Hypergeometric2F1}\left (-\frac {1}{2},-p,\frac {1}{2},-\frac {b \sec ^2(e+f x)}{a-b}\right )}{3 (a-b)}}{f}\) |
((Cos[e + f*x]^3*(a - b + b*Sec[e + f*x]^2)^(1 + p))/(3*(a - b)) - ((3*a - 2*b*(1 + p))*Cos[e + f*x]*Hypergeometric2F1[-1/2, -p, 1/2, -((b*Sec[e + f *x]^2)/(a - b))]*(a - b + b*Sec[e + f*x]^2)^p)/(3*(a - b)*(1 + (b*Sec[e + f*x]^2)/(a - b))^p))/f
3.2.55.3.1 Defintions of rubi rules used
Int[((c_.)*(x_))^(m_.)*((a_) + (b_.)*(x_)^2)^(p_), x_Symbol] :> Simp[a^p*(( c*x)^(m + 1)/(c*(m + 1)))*Hypergeometric2F1[-p, (m + 1)/2, (m + 1)/2 + 1, ( -b)*(x^2/a)], x] /; FreeQ[{a, b, c, m, p}, x] && !IGtQ[p, 0] && (ILtQ[p, 0 ] || GtQ[a, 0])
Int[((c_.)*(x_))^(m_.)*((a_) + (b_.)*(x_)^2)^(p_), x_Symbol] :> Simp[a^IntP art[p]*((a + b*x^2)^FracPart[p]/(1 + b*(x^2/a))^FracPart[p]) Int[(c*x)^m* (1 + b*(x^2/a))^p, x], x] /; FreeQ[{a, b, c, m, p}, x] && !IGtQ[p, 0] && !(ILtQ[p, 0] || GtQ[a, 0])
Int[((e_.)*(x_))^(m_.)*((a_) + (b_.)*(x_)^2)^(p_.)*((c_) + (d_.)*(x_)^2), x _Symbol] :> Simp[c*(e*x)^(m + 1)*((a + b*x^2)^(p + 1)/(a*e*(m + 1))), x] + Simp[(a*d*(m + 1) - b*c*(m + 2*p + 3))/(a*e^2*(m + 1)) Int[(e*x)^(m + 2)* (a + b*x^2)^p, x], x] /; FreeQ[{a, b, c, d, e, p}, x] && NeQ[b*c - a*d, 0] && LtQ[m, -1] && !ILtQ[p, -1]
Int[sin[(e_.) + (f_.)*(x_)]^(m_.)*((a_) + (b_.)*tan[(e_.) + (f_.)*(x_)]^2)^ (p_.), x_Symbol] :> With[{ff = FreeFactors[Sec[e + f*x], x]}, Simp[1/(f*ff^ m) Subst[Int[(-1 + ff^2*x^2)^((m - 1)/2)*((a - b + b*ff^2*x^2)^p/x^(m + 1 )), x], x, Sec[e + f*x]/ff], x]] /; FreeQ[{a, b, e, f, p}, x] && IntegerQ[( m - 1)/2]
\[\int \sin \left (f x +e \right )^{3} \left (a +b \tan \left (f x +e \right )^{2}\right )^{p}d x\]
\[ \int \sin ^3(e+f x) \left (a+b \tan ^2(e+f x)\right )^p \, dx=\int { {\left (b \tan \left (f x + e\right )^{2} + a\right )}^{p} \sin \left (f x + e\right )^{3} \,d x } \]
Timed out. \[ \int \sin ^3(e+f x) \left (a+b \tan ^2(e+f x)\right )^p \, dx=\text {Timed out} \]
\[ \int \sin ^3(e+f x) \left (a+b \tan ^2(e+f x)\right )^p \, dx=\int { {\left (b \tan \left (f x + e\right )^{2} + a\right )}^{p} \sin \left (f x + e\right )^{3} \,d x } \]
\[ \int \sin ^3(e+f x) \left (a+b \tan ^2(e+f x)\right )^p \, dx=\int { {\left (b \tan \left (f x + e\right )^{2} + a\right )}^{p} \sin \left (f x + e\right )^{3} \,d x } \]
Timed out. \[ \int \sin ^3(e+f x) \left (a+b \tan ^2(e+f x)\right )^p \, dx=\int {\sin \left (e+f\,x\right )}^3\,{\left (b\,{\mathrm {tan}\left (e+f\,x\right )}^2+a\right )}^p \,d x \]