Integrand size = 18, antiderivative size = 245 \[ \int \frac {x^3}{a+b \sin \left (c+d x^2\right )} \, dx=-\frac {i x^2 \log \left (1-\frac {i b e^{i \left (c+d x^2\right )}}{a-\sqrt {a^2-b^2}}\right )}{2 \sqrt {a^2-b^2} d}+\frac {i x^2 \log \left (1-\frac {i b e^{i \left (c+d x^2\right )}}{a+\sqrt {a^2-b^2}}\right )}{2 \sqrt {a^2-b^2} d}-\frac {\operatorname {PolyLog}\left (2,\frac {i b e^{i \left (c+d x^2\right )}}{a-\sqrt {a^2-b^2}}\right )}{2 \sqrt {a^2-b^2} d^2}+\frac {\operatorname {PolyLog}\left (2,\frac {i b e^{i \left (c+d x^2\right )}}{a+\sqrt {a^2-b^2}}\right )}{2 \sqrt {a^2-b^2} d^2} \]
-1/2*I*x^2*ln(1-I*b*exp(I*(d*x^2+c))/(a-(a^2-b^2)^(1/2)))/d/(a^2-b^2)^(1/2 )+1/2*I*x^2*ln(1-I*b*exp(I*(d*x^2+c))/(a+(a^2-b^2)^(1/2)))/d/(a^2-b^2)^(1/ 2)-1/2*polylog(2,I*b*exp(I*(d*x^2+c))/(a-(a^2-b^2)^(1/2)))/d^2/(a^2-b^2)^( 1/2)+1/2*polylog(2,I*b*exp(I*(d*x^2+c))/(a+(a^2-b^2)^(1/2)))/d^2/(a^2-b^2) ^(1/2)
Time = 0.05 (sec) , antiderivative size = 188, normalized size of antiderivative = 0.77 \[ \int \frac {x^3}{a+b \sin \left (c+d x^2\right )} \, dx=\frac {-i d x^2 \left (\log \left (1+\frac {i b e^{i \left (c+d x^2\right )}}{-a+\sqrt {a^2-b^2}}\right )-\log \left (1-\frac {i b e^{i \left (c+d x^2\right )}}{a+\sqrt {a^2-b^2}}\right )\right )-\operatorname {PolyLog}\left (2,-\frac {i b e^{i \left (c+d x^2\right )}}{-a+\sqrt {a^2-b^2}}\right )+\operatorname {PolyLog}\left (2,\frac {i b e^{i \left (c+d x^2\right )}}{a+\sqrt {a^2-b^2}}\right )}{2 \sqrt {a^2-b^2} d^2} \]
((-I)*d*x^2*(Log[1 + (I*b*E^(I*(c + d*x^2)))/(-a + Sqrt[a^2 - b^2])] - Log [1 - (I*b*E^(I*(c + d*x^2)))/(a + Sqrt[a^2 - b^2])]) - PolyLog[2, ((-I)*b* E^(I*(c + d*x^2)))/(-a + Sqrt[a^2 - b^2])] + PolyLog[2, (I*b*E^(I*(c + d*x ^2)))/(a + Sqrt[a^2 - b^2])])/(2*Sqrt[a^2 - b^2]*d^2)
Time = 0.87 (sec) , antiderivative size = 237, normalized size of antiderivative = 0.97, number of steps used = 9, number of rules used = 8, \(\frac {\text {number of rules}}{\text {integrand size}}\) = 0.444, Rules used = {3860, 3042, 3804, 2694, 27, 2620, 2715, 2838}
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.
\(\displaystyle \int \frac {x^3}{a+b \sin \left (c+d x^2\right )} \, dx\) |
\(\Big \downarrow \) 3860 |
\(\displaystyle \frac {1}{2} \int \frac {x^2}{a+b \sin \left (d x^2+c\right )}dx^2\) |
\(\Big \downarrow \) 3042 |
\(\displaystyle \frac {1}{2} \int \frac {x^2}{a+b \sin \left (d x^2+c\right )}dx^2\) |
\(\Big \downarrow \) 3804 |
\(\displaystyle \int \frac {x^2 e^{i \left (c+d x^2\right )}}{2 a e^{i \left (c+d x^2\right )}-i b e^{2 i \left (c+d x^2\right )}+i b}dx^2\) |
\(\Big \downarrow \) 2694 |
\(\displaystyle \frac {i b \int \frac {e^{i \left (d x^2+c\right )} x^2}{2 \left (a-i b e^{i \left (d x^2+c\right )}+\sqrt {a^2-b^2}\right )}dx^2}{\sqrt {a^2-b^2}}-\frac {i b \int \frac {e^{i \left (d x^2+c\right )} x^2}{2 \left (a-i b e^{i \left (d x^2+c\right )}-\sqrt {a^2-b^2}\right )}dx^2}{\sqrt {a^2-b^2}}\) |
\(\Big \downarrow \) 27 |
\(\displaystyle \frac {i b \int \frac {e^{i \left (d x^2+c\right )} x^2}{a-i b e^{i \left (d x^2+c\right )}+\sqrt {a^2-b^2}}dx^2}{2 \sqrt {a^2-b^2}}-\frac {i b \int \frac {e^{i \left (d x^2+c\right )} x^2}{a-i b e^{i \left (d x^2+c\right )}-\sqrt {a^2-b^2}}dx^2}{2 \sqrt {a^2-b^2}}\) |
\(\Big \downarrow \) 2620 |
\(\displaystyle \frac {i b \left (\frac {x^2 \log \left (1-\frac {i b e^{i \left (c+d x^2\right )}}{\sqrt {a^2-b^2}+a}\right )}{b d}-\frac {\int \log \left (1-\frac {i b e^{i \left (d x^2+c\right )}}{a+\sqrt {a^2-b^2}}\right )dx^2}{b d}\right )}{2 \sqrt {a^2-b^2}}-\frac {i b \left (\frac {x^2 \log \left (1-\frac {i b e^{i \left (c+d x^2\right )}}{a-\sqrt {a^2-b^2}}\right )}{b d}-\frac {\int \log \left (1-\frac {i b e^{i \left (d x^2+c\right )}}{a-\sqrt {a^2-b^2}}\right )dx^2}{b d}\right )}{2 \sqrt {a^2-b^2}}\) |
\(\Big \downarrow \) 2715 |
\(\displaystyle \frac {i b \left (\frac {i \int \frac {\log \left (1-\frac {i b e^{i \left (d x^2+c\right )}}{a+\sqrt {a^2-b^2}}\right )}{x^2}de^{i \left (d x^2+c\right )}}{b d^2}+\frac {x^2 \log \left (1-\frac {i b e^{i \left (c+d x^2\right )}}{\sqrt {a^2-b^2}+a}\right )}{b d}\right )}{2 \sqrt {a^2-b^2}}-\frac {i b \left (\frac {i \int \frac {\log \left (1-\frac {i b e^{i \left (d x^2+c\right )}}{a-\sqrt {a^2-b^2}}\right )}{x^2}de^{i \left (d x^2+c\right )}}{b d^2}+\frac {x^2 \log \left (1-\frac {i b e^{i \left (c+d x^2\right )}}{a-\sqrt {a^2-b^2}}\right )}{b d}\right )}{2 \sqrt {a^2-b^2}}\) |
\(\Big \downarrow \) 2838 |
\(\displaystyle \frac {i b \left (\frac {x^2 \log \left (1-\frac {i b e^{i \left (c+d x^2\right )}}{\sqrt {a^2-b^2}+a}\right )}{b d}-\frac {i \operatorname {PolyLog}\left (2,\frac {i b e^{i \left (d x^2+c\right )}}{a+\sqrt {a^2-b^2}}\right )}{b d^2}\right )}{2 \sqrt {a^2-b^2}}-\frac {i b \left (\frac {x^2 \log \left (1-\frac {i b e^{i \left (c+d x^2\right )}}{a-\sqrt {a^2-b^2}}\right )}{b d}-\frac {i \operatorname {PolyLog}\left (2,\frac {i b e^{i \left (d x^2+c\right )}}{a-\sqrt {a^2-b^2}}\right )}{b d^2}\right )}{2 \sqrt {a^2-b^2}}\) |
((-1/2*I)*b*((x^2*Log[1 - (I*b*E^(I*(c + d*x^2)))/(a - Sqrt[a^2 - b^2])])/ (b*d) - (I*PolyLog[2, (I*b*E^(I*(c + d*x^2)))/(a - Sqrt[a^2 - b^2])])/(b*d ^2)))/Sqrt[a^2 - b^2] + ((I/2)*b*((x^2*Log[1 - (I*b*E^(I*(c + d*x^2)))/(a + Sqrt[a^2 - b^2])])/(b*d) - (I*PolyLog[2, (I*b*E^(I*(c + d*x^2)))/(a + Sq rt[a^2 - b^2])])/(b*d^2)))/Sqrt[a^2 - b^2]
3.1.36.3.1 Defintions of rubi rules used
Int[(a_)*(Fx_), x_Symbol] :> Simp[a Int[Fx, x], x] /; FreeQ[a, x] && !Ma tchQ[Fx, (b_)*(Gx_) /; FreeQ[b, x]]
Int[(((F_)^((g_.)*((e_.) + (f_.)*(x_))))^(n_.)*((c_.) + (d_.)*(x_))^(m_.))/ ((a_) + (b_.)*((F_)^((g_.)*((e_.) + (f_.)*(x_))))^(n_.)), x_Symbol] :> Simp [((c + d*x)^m/(b*f*g*n*Log[F]))*Log[1 + b*((F^(g*(e + f*x)))^n/a)], x] - Si mp[d*(m/(b*f*g*n*Log[F])) Int[(c + d*x)^(m - 1)*Log[1 + b*((F^(g*(e + f*x )))^n/a)], x], x] /; FreeQ[{F, a, b, c, d, e, f, g, n}, x] && IGtQ[m, 0]
Int[((F_)^(u_)*((f_.) + (g_.)*(x_))^(m_.))/((a_.) + (b_.)*(F_)^(u_) + (c_.) *(F_)^(v_)), x_Symbol] :> With[{q = Rt[b^2 - 4*a*c, 2]}, Simp[2*(c/q) Int [(f + g*x)^m*(F^u/(b - q + 2*c*F^u)), x], x] - Simp[2*(c/q) Int[(f + g*x) ^m*(F^u/(b + q + 2*c*F^u)), x], x]] /; FreeQ[{F, a, b, c, f, g}, x] && EqQ[ v, 2*u] && LinearQ[u, x] && NeQ[b^2 - 4*a*c, 0] && IGtQ[m, 0]
Int[Log[(a_) + (b_.)*((F_)^((e_.)*((c_.) + (d_.)*(x_))))^(n_.)], x_Symbol] :> Simp[1/(d*e*n*Log[F]) Subst[Int[Log[a + b*x]/x, x], x, (F^(e*(c + d*x) ))^n], x] /; FreeQ[{F, a, b, c, d, e, n}, x] && GtQ[a, 0]
Int[Log[(c_.)*((d_) + (e_.)*(x_)^(n_.))]/(x_), x_Symbol] :> Simp[-PolyLog[2 , (-c)*e*x^n]/n, x] /; FreeQ[{c, d, e, n}, x] && EqQ[c*d, 1]
Int[((c_.) + (d_.)*(x_))^(m_.)/((a_) + (b_.)*sin[(e_.) + (f_.)*(x_)]), x_Sy mbol] :> Simp[2 Int[(c + d*x)^m*(E^(I*(e + f*x))/(I*b + 2*a*E^(I*(e + f*x )) - I*b*E^(2*I*(e + f*x)))), x], x] /; FreeQ[{a, b, c, d, e, f}, x] && NeQ [a^2 - b^2, 0] && IGtQ[m, 0]
Int[(x_)^(m_.)*((a_.) + (b_.)*Sin[(c_.) + (d_.)*(x_)^(n_)])^(p_.), x_Symbol ] :> Simp[1/n Subst[Int[x^(Simplify[(m + 1)/n] - 1)*(a + b*Sin[c + d*x])^ p, x], x, x^n], x] /; FreeQ[{a, b, c, d, m, n, p}, x] && IntegerQ[Simplify[ (m + 1)/n]] && (EqQ[p, 1] || EqQ[m, n - 1] || (IntegerQ[p] && GtQ[Simplify[ (m + 1)/n], 0]))
\[\int \frac {x^{3}}{a +b \sin \left (d \,x^{2}+c \right )}d x\]
Both result and optimal contain complex but leaf count of result is larger than twice the leaf count of optimal. 1041 vs. \(2 (199) = 398\).
Time = 0.42 (sec) , antiderivative size = 1041, normalized size of antiderivative = 4.25 \[ \int \frac {x^3}{a+b \sin \left (c+d x^2\right )} \, dx=\text {Too large to display} \]
-1/4*(b*c*sqrt(-(a^2 - b^2)/b^2)*log(2*b*cos(d*x^2 + c) + 2*I*b*sin(d*x^2 + c) + 2*b*sqrt(-(a^2 - b^2)/b^2) + 2*I*a) + b*c*sqrt(-(a^2 - b^2)/b^2)*lo g(2*b*cos(d*x^2 + c) - 2*I*b*sin(d*x^2 + c) + 2*b*sqrt(-(a^2 - b^2)/b^2) - 2*I*a) - b*c*sqrt(-(a^2 - b^2)/b^2)*log(-2*b*cos(d*x^2 + c) + 2*I*b*sin(d *x^2 + c) + 2*b*sqrt(-(a^2 - b^2)/b^2) + 2*I*a) - b*c*sqrt(-(a^2 - b^2)/b^ 2)*log(-2*b*cos(d*x^2 + c) - 2*I*b*sin(d*x^2 + c) + 2*b*sqrt(-(a^2 - b^2)/ b^2) - 2*I*a) - I*b*sqrt(-(a^2 - b^2)/b^2)*dilog((I*a*cos(d*x^2 + c) - a*s in(d*x^2 + c) + (b*cos(d*x^2 + c) + I*b*sin(d*x^2 + c))*sqrt(-(a^2 - b^2)/ b^2) - b)/b + 1) + I*b*sqrt(-(a^2 - b^2)/b^2)*dilog((I*a*cos(d*x^2 + c) - a*sin(d*x^2 + c) - (b*cos(d*x^2 + c) + I*b*sin(d*x^2 + c))*sqrt(-(a^2 - b^ 2)/b^2) - b)/b + 1) + I*b*sqrt(-(a^2 - b^2)/b^2)*dilog((-I*a*cos(d*x^2 + c ) - a*sin(d*x^2 + c) + (b*cos(d*x^2 + c) - I*b*sin(d*x^2 + c))*sqrt(-(a^2 - b^2)/b^2) - b)/b + 1) - I*b*sqrt(-(a^2 - b^2)/b^2)*dilog((-I*a*cos(d*x^2 + c) - a*sin(d*x^2 + c) - (b*cos(d*x^2 + c) - I*b*sin(d*x^2 + c))*sqrt(-( a^2 - b^2)/b^2) - b)/b + 1) + (b*d*x^2 + b*c)*sqrt(-(a^2 - b^2)/b^2)*log(- (I*a*cos(d*x^2 + c) - a*sin(d*x^2 + c) + (b*cos(d*x^2 + c) + I*b*sin(d*x^2 + c))*sqrt(-(a^2 - b^2)/b^2) - b)/b) - (b*d*x^2 + b*c)*sqrt(-(a^2 - b^2)/ b^2)*log(-(I*a*cos(d*x^2 + c) - a*sin(d*x^2 + c) - (b*cos(d*x^2 + c) + I*b *sin(d*x^2 + c))*sqrt(-(a^2 - b^2)/b^2) - b)/b) + (b*d*x^2 + b*c)*sqrt(-(a ^2 - b^2)/b^2)*log(-(-I*a*cos(d*x^2 + c) - a*sin(d*x^2 + c) + (b*cos(d*...
\[ \int \frac {x^3}{a+b \sin \left (c+d x^2\right )} \, dx=\int \frac {x^{3}}{a + b \sin {\left (c + d x^{2} \right )}}\, dx \]
\[ \int \frac {x^3}{a+b \sin \left (c+d x^2\right )} \, dx=\int { \frac {x^{3}}{b \sin \left (d x^{2} + c\right ) + a} \,d x } \]
\[ \int \frac {x^3}{a+b \sin \left (c+d x^2\right )} \, dx=\int { \frac {x^{3}}{b \sin \left (d x^{2} + c\right ) + a} \,d x } \]
Timed out. \[ \int \frac {x^3}{a+b \sin \left (c+d x^2\right )} \, dx=\int \frac {x^3}{a+b\,\sin \left (d\,x^2+c\right )} \,d x \]