Integrand size = 20, antiderivative size = 279 \[ \int (e x)^m \left (a+b \sin \left (c+d x^2\right )\right )^2 \, dx=\frac {\left (2 a^2+b^2\right ) (e x)^{1+m}}{2 e (1+m)}+\frac {i a b e^{i c} (e x)^{1+m} \left (-i d x^2\right )^{\frac {1}{2} (-1-m)} \Gamma \left (\frac {1+m}{2},-i d x^2\right )}{2 e}-\frac {i a b e^{-i c} (e x)^{1+m} \left (i d x^2\right )^{\frac {1}{2} (-1-m)} \Gamma \left (\frac {1+m}{2},i d x^2\right )}{2 e}+\frac {2^{-\frac {7}{2}-\frac {m}{2}} b^2 e^{2 i c} (e x)^{1+m} \left (-i d x^2\right )^{\frac {1}{2} (-1-m)} \Gamma \left (\frac {1+m}{2},-2 i d x^2\right )}{e}+\frac {2^{-\frac {7}{2}-\frac {m}{2}} b^2 e^{-2 i c} (e x)^{1+m} \left (i d x^2\right )^{\frac {1}{2} (-1-m)} \Gamma \left (\frac {1+m}{2},2 i d x^2\right )}{e} \]
1/2*(2*a^2+b^2)*(e*x)^(1+m)/e/(1+m)+1/2*I*a*b*exp(I*c)*(e*x)^(1+m)*(-I*d*x ^2)^(-1/2-1/2*m)*GAMMA(1/2+1/2*m,-I*d*x^2)/e-1/2*I*a*b*(e*x)^(1+m)*(I*d*x^ 2)^(-1/2-1/2*m)*GAMMA(1/2+1/2*m,I*d*x^2)/e/exp(I*c)+2^(-7/2-1/2*m)*b^2*exp (2*I*c)*(e*x)^(1+m)*(-I*d*x^2)^(-1/2-1/2*m)*GAMMA(1/2+1/2*m,-2*I*d*x^2)/e+ 2^(-7/2-1/2*m)*b^2*(e*x)^(1+m)*(I*d*x^2)^(-1/2-1/2*m)*GAMMA(1/2+1/2*m,2*I* d*x^2)/e/exp(2*I*c)
Time = 1.90 (sec) , antiderivative size = 551, normalized size of antiderivative = 1.97 \[ \int (e x)^m \left (a+b \sin \left (c+d x^2\right )\right )^2 \, dx=\frac {2^{\frac {1}{2} (-7-m)} x (e x)^m \left (d^2 x^4\right )^{\frac {1}{2} (-1-m)} \left (2^{\frac {7+m}{2}} a^2 \left (d^2 x^4\right )^{\frac {1+m}{2}}+2^{\frac {5+m}{2}} b^2 \left (d^2 x^4\right )^{\frac {1+m}{2}}+b^2 \left (i d x^2\right )^{\frac {1+m}{2}} \cos (2 c) \Gamma \left (\frac {1+m}{2},-2 i d x^2\right )+b^2 m \left (i d x^2\right )^{\frac {1+m}{2}} \cos (2 c) \Gamma \left (\frac {1+m}{2},-2 i d x^2\right )+b^2 \left (-i d x^2\right )^{\frac {1+m}{2}} \cos (2 c) \Gamma \left (\frac {1+m}{2},2 i d x^2\right )+b^2 m \left (-i d x^2\right )^{\frac {1+m}{2}} \cos (2 c) \Gamma \left (\frac {1+m}{2},2 i d x^2\right )-i 2^{\frac {5+m}{2}} a b (1+m) \left (-i d x^2\right )^{\frac {1+m}{2}} \Gamma \left (\frac {1+m}{2},i d x^2\right ) (\cos (c)-i \sin (c))+i 2^{\frac {5+m}{2}} a b (1+m) \left (i d x^2\right )^{\frac {1+m}{2}} \Gamma \left (\frac {1+m}{2},-i d x^2\right ) (\cos (c)+i \sin (c))+i b^2 \left (i d x^2\right )^{\frac {1+m}{2}} \Gamma \left (\frac {1+m}{2},-2 i d x^2\right ) \sin (2 c)+i b^2 m \left (i d x^2\right )^{\frac {1+m}{2}} \Gamma \left (\frac {1+m}{2},-2 i d x^2\right ) \sin (2 c)-i b^2 \left (-i d x^2\right )^{\frac {1+m}{2}} \Gamma \left (\frac {1+m}{2},2 i d x^2\right ) \sin (2 c)-i b^2 m \left (-i d x^2\right )^{\frac {1+m}{2}} \Gamma \left (\frac {1+m}{2},2 i d x^2\right ) \sin (2 c)\right )}{1+m} \]
(2^((-7 - m)/2)*x*(e*x)^m*(d^2*x^4)^((-1 - m)/2)*(2^((7 + m)/2)*a^2*(d^2*x ^4)^((1 + m)/2) + 2^((5 + m)/2)*b^2*(d^2*x^4)^((1 + m)/2) + b^2*(I*d*x^2)^ ((1 + m)/2)*Cos[2*c]*Gamma[(1 + m)/2, (-2*I)*d*x^2] + b^2*m*(I*d*x^2)^((1 + m)/2)*Cos[2*c]*Gamma[(1 + m)/2, (-2*I)*d*x^2] + b^2*((-I)*d*x^2)^((1 + m )/2)*Cos[2*c]*Gamma[(1 + m)/2, (2*I)*d*x^2] + b^2*m*((-I)*d*x^2)^((1 + m)/ 2)*Cos[2*c]*Gamma[(1 + m)/2, (2*I)*d*x^2] - I*2^((5 + m)/2)*a*b*(1 + m)*(( -I)*d*x^2)^((1 + m)/2)*Gamma[(1 + m)/2, I*d*x^2]*(Cos[c] - I*Sin[c]) + I*2 ^((5 + m)/2)*a*b*(1 + m)*(I*d*x^2)^((1 + m)/2)*Gamma[(1 + m)/2, (-I)*d*x^2 ]*(Cos[c] + I*Sin[c]) + I*b^2*(I*d*x^2)^((1 + m)/2)*Gamma[(1 + m)/2, (-2*I )*d*x^2]*Sin[2*c] + I*b^2*m*(I*d*x^2)^((1 + m)/2)*Gamma[(1 + m)/2, (-2*I)* d*x^2]*Sin[2*c] - I*b^2*((-I)*d*x^2)^((1 + m)/2)*Gamma[(1 + m)/2, (2*I)*d* x^2]*Sin[2*c] - I*b^2*m*((-I)*d*x^2)^((1 + m)/2)*Gamma[(1 + m)/2, (2*I)*d* x^2]*Sin[2*c]))/(1 + m)
Time = 0.46 (sec) , antiderivative size = 279, normalized size of antiderivative = 1.00, number of steps used = 3, number of rules used = 3, \(\frac {\text {number of rules}}{\text {integrand size}}\) = 0.150, Rules used = {3884, 6, 2009}
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.
\(\displaystyle \int (e x)^m \left (a+b \sin \left (c+d x^2\right )\right )^2 \, dx\) |
\(\Big \downarrow \) 3884 |
\(\displaystyle \int \left (a^2 (e x)^m+2 a b (e x)^m \sin \left (c+d x^2\right )-\frac {1}{2} b^2 (e x)^m \cos \left (2 c+2 d x^2\right )+\frac {1}{2} b^2 (e x)^m\right )dx\) |
\(\Big \downarrow \) 6 |
\(\displaystyle \int \left (\left (a^2+\frac {b^2}{2}\right ) (e x)^m+2 a b (e x)^m \sin \left (c+d x^2\right )-\frac {1}{2} b^2 (e x)^m \cos \left (2 c+2 d x^2\right )\right )dx\) |
\(\Big \downarrow \) 2009 |
\(\displaystyle \frac {\left (2 a^2+b^2\right ) (e x)^{m+1}}{2 e (m+1)}+\frac {i a b e^{i c} \left (-i d x^2\right )^{\frac {1}{2} (-m-1)} (e x)^{m+1} \Gamma \left (\frac {m+1}{2},-i d x^2\right )}{2 e}-\frac {i a b e^{-i c} \left (i d x^2\right )^{\frac {1}{2} (-m-1)} (e x)^{m+1} \Gamma \left (\frac {m+1}{2},i d x^2\right )}{2 e}+\frac {b^2 e^{2 i c} 2^{-\frac {m}{2}-\frac {7}{2}} \left (-i d x^2\right )^{\frac {1}{2} (-m-1)} (e x)^{m+1} \Gamma \left (\frac {m+1}{2},-2 i d x^2\right )}{e}+\frac {b^2 e^{-2 i c} 2^{-\frac {m}{2}-\frac {7}{2}} \left (i d x^2\right )^{\frac {1}{2} (-m-1)} (e x)^{m+1} \Gamma \left (\frac {m+1}{2},2 i d x^2\right )}{e}\) |
((2*a^2 + b^2)*(e*x)^(1 + m))/(2*e*(1 + m)) + ((I/2)*a*b*E^(I*c)*(e*x)^(1 + m)*((-I)*d*x^2)^((-1 - m)/2)*Gamma[(1 + m)/2, (-I)*d*x^2])/e - ((I/2)*a* b*(e*x)^(1 + m)*(I*d*x^2)^((-1 - m)/2)*Gamma[(1 + m)/2, I*d*x^2])/(e*E^(I* c)) + (2^(-7/2 - m/2)*b^2*E^((2*I)*c)*(e*x)^(1 + m)*((-I)*d*x^2)^((-1 - m) /2)*Gamma[(1 + m)/2, (-2*I)*d*x^2])/e + (2^(-7/2 - m/2)*b^2*(e*x)^(1 + m)* (I*d*x^2)^((-1 - m)/2)*Gamma[(1 + m)/2, (2*I)*d*x^2])/(e*E^((2*I)*c))
3.1.53.3.1 Defintions of rubi rules used
Int[(u_.)*((v_.) + (a_.)*(Fx_) + (b_.)*(Fx_))^(p_.), x_Symbol] :> Int[u*(v + (a + b)*Fx)^p, x] /; FreeQ[{a, b}, x] && !FreeQ[Fx, x]
Int[((e_.)*(x_))^(m_.)*((a_.) + (b_.)*Sin[(c_.) + (d_.)*(x_)^(n_)])^(p_), x _Symbol] :> Int[ExpandTrigReduce[(e*x)^m, (a + b*Sin[c + d*x^n])^p, x], x] /; FreeQ[{a, b, c, d, e, m}, x] && IGtQ[p, 1] && IGtQ[n, 0]
\[\int \left (e x \right )^{m} {\left (a +b \sin \left (d \,x^{2}+c \right )\right )}^{2}d x\]
Time = 0.11 (sec) , antiderivative size = 198, normalized size of antiderivative = 0.71 \[ \int (e x)^m \left (a+b \sin \left (c+d x^2\right )\right )^2 \, dx=\frac {8 \, {\left (2 \, a^{2} + b^{2}\right )} \left (e x\right )^{m} d x + {\left (-i \, b^{2} e m - i \, b^{2} e\right )} e^{\left (-\frac {1}{2} \, {\left (m - 1\right )} \log \left (\frac {2 i \, d}{e^{2}}\right ) - 2 i \, c\right )} \Gamma \left (\frac {1}{2} \, m + \frac {1}{2}, 2 i \, d x^{2}\right ) - 8 \, {\left (a b e m + a b e\right )} e^{\left (-\frac {1}{2} \, {\left (m - 1\right )} \log \left (\frac {i \, d}{e^{2}}\right ) - i \, c\right )} \Gamma \left (\frac {1}{2} \, m + \frac {1}{2}, i \, d x^{2}\right ) - 8 \, {\left (a b e m + a b e\right )} e^{\left (-\frac {1}{2} \, {\left (m - 1\right )} \log \left (-\frac {i \, d}{e^{2}}\right ) + i \, c\right )} \Gamma \left (\frac {1}{2} \, m + \frac {1}{2}, -i \, d x^{2}\right ) + {\left (i \, b^{2} e m + i \, b^{2} e\right )} e^{\left (-\frac {1}{2} \, {\left (m - 1\right )} \log \left (-\frac {2 i \, d}{e^{2}}\right ) + 2 i \, c\right )} \Gamma \left (\frac {1}{2} \, m + \frac {1}{2}, -2 i \, d x^{2}\right )}{16 \, {\left (d m + d\right )}} \]
1/16*(8*(2*a^2 + b^2)*(e*x)^m*d*x + (-I*b^2*e*m - I*b^2*e)*e^(-1/2*(m - 1) *log(2*I*d/e^2) - 2*I*c)*gamma(1/2*m + 1/2, 2*I*d*x^2) - 8*(a*b*e*m + a*b* e)*e^(-1/2*(m - 1)*log(I*d/e^2) - I*c)*gamma(1/2*m + 1/2, I*d*x^2) - 8*(a* b*e*m + a*b*e)*e^(-1/2*(m - 1)*log(-I*d/e^2) + I*c)*gamma(1/2*m + 1/2, -I* d*x^2) + (I*b^2*e*m + I*b^2*e)*e^(-1/2*(m - 1)*log(-2*I*d/e^2) + 2*I*c)*ga mma(1/2*m + 1/2, -2*I*d*x^2))/(d*m + d)
\[ \int (e x)^m \left (a+b \sin \left (c+d x^2\right )\right )^2 \, dx=\int \left (e x\right )^{m} \left (a + b \sin {\left (c + d x^{2} \right )}\right )^{2}\, dx \]
\[ \int (e x)^m \left (a+b \sin \left (c+d x^2\right )\right )^2 \, dx=\int { {\left (b \sin \left (d x^{2} + c\right ) + a\right )}^{2} \left (e x\right )^{m} \,d x } \]
(e*x)^(m + 1)*a^2/(e*(m + 1)) + 1/2*(b^2*e^m*x*x^m - (b^2*e^m*m + b^2*e^m) *integrate(x^m*cos(2*d*x^2 + 2*c), x) + 4*(a*b*e^m*m + a*b*e^m)*integrate( x^m*sin(d*x^2 + c), x))/(m + 1)
\[ \int (e x)^m \left (a+b \sin \left (c+d x^2\right )\right )^2 \, dx=\int { {\left (b \sin \left (d x^{2} + c\right ) + a\right )}^{2} \left (e x\right )^{m} \,d x } \]
Timed out. \[ \int (e x)^m \left (a+b \sin \left (c+d x^2\right )\right )^2 \, dx=\int {\left (e\,x\right )}^m\,{\left (a+b\,\sin \left (d\,x^2+c\right )\right )}^2 \,d x \]