Integrand size = 25, antiderivative size = 127 \[ \int (d \csc (e+f x))^m \left (a+b \tan ^2(e+f x)\right )^p \, dx=\frac {\operatorname {AppellF1}\left (\frac {1-m}{2},1-\frac {m}{2},-p,\frac {3-m}{2},-\tan ^2(e+f x),-\frac {b \tan ^2(e+f x)}{a}\right ) (d \csc (e+f x))^m \sec ^2(e+f x)^{-m/2} \tan (e+f x) \left (a+b \tan ^2(e+f x)\right )^p \left (1+\frac {b \tan ^2(e+f x)}{a}\right )^{-p}}{f (1-m)} \]
AppellF1(-1/2*m+1/2,1-1/2*m,-p,3/2-1/2*m,-tan(f*x+e)^2,-b*tan(f*x+e)^2/a)* (d*csc(f*x+e))^m*tan(f*x+e)*(a+b*tan(f*x+e)^2)^p/f/(1-m)/((sec(f*x+e)^2)^( 1/2*m))/((1+b*tan(f*x+e)^2/a)^p)
Leaf count is larger than twice the leaf count of optimal. \(292\) vs. \(2(127)=254\).
Time = 5.38 (sec) , antiderivative size = 292, normalized size of antiderivative = 2.30 \[ \int (d \csc (e+f x))^m \left (a+b \tan ^2(e+f x)\right )^p \, dx=-\frac {a (-3+m) \operatorname {AppellF1}\left (\frac {1}{2}-\frac {m}{2},1-\frac {m}{2},-p,\frac {3}{2}-\frac {m}{2},-\tan ^2(e+f x),-\frac {b \tan ^2(e+f x)}{a}\right ) \cos ^2(e+f x) \cot (e+f x) (d \csc (e+f x))^m \left (a+b \tan ^2(e+f x)\right )^p}{f (-1+m) \left (-2 b p \operatorname {AppellF1}\left (\frac {3}{2}-\frac {m}{2},1-\frac {m}{2},1-p,\frac {5}{2}-\frac {m}{2},-\tan ^2(e+f x),-\frac {b \tan ^2(e+f x)}{a}\right )-a (-2+m) \operatorname {AppellF1}\left (\frac {3}{2}-\frac {m}{2},2-\frac {m}{2},-p,\frac {5}{2}-\frac {m}{2},-\tan ^2(e+f x),-\frac {b \tan ^2(e+f x)}{a}\right )+a (-3+m) \operatorname {AppellF1}\left (\frac {1}{2}-\frac {m}{2},1-\frac {m}{2},-p,\frac {3}{2}-\frac {m}{2},-\tan ^2(e+f x),-\frac {b \tan ^2(e+f x)}{a}\right ) \cot ^2(e+f x)\right )} \]
-((a*(-3 + m)*AppellF1[1/2 - m/2, 1 - m/2, -p, 3/2 - m/2, -Tan[e + f*x]^2, -((b*Tan[e + f*x]^2)/a)]*Cos[e + f*x]^2*Cot[e + f*x]*(d*Csc[e + f*x])^m*( a + b*Tan[e + f*x]^2)^p)/(f*(-1 + m)*(-2*b*p*AppellF1[3/2 - m/2, 1 - m/2, 1 - p, 5/2 - m/2, -Tan[e + f*x]^2, -((b*Tan[e + f*x]^2)/a)] - a*(-2 + m)*A ppellF1[3/2 - m/2, 2 - m/2, -p, 5/2 - m/2, -Tan[e + f*x]^2, -((b*Tan[e + f *x]^2)/a)] + a*(-3 + m)*AppellF1[1/2 - m/2, 1 - m/2, -p, 3/2 - m/2, -Tan[e + f*x]^2, -((b*Tan[e + f*x]^2)/a)]*Cot[e + f*x]^2)))
Time = 0.48 (sec) , antiderivative size = 155, normalized size of antiderivative = 1.22, number of steps used = 8, number of rules used = 7, \(\frac {\text {number of rules}}{\text {integrand size}}\) = 0.280, Rules used = {3042, 4164, 3042, 4150, 393, 152, 150}
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.
\(\displaystyle \int (d \csc (e+f x))^m \left (a+b \tan ^2(e+f x)\right )^p \, dx\) |
\(\Big \downarrow \) 3042 |
\(\displaystyle \int (d \csc (e+f x))^m \left (a+b \tan (e+f x)^2\right )^pdx\) |
\(\Big \downarrow \) 4164 |
\(\displaystyle \left (\frac {\sin (e+f x)}{d}\right )^m (d \csc (e+f x))^m \int \left (\frac {\sin (e+f x)}{d}\right )^{-m} \left (b \tan ^2(e+f x)+a\right )^pdx\) |
\(\Big \downarrow \) 3042 |
\(\displaystyle \left (\frac {\sin (e+f x)}{d}\right )^m (d \csc (e+f x))^m \int \left (\frac {\sin (e+f x)}{d}\right )^{-m} \left (b \tan (e+f x)^2+a\right )^pdx\) |
\(\Big \downarrow \) 4150 |
\(\displaystyle \frac {\tan ^m(e+f x) \sec ^2(e+f x)^{-m/2} (d \csc (e+f x))^m \int \tan ^{-m}(e+f x) \left (\tan ^2(e+f x)+1\right )^{\frac {m-2}{2}} \left (b \tan ^2(e+f x)+a\right )^pd\tan (e+f x)}{f}\) |
\(\Big \downarrow \) 393 |
\(\displaystyle \frac {\cot (e+f x) \tan ^2(e+f x)^{\frac {m+1}{2}} \sec ^2(e+f x)^{-m/2} (d \csc (e+f x))^m \int \tan ^2(e+f x)^{\frac {1}{2} (-m-1)} \left (\tan ^2(e+f x)+1\right )^{\frac {m-2}{2}} \left (b \tan ^2(e+f x)+a\right )^pd\tan ^2(e+f x)}{2 f}\) |
\(\Big \downarrow \) 152 |
\(\displaystyle \frac {\cot (e+f x) \tan ^2(e+f x)^{\frac {m+1}{2}} \sec ^2(e+f x)^{-m/2} (d \csc (e+f x))^m \left (a+b \tan ^2(e+f x)\right )^p \left (\frac {b \tan ^2(e+f x)}{a}+1\right )^{-p} \int \tan ^2(e+f x)^{\frac {1}{2} (-m-1)} \left (\tan ^2(e+f x)+1\right )^{\frac {m-2}{2}} \left (\frac {b \tan ^2(e+f x)}{a}+1\right )^pd\tan ^2(e+f x)}{2 f}\) |
\(\Big \downarrow \) 150 |
\(\displaystyle \frac {\cot (e+f x) \tan ^2(e+f x)^{\frac {1-m}{2}+\frac {m+1}{2}} \sec ^2(e+f x)^{-m/2} (d \csc (e+f x))^m \left (a+b \tan ^2(e+f x)\right )^p \left (\frac {b \tan ^2(e+f x)}{a}+1\right )^{-p} \operatorname {AppellF1}\left (\frac {1-m}{2},\frac {2-m}{2},-p,\frac {3-m}{2},-\tan ^2(e+f x),-\frac {b \tan ^2(e+f x)}{a}\right )}{f (1-m)}\) |
(AppellF1[(1 - m)/2, (2 - m)/2, -p, (3 - m)/2, -Tan[e + f*x]^2, -((b*Tan[e + f*x]^2)/a)]*Cot[e + f*x]*(d*Csc[e + f*x])^m*(Tan[e + f*x]^2)^((1 - m)/2 + (1 + m)/2)*(a + b*Tan[e + f*x]^2)^p)/(f*(1 - m)*(Sec[e + f*x]^2)^(m/2)* (1 + (b*Tan[e + f*x]^2)/a)^p)
3.5.97.3.1 Defintions of rubi rules used
Int[((b_.)*(x_))^(m_)*((c_) + (d_.)*(x_))^(n_)*((e_) + (f_.)*(x_))^(p_), x_ ] :> Simp[c^n*e^p*((b*x)^(m + 1)/(b*(m + 1)))*AppellF1[m + 1, -n, -p, m + 2 , (-d)*(x/c), (-f)*(x/e)], x] /; FreeQ[{b, c, d, e, f, m, n, p}, x] && !In tegerQ[m] && !IntegerQ[n] && GtQ[c, 0] && (IntegerQ[p] || GtQ[e, 0])
Int[((b_.)*(x_))^(m_)*((c_) + (d_.)*(x_))^(n_)*((e_) + (f_.)*(x_))^(p_), x_ ] :> Simp[c^IntPart[n]*((c + d*x)^FracPart[n]/(1 + d*(x/c))^FracPart[n]) Int[(b*x)^m*(1 + d*(x/c))^n*(e + f*x)^p, x], x] /; FreeQ[{b, c, d, e, f, m, n, p}, x] && !IntegerQ[m] && !IntegerQ[n] && !GtQ[c, 0]
Int[((e_.)*(x_))^(m_.)*((a_) + (b_.)*(x_)^2)^(p_.)*((c_) + (d_.)*(x_)^2)^(q _.), x_Symbol] :> Simp[(e*x)^m/(2*x*(x^2)^(Simplify[(m + 1)/2] - 1)) Subs t[Int[x^(Simplify[(m + 1)/2] - 1)*(a + b*x)^p*(c + d*x)^q, x], x, x^2], x] /; FreeQ[{a, b, c, d, e, m, p, q}, x] && NeQ[b*c - a*d, 0] && IntegerQ[Simp lify[m + 2*p]] && !IntegerQ[m]
Int[((d_.)*sin[(e_.) + (f_.)*(x_)])^(m_)*((a_) + (b_.)*tan[(e_.) + (f_.)*(x _)]^2)^(p_), x_Symbol] :> With[{ff = FreeFactors[Tan[e + f*x], x]}, Simp[ff *(d*Sin[e + f*x])^m*((Sec[e + f*x]^2)^(m/2)/(f*Tan[e + f*x]^m)) Subst[Int [(ff*x)^m*((a + b*ff^2*x^2)^p/(1 + ff^2*x^2)^(m/2 + 1)), x], x, Tan[e + f*x ]/ff], x]] /; FreeQ[{a, b, d, e, f, m, p}, x] && !IntegerQ[m]
Int[(csc[(e_.) + (f_.)*(x_)]*(d_.))^(m_)*((a_) + (b_.)*((c_.)*tan[(e_.) + ( f_.)*(x_)])^(n_))^(p_), x_Symbol] :> Simp[(d*Csc[e + f*x])^FracPart[m]*(Sin [e + f*x]/d)^FracPart[m] Int[(a + b*(c*Tan[e + f*x])^n)^p/(Sin[e + f*x]/d )^m, x], x] /; FreeQ[{a, b, c, d, e, f, m, n, p}, x] && !IntegerQ[m]
\[\int \left (d \csc \left (f x +e \right )\right )^{m} \left (a +b \tan \left (f x +e \right )^{2}\right )^{p}d x\]
\[ \int (d \csc (e+f x))^m \left (a+b \tan ^2(e+f x)\right )^p \, dx=\int { {\left (b \tan \left (f x + e\right )^{2} + a\right )}^{p} \left (d \csc \left (f x + e\right )\right )^{m} \,d x } \]
Timed out. \[ \int (d \csc (e+f x))^m \left (a+b \tan ^2(e+f x)\right )^p \, dx=\text {Timed out} \]
\[ \int (d \csc (e+f x))^m \left (a+b \tan ^2(e+f x)\right )^p \, dx=\int { {\left (b \tan \left (f x + e\right )^{2} + a\right )}^{p} \left (d \csc \left (f x + e\right )\right )^{m} \,d x } \]
\[ \int (d \csc (e+f x))^m \left (a+b \tan ^2(e+f x)\right )^p \, dx=\int { {\left (b \tan \left (f x + e\right )^{2} + a\right )}^{p} \left (d \csc \left (f x + e\right )\right )^{m} \,d x } \]
Timed out. \[ \int (d \csc (e+f x))^m \left (a+b \tan ^2(e+f x)\right )^p \, dx=\int {\left (b\,{\mathrm {tan}\left (e+f\,x\right )}^2+a\right )}^p\,{\left (\frac {d}{\sin \left (e+f\,x\right )}\right )}^m \,d x \]