Integrand size = 12, antiderivative size = 225 \[ \int \frac {x}{a+b \cos (x) \sin (x)} \, dx=-\frac {i x \log \left (1-\frac {i b e^{2 i x}}{2 a-\sqrt {4 a^2-b^2}}\right )}{\sqrt {4 a^2-b^2}}+\frac {i x \log \left (1-\frac {i b e^{2 i x}}{2 a+\sqrt {4 a^2-b^2}}\right )}{\sqrt {4 a^2-b^2}}-\frac {\operatorname {PolyLog}\left (2,\frac {i b e^{2 i x}}{2 a-\sqrt {4 a^2-b^2}}\right )}{2 \sqrt {4 a^2-b^2}}+\frac {\operatorname {PolyLog}\left (2,\frac {i b e^{2 i x}}{2 a+\sqrt {4 a^2-b^2}}\right )}{2 \sqrt {4 a^2-b^2}} \]
-I*x*ln(1-I*b*exp(2*I*x)/(2*a-(4*a^2-b^2)^(1/2)))/(4*a^2-b^2)^(1/2)+I*x*ln (1-I*b*exp(2*I*x)/(2*a+(4*a^2-b^2)^(1/2)))/(4*a^2-b^2)^(1/2)-1/2*polylog(2 ,I*b*exp(2*I*x)/(2*a-(4*a^2-b^2)^(1/2)))/(4*a^2-b^2)^(1/2)+1/2*polylog(2,I *b*exp(2*I*x)/(2*a+(4*a^2-b^2)^(1/2)))/(4*a^2-b^2)^(1/2)
Both result and optimal contain complex but leaf count is larger than twice the leaf count of optimal. \(788\) vs. \(2(225)=450\).
Time = 1.25 (sec) , antiderivative size = 788, normalized size of antiderivative = 3.50 \[ \int \frac {x}{a+b \cos (x) \sin (x)} \, dx=\frac {1}{2} \left (\frac {\pi \arctan \left (\frac {b+2 a \tan (x)}{\sqrt {4 a^2-b^2}}\right )}{\sqrt {4 a^2-b^2}}+\frac {2 \arccos \left (-\frac {2 a}{b}\right ) \text {arctanh}\left (\frac {(2 a-b) \cot \left (\frac {\pi }{4}+x\right )}{\sqrt {-4 a^2+b^2}}\right )+(\pi -4 x) \text {arctanh}\left (\frac {(2 a+b) \tan \left (\frac {\pi }{4}+x\right )}{\sqrt {-4 a^2+b^2}}\right )-\left (\arccos \left (-\frac {2 a}{b}\right )+2 i \text {arctanh}\left (\frac {(2 a-b) \cot \left (\frac {\pi }{4}+x\right )}{\sqrt {-4 a^2+b^2}}\right )\right ) \log \left (\frac {(2 a+b) \left (-2 a+b-i \sqrt {-4 a^2+b^2}\right ) \left (1+i \cot \left (\frac {\pi }{4}+x\right )\right )}{b \left (2 a+b+\sqrt {-4 a^2+b^2} \cot \left (\frac {\pi }{4}+x\right )\right )}\right )-\left (\arccos \left (-\frac {2 a}{b}\right )-2 i \text {arctanh}\left (\frac {(2 a-b) \cot \left (\frac {\pi }{4}+x\right )}{\sqrt {-4 a^2+b^2}}\right )\right ) \log \left (\frac {(2 a+b) \left (2 i a-i b+\sqrt {-4 a^2+b^2}\right ) \left (i+\cot \left (\frac {\pi }{4}+x\right )\right )}{b \left (2 a+b+\sqrt {-4 a^2+b^2} \cot \left (\frac {\pi }{4}+x\right )\right )}\right )+\left (\arccos \left (-\frac {2 a}{b}\right )+2 i \left (\text {arctanh}\left (\frac {(2 a-b) \cot \left (\frac {\pi }{4}+x\right )}{\sqrt {-4 a^2+b^2}}\right )+\text {arctanh}\left (\frac {(2 a+b) \tan \left (\frac {\pi }{4}+x\right )}{\sqrt {-4 a^2+b^2}}\right )\right )\right ) \log \left (\frac {\sqrt [4]{-1} \sqrt {-4 a^2+b^2} e^{-i x}}{2 \sqrt {b} \sqrt {a+b \cos (x) \sin (x)}}\right )+\left (\arccos \left (-\frac {2 a}{b}\right )-2 i \text {arctanh}\left (\frac {(2 a-b) \cot \left (\frac {\pi }{4}+x\right )}{\sqrt {-4 a^2+b^2}}\right )-2 i \text {arctanh}\left (\frac {(2 a+b) \tan \left (\frac {\pi }{4}+x\right )}{\sqrt {-4 a^2+b^2}}\right )\right ) \log \left (-\frac {(-1)^{3/4} \sqrt {-4 a^2+b^2} e^{i x}}{2 \sqrt {b} \sqrt {a+b \cos (x) \sin (x)}}\right )+i \left (\operatorname {PolyLog}\left (2,\frac {\left (2 a-i \sqrt {-4 a^2+b^2}\right ) \left (2 a+b-\sqrt {-4 a^2+b^2} \cot \left (\frac {\pi }{4}+x\right )\right )}{b \left (2 a+b+\sqrt {-4 a^2+b^2} \cot \left (\frac {\pi }{4}+x\right )\right )}\right )-\operatorname {PolyLog}\left (2,\frac {\left (2 a+i \sqrt {-4 a^2+b^2}\right ) \left (2 a+b-\sqrt {-4 a^2+b^2} \cot \left (\frac {\pi }{4}+x\right )\right )}{b \left (2 a+b+\sqrt {-4 a^2+b^2} \cot \left (\frac {\pi }{4}+x\right )\right )}\right )\right )}{\sqrt {-4 a^2+b^2}}\right ) \]
((Pi*ArcTan[(b + 2*a*Tan[x])/Sqrt[4*a^2 - b^2]])/Sqrt[4*a^2 - b^2] + (2*Ar cCos[(-2*a)/b]*ArcTanh[((2*a - b)*Cot[Pi/4 + x])/Sqrt[-4*a^2 + b^2]] + (Pi - 4*x)*ArcTanh[((2*a + b)*Tan[Pi/4 + x])/Sqrt[-4*a^2 + b^2]] - (ArcCos[(- 2*a)/b] + (2*I)*ArcTanh[((2*a - b)*Cot[Pi/4 + x])/Sqrt[-4*a^2 + b^2]])*Log [((2*a + b)*(-2*a + b - I*Sqrt[-4*a^2 + b^2])*(1 + I*Cot[Pi/4 + x]))/(b*(2 *a + b + Sqrt[-4*a^2 + b^2]*Cot[Pi/4 + x]))] - (ArcCos[(-2*a)/b] - (2*I)*A rcTanh[((2*a - b)*Cot[Pi/4 + x])/Sqrt[-4*a^2 + b^2]])*Log[((2*a + b)*((2*I )*a - I*b + Sqrt[-4*a^2 + b^2])*(I + Cot[Pi/4 + x]))/(b*(2*a + b + Sqrt[-4 *a^2 + b^2]*Cot[Pi/4 + x]))] + (ArcCos[(-2*a)/b] + (2*I)*(ArcTanh[((2*a - b)*Cot[Pi/4 + x])/Sqrt[-4*a^2 + b^2]] + ArcTanh[((2*a + b)*Tan[Pi/4 + x])/ Sqrt[-4*a^2 + b^2]]))*Log[((-1)^(1/4)*Sqrt[-4*a^2 + b^2])/(2*Sqrt[b]*E^(I* x)*Sqrt[a + b*Cos[x]*Sin[x]])] + (ArcCos[(-2*a)/b] - (2*I)*ArcTanh[((2*a - b)*Cot[Pi/4 + x])/Sqrt[-4*a^2 + b^2]] - (2*I)*ArcTanh[((2*a + b)*Tan[Pi/4 + x])/Sqrt[-4*a^2 + b^2]])*Log[-1/2*((-1)^(3/4)*Sqrt[-4*a^2 + b^2]*E^(I*x ))/(Sqrt[b]*Sqrt[a + b*Cos[x]*Sin[x]])] + I*(PolyLog[2, ((2*a - I*Sqrt[-4* a^2 + b^2])*(2*a + b - Sqrt[-4*a^2 + b^2]*Cot[Pi/4 + x]))/(b*(2*a + b + Sq rt[-4*a^2 + b^2]*Cot[Pi/4 + x]))] - PolyLog[2, ((2*a + I*Sqrt[-4*a^2 + b^2 ])*(2*a + b - Sqrt[-4*a^2 + b^2]*Cot[Pi/4 + x]))/(b*(2*a + b + Sqrt[-4*a^2 + b^2]*Cot[Pi/4 + x]))]))/Sqrt[-4*a^2 + b^2])/2
Time = 0.70 (sec) , antiderivative size = 229, normalized size of antiderivative = 1.02, number of steps used = 10, number of rules used = 9, \(\frac {\text {number of rules}}{\text {integrand size}}\) = 0.750, Rules used = {5095, 3042, 3804, 27, 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.
\(\displaystyle \int \frac {x}{a+b \sin (x) \cos (x)} \, dx\) |
\(\Big \downarrow \) 5095 |
\(\displaystyle \int \frac {x}{a+\frac {1}{2} b \sin (2 x)}dx\) |
\(\Big \downarrow \) 3042 |
\(\displaystyle \int \frac {x}{a+\frac {1}{2} b \sin (2 x)}dx\) |
\(\Big \downarrow \) 3804 |
\(\displaystyle 2 \int \frac {2 e^{2 i x} x}{4 e^{2 i x} a-i b e^{4 i x}+i b}dx\) |
\(\Big \downarrow \) 27 |
\(\displaystyle 4 \int \frac {e^{2 i x} x}{4 e^{2 i x} a-i b e^{4 i x}+i b}dx\) |
\(\Big \downarrow \) 2694 |
\(\displaystyle 4 \left (\frac {i b \int \frac {e^{2 i x} x}{2 \left (2 a-i b e^{2 i x}+\sqrt {4 a^2-b^2}\right )}dx}{\sqrt {4 a^2-b^2}}-\frac {i b \int \frac {e^{2 i x} x}{2 \left (2 a-i b e^{2 i x}-\sqrt {4 a^2-b^2}\right )}dx}{\sqrt {4 a^2-b^2}}\right )\) |
\(\Big \downarrow \) 27 |
\(\displaystyle 4 \left (\frac {i b \int \frac {e^{2 i x} x}{2 a-i b e^{2 i x}+\sqrt {4 a^2-b^2}}dx}{2 \sqrt {4 a^2-b^2}}-\frac {i b \int \frac {e^{2 i x} x}{2 a-i b e^{2 i x}-\sqrt {4 a^2-b^2}}dx}{2 \sqrt {4 a^2-b^2}}\right )\) |
\(\Big \downarrow \) 2620 |
\(\displaystyle 4 \left (\frac {i b \left (\frac {x \log \left (1-\frac {i b e^{2 i x}}{\sqrt {4 a^2-b^2}+2 a}\right )}{2 b}-\frac {\int \log \left (1-\frac {i b e^{2 i x}}{2 a+\sqrt {4 a^2-b^2}}\right )dx}{2 b}\right )}{2 \sqrt {4 a^2-b^2}}-\frac {i b \left (\frac {x \log \left (1-\frac {i b e^{2 i x}}{2 a-\sqrt {4 a^2-b^2}}\right )}{2 b}-\frac {\int \log \left (1-\frac {i b e^{2 i x}}{2 a-\sqrt {4 a^2-b^2}}\right )dx}{2 b}\right )}{2 \sqrt {4 a^2-b^2}}\right )\) |
\(\Big \downarrow \) 2715 |
\(\displaystyle 4 \left (\frac {i b \left (\frac {i \int e^{-2 i x} \log \left (1-\frac {i b e^{2 i x}}{2 a+\sqrt {4 a^2-b^2}}\right )de^{2 i x}}{4 b}+\frac {x \log \left (1-\frac {i b e^{2 i x}}{\sqrt {4 a^2-b^2}+2 a}\right )}{2 b}\right )}{2 \sqrt {4 a^2-b^2}}-\frac {i b \left (\frac {i \int e^{-2 i x} \log \left (1-\frac {i b e^{2 i x}}{2 a-\sqrt {4 a^2-b^2}}\right )de^{2 i x}}{4 b}+\frac {x \log \left (1-\frac {i b e^{2 i x}}{2 a-\sqrt {4 a^2-b^2}}\right )}{2 b}\right )}{2 \sqrt {4 a^2-b^2}}\right )\) |
\(\Big \downarrow \) 2838 |
\(\displaystyle 4 \left (\frac {i b \left (\frac {x \log \left (1-\frac {i b e^{2 i x}}{\sqrt {4 a^2-b^2}+2 a}\right )}{2 b}-\frac {i \operatorname {PolyLog}\left (2,\frac {i b e^{2 i x}}{2 a+\sqrt {4 a^2-b^2}}\right )}{4 b}\right )}{2 \sqrt {4 a^2-b^2}}-\frac {i b \left (\frac {x \log \left (1-\frac {i b e^{2 i x}}{2 a-\sqrt {4 a^2-b^2}}\right )}{2 b}-\frac {i \operatorname {PolyLog}\left (2,\frac {i b e^{2 i x}}{2 a-\sqrt {4 a^2-b^2}}\right )}{4 b}\right )}{2 \sqrt {4 a^2-b^2}}\right )\) |
4*(((-1/2*I)*b*((x*Log[1 - (I*b*E^((2*I)*x))/(2*a - Sqrt[4*a^2 - b^2])])/( 2*b) - ((I/4)*PolyLog[2, (I*b*E^((2*I)*x))/(2*a - Sqrt[4*a^2 - b^2])])/b)) /Sqrt[4*a^2 - b^2] + ((I/2)*b*((x*Log[1 - (I*b*E^((2*I)*x))/(2*a + Sqrt[4* a^2 - b^2])])/(2*b) - ((I/4)*PolyLog[2, (I*b*E^((2*I)*x))/(2*a + Sqrt[4*a^ 2 - b^2])])/b))/Sqrt[4*a^2 - b^2])
3.6.81.3.1 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[((e_.) + (f_.)*(x_))^(m_.)*((a_) + Cos[(c_.) + (d_.)*(x_)]*(b_.)*Sin[(c _.) + (d_.)*(x_)])^(n_.), x_Symbol] :> Int[(e + f*x)^m*(a + b*(Sin[2*c + 2* d*x]/2))^n, x] /; FreeQ[{a, b, c, d, e, f, m, n}, x]
Both result and optimal contain complex but leaf count of result is larger than twice the leaf count of optimal. 1283 vs. \(2 (191 ) = 382\).
Time = 0.91 (sec) , antiderivative size = 1284, normalized size of antiderivative = 5.71
4*I/(8*a^2-2*b^2)/(-2*I*a+(-(2*a-b)*(2*a+b))^(1/2))*ln(1-b*exp(2*I*x)/(-2* I*a+(-(2*a-b)*(2*a+b))^(1/2)))*(-(2*a-b)*(2*a+b))^(1/2)*a*x+4/(8*a^2-2*b^2 )/(-2*I*a+(-(2*a-b)*(2*a+b))^(1/2))*(-(2*a-b)*(2*a+b))^(1/2)*a*x^2-2/(8*a^ 2-2*b^2)/(-2*I*a+(-(2*a-b)*(2*a+b))^(1/2))*ln(1-b*exp(2*I*x)/(-2*I*a+(-(2* a-b)*(2*a+b))^(1/2)))*b^2*x+2/(8*a^2-2*b^2)/(-2*I*a+(-(2*a-b)*(2*a+b))^(1/ 2))*polylog(2,b*exp(2*I*x)/(-2*I*a+(-(2*a-b)*(2*a+b))^(1/2)))*(-(2*a-b)*(2 *a+b))^(1/2)*a+8/(8*a^2-2*b^2)/(-2*I*a-(-(2*a-b)*(2*a+b))^(1/2))*ln(1-b*ex p(2*I*x)/(-2*I*a-(-(2*a-b)*(2*a+b))^(1/2)))*a^2*x-4*I/(8*a^2-2*b^2)/(-2*I* a+(-(2*a-b)*(2*a+b))^(1/2))*polylog(2,b*exp(2*I*x)/(-2*I*a+(-(2*a-b)*(2*a+ b))^(1/2)))*a^2+I/(8*a^2-2*b^2)/(-2*I*a+(-(2*a-b)*(2*a+b))^(1/2))*polylog( 2,b*exp(2*I*x)/(-2*I*a+(-(2*a-b)*(2*a+b))^(1/2)))*b^2+2*I/(8*a^2-2*b^2)/(- 2*I*a+(-(2*a-b)*(2*a+b))^(1/2))*x^2*b^2-4*I/(8*a^2-2*b^2)/(-2*I*a-(-(2*a-b )*(2*a+b))^(1/2))*(-(2*a-b)*(2*a+b))^(1/2)*ln(1-b*exp(2*I*x)/(-2*I*a-(-(2* a-b)*(2*a+b))^(1/2)))*a*x-8*I/(8*a^2-2*b^2)/(-2*I*a+(-(2*a-b)*(2*a+b))^(1/ 2))*a^2*x^2+8/(8*a^2-2*b^2)/(-2*I*a+(-(2*a-b)*(2*a+b))^(1/2))*ln(1-b*exp(2 *I*x)/(-2*I*a+(-(2*a-b)*(2*a+b))^(1/2)))*a^2*x-4/(8*a^2-2*b^2)/(-2*I*a-(-( 2*a-b)*(2*a+b))^(1/2))*(-(2*a-b)*(2*a+b))^(1/2)*a*x^2-2/(8*a^2-2*b^2)/(-2* I*a-(-(2*a-b)*(2*a+b))^(1/2))*ln(1-b*exp(2*I*x)/(-2*I*a-(-(2*a-b)*(2*a+b)) ^(1/2)))*b^2*x-2/(8*a^2-2*b^2)/(-2*I*a-(-(2*a-b)*(2*a+b))^(1/2))*(-(2*a-b) *(2*a+b))^(1/2)*polylog(2,b*exp(2*I*x)/(-2*I*a-(-(2*a-b)*(2*a+b))^(1/2)...
Both result and optimal contain complex but leaf count of result is larger than twice the leaf count of optimal. 1676 vs. \(2 (179) = 358\).
Time = 1.19 (sec) , antiderivative size = 1676, normalized size of antiderivative = 7.45 \[ \int \frac {x}{a+b \cos (x) \sin (x)} \, dx=\text {Too large to display} \]
-1/2*(b*x*sqrt(-(4*a^2 - b^2)/b^2)*log(-((2*I*a*cos(x) + 2*a*sin(x) - (b*c os(x) - I*b*sin(x))*sqrt(-(4*a^2 - b^2)/b^2))*sqrt((b*sqrt(-(4*a^2 - b^2)/ b^2) + 2*I*a)/b) - b)/b) + b*x*sqrt(-(4*a^2 - b^2)/b^2)*log(-((-2*I*a*cos( x) - 2*a*sin(x) + (b*cos(x) - I*b*sin(x))*sqrt(-(4*a^2 - b^2)/b^2))*sqrt(( b*sqrt(-(4*a^2 - b^2)/b^2) + 2*I*a)/b) - b)/b) - b*x*sqrt(-(4*a^2 - b^2)/b ^2)*log(-((2*I*a*cos(x) - 2*a*sin(x) - (b*cos(x) + I*b*sin(x))*sqrt(-(4*a^ 2 - b^2)/b^2))*sqrt(-(b*sqrt(-(4*a^2 - b^2)/b^2) + 2*I*a)/b) - b)/b) - b*x *sqrt(-(4*a^2 - b^2)/b^2)*log(-((-2*I*a*cos(x) + 2*a*sin(x) + (b*cos(x) + I*b*sin(x))*sqrt(-(4*a^2 - b^2)/b^2))*sqrt(-(b*sqrt(-(4*a^2 - b^2)/b^2) + 2*I*a)/b) - b)/b) + b*x*sqrt(-(4*a^2 - b^2)/b^2)*log(-((2*I*a*cos(x) - 2*a *sin(x) + (b*cos(x) + I*b*sin(x))*sqrt(-(4*a^2 - b^2)/b^2))*sqrt((b*sqrt(- (4*a^2 - b^2)/b^2) - 2*I*a)/b) - b)/b) + b*x*sqrt(-(4*a^2 - b^2)/b^2)*log( -((-2*I*a*cos(x) + 2*a*sin(x) - (b*cos(x) + I*b*sin(x))*sqrt(-(4*a^2 - b^2 )/b^2))*sqrt((b*sqrt(-(4*a^2 - b^2)/b^2) - 2*I*a)/b) - b)/b) - b*x*sqrt(-( 4*a^2 - b^2)/b^2)*log(-((2*I*a*cos(x) + 2*a*sin(x) + (b*cos(x) - I*b*sin(x ))*sqrt(-(4*a^2 - b^2)/b^2))*sqrt(-(b*sqrt(-(4*a^2 - b^2)/b^2) - 2*I*a)/b) - b)/b) - b*x*sqrt(-(4*a^2 - b^2)/b^2)*log(-((-2*I*a*cos(x) - 2*a*sin(x) - (b*cos(x) - I*b*sin(x))*sqrt(-(4*a^2 - b^2)/b^2))*sqrt(-(b*sqrt(-(4*a^2 - b^2)/b^2) - 2*I*a)/b) - b)/b) + I*b*sqrt(-(4*a^2 - b^2)/b^2)*dilog(((2*I *a*cos(x) + 2*a*sin(x) - (b*cos(x) - I*b*sin(x))*sqrt(-(4*a^2 - b^2)/b^...
\[ \int \frac {x}{a+b \cos (x) \sin (x)} \, dx=\int \frac {x}{a + b \sin {\left (x \right )} \cos {\left (x \right )}}\, dx \]
\[ \int \frac {x}{a+b \cos (x) \sin (x)} \, dx=\int { \frac {x}{b \cos \left (x\right ) \sin \left (x\right ) + a} \,d x } \]
\[ \int \frac {x}{a+b \cos (x) \sin (x)} \, dx=\int { \frac {x}{b \cos \left (x\right ) \sin \left (x\right ) + a} \,d x } \]
Timed out. \[ \int \frac {x}{a+b \cos (x) \sin (x)} \, dx=\int \frac {x}{a+b\,\cos \left (x\right )\,\sin \left (x\right )} \,d x \]