Integrand size = 20, antiderivative size = 156 \[ \int \frac {(a+b \sin (e+f x))^2}{c+d x} \, dx=-\frac {b^2 \cos \left (2 e-\frac {2 c f}{d}\right ) \operatorname {CosIntegral}\left (\frac {2 c f}{d}+2 f x\right )}{2 d}+\frac {a^2 \log (c+d x)}{d}+\frac {b^2 \log (c+d x)}{2 d}+\frac {2 a b \operatorname {CosIntegral}\left (\frac {c f}{d}+f x\right ) \sin \left (e-\frac {c f}{d}\right )}{d}+\frac {2 a b \cos \left (e-\frac {c f}{d}\right ) \text {Si}\left (\frac {c f}{d}+f x\right )}{d}+\frac {b^2 \sin \left (2 e-\frac {2 c f}{d}\right ) \text {Si}\left (\frac {2 c f}{d}+2 f x\right )}{2 d} \]
-1/2*b^2*Ci(2*c*f/d+2*f*x)*cos(-2*e+2*c*f/d)/d+a^2*ln(d*x+c)/d+1/2*b^2*ln( d*x+c)/d+2*a*b*cos(-e+c*f/d)*Si(c*f/d+f*x)/d-1/2*b^2*Si(2*c*f/d+2*f*x)*sin (-2*e+2*c*f/d)/d-2*a*b*Ci(c*f/d+f*x)*sin(-e+c*f/d)/d
Time = 0.24 (sec) , antiderivative size = 134, normalized size of antiderivative = 0.86 \[ \int \frac {(a+b \sin (e+f x))^2}{c+d x} \, dx=\frac {-b^2 \cos \left (2 e-\frac {2 c f}{d}\right ) \operatorname {CosIntegral}\left (\frac {2 f (c+d x)}{d}\right )+2 a^2 \log (c+d x)+b^2 \log (c+d x)+4 a b \operatorname {CosIntegral}\left (f \left (\frac {c}{d}+x\right )\right ) \sin \left (e-\frac {c f}{d}\right )+4 a b \cos \left (e-\frac {c f}{d}\right ) \text {Si}\left (f \left (\frac {c}{d}+x\right )\right )+b^2 \sin \left (2 e-\frac {2 c f}{d}\right ) \text {Si}\left (\frac {2 f (c+d x)}{d}\right )}{2 d} \]
(-(b^2*Cos[2*e - (2*c*f)/d]*CosIntegral[(2*f*(c + d*x))/d]) + 2*a^2*Log[c + d*x] + b^2*Log[c + d*x] + 4*a*b*CosIntegral[f*(c/d + x)]*Sin[e - (c*f)/d ] + 4*a*b*Cos[e - (c*f)/d]*SinIntegral[f*(c/d + x)] + b^2*Sin[2*e - (2*c*f )/d]*SinIntegral[(2*f*(c + d*x))/d])/(2*d)
Time = 0.50 (sec) , antiderivative size = 156, 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 = {3042, 3798, 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.
\(\displaystyle \int \frac {(a+b \sin (e+f x))^2}{c+d x} \, dx\) |
\(\Big \downarrow \) 3042 |
\(\displaystyle \int \frac {(a+b \sin (e+f x))^2}{c+d x}dx\) |
\(\Big \downarrow \) 3798 |
\(\displaystyle \int \left (\frac {a^2}{c+d x}+\frac {2 a b \sin (e+f x)}{c+d x}+\frac {b^2 \sin ^2(e+f x)}{c+d x}\right )dx\) |
\(\Big \downarrow \) 2009 |
\(\displaystyle \frac {a^2 \log (c+d x)}{d}+\frac {2 a b \operatorname {CosIntegral}\left (x f+\frac {c f}{d}\right ) \sin \left (e-\frac {c f}{d}\right )}{d}+\frac {2 a b \cos \left (e-\frac {c f}{d}\right ) \text {Si}\left (x f+\frac {c f}{d}\right )}{d}-\frac {b^2 \operatorname {CosIntegral}\left (2 x f+\frac {2 c f}{d}\right ) \cos \left (2 e-\frac {2 c f}{d}\right )}{2 d}+\frac {b^2 \sin \left (2 e-\frac {2 c f}{d}\right ) \text {Si}\left (2 x f+\frac {2 c f}{d}\right )}{2 d}+\frac {b^2 \log (c+d x)}{2 d}\) |
-1/2*(b^2*Cos[2*e - (2*c*f)/d]*CosIntegral[(2*c*f)/d + 2*f*x])/d + (a^2*Lo g[c + d*x])/d + (b^2*Log[c + d*x])/(2*d) + (2*a*b*CosIntegral[(c*f)/d + f* x]*Sin[e - (c*f)/d])/d + (2*a*b*Cos[e - (c*f)/d]*SinIntegral[(c*f)/d + f*x ])/d + (b^2*Sin[2*e - (2*c*f)/d]*SinIntegral[(2*c*f)/d + 2*f*x])/(2*d)
3.2.60.3.1 Defintions of rubi rules used
Int[((c_.) + (d_.)*(x_))^(m_.)*((a_) + (b_.)*sin[(e_.) + (f_.)*(x_)])^(n_.) , x_Symbol] :> Int[ExpandIntegrand[(c + d*x)^m, (a + b*Sin[e + f*x])^n, x], x] /; FreeQ[{a, b, c, d, e, f, m}, x] && IGtQ[n, 0] && (EqQ[n, 1] || IGtQ[ m, 0] || NeQ[a^2 - b^2, 0])
Time = 0.23 (sec) , antiderivative size = 203, normalized size of antiderivative = 1.30
method | result | size |
parts | \(\frac {a^{2} \ln \left (d x +c \right )}{d}+\frac {b^{2} \ln \left (c f -d e +d \left (f x +e \right )\right )}{2 d}-\frac {b^{2} \operatorname {Si}\left (2 f x +2 e +\frac {2 c f -2 d e}{d}\right ) \sin \left (\frac {2 c f -2 d e}{d}\right )}{2 d}-\frac {b^{2} \operatorname {Ci}\left (2 f x +2 e +\frac {2 c f -2 d e}{d}\right ) \cos \left (\frac {2 c f -2 d e}{d}\right )}{2 d}+2 a b \left (\frac {\operatorname {Si}\left (f x +e +\frac {c f -d e}{d}\right ) \cos \left (\frac {c f -d e}{d}\right )}{d}-\frac {\operatorname {Ci}\left (f x +e +\frac {c f -d e}{d}\right ) \sin \left (\frac {c f -d e}{d}\right )}{d}\right )\) | \(203\) |
derivativedivides | \(\frac {\frac {f \,a^{2} \ln \left (c f -d e +d \left (f x +e \right )\right )}{d}+2 f b a \left (\frac {\operatorname {Si}\left (f x +e +\frac {c f -d e}{d}\right ) \cos \left (\frac {c f -d e}{d}\right )}{d}-\frac {\operatorname {Ci}\left (f x +e +\frac {c f -d e}{d}\right ) \sin \left (\frac {c f -d e}{d}\right )}{d}\right )+\frac {f \,b^{2} \ln \left (c f -d e +d \left (f x +e \right )\right )}{2 d}-\frac {f \,b^{2} \left (\frac {2 \,\operatorname {Si}\left (2 f x +2 e +\frac {2 c f -2 d e}{d}\right ) \sin \left (\frac {2 c f -2 d e}{d}\right )}{d}+\frac {2 \,\operatorname {Ci}\left (2 f x +2 e +\frac {2 c f -2 d e}{d}\right ) \cos \left (\frac {2 c f -2 d e}{d}\right )}{d}\right )}{4}}{f}\) | \(221\) |
default | \(\frac {\frac {f \,a^{2} \ln \left (c f -d e +d \left (f x +e \right )\right )}{d}+2 f b a \left (\frac {\operatorname {Si}\left (f x +e +\frac {c f -d e}{d}\right ) \cos \left (\frac {c f -d e}{d}\right )}{d}-\frac {\operatorname {Ci}\left (f x +e +\frac {c f -d e}{d}\right ) \sin \left (\frac {c f -d e}{d}\right )}{d}\right )+\frac {f \,b^{2} \ln \left (c f -d e +d \left (f x +e \right )\right )}{2 d}-\frac {f \,b^{2} \left (\frac {2 \,\operatorname {Si}\left (2 f x +2 e +\frac {2 c f -2 d e}{d}\right ) \sin \left (\frac {2 c f -2 d e}{d}\right )}{d}+\frac {2 \,\operatorname {Ci}\left (2 f x +2 e +\frac {2 c f -2 d e}{d}\right ) \cos \left (\frac {2 c f -2 d e}{d}\right )}{d}\right )}{4}}{f}\) | \(221\) |
risch | \(-\frac {i a b \,{\mathrm e}^{\frac {i \left (c f -d e \right )}{d}} \operatorname {Ei}_{1}\left (i f x +i e +\frac {i \left (c f -d e \right )}{d}\right )}{d}+\frac {a^{2} \ln \left (d x +c \right )}{d}+\frac {b^{2} \ln \left (d x +c \right )}{2 d}+\frac {b^{2} {\mathrm e}^{\frac {2 i \left (c f -d e \right )}{d}} \operatorname {Ei}_{1}\left (2 i f x +2 i e +\frac {2 i \left (c f -d e \right )}{d}\right )}{4 d}+\frac {b^{2} {\mathrm e}^{-\frac {2 i \left (c f -d e \right )}{d}} \operatorname {Ei}_{1}\left (-2 i f x -2 i e -\frac {2 \left (i c f -i d e \right )}{d}\right )}{4 d}+\frac {i a b \,{\mathrm e}^{-\frac {i \left (c f -d e \right )}{d}} \operatorname {Ei}_{1}\left (-i f x -i e -\frac {i c f -i d e}{d}\right )}{d}\) | \(229\) |
a^2*ln(d*x+c)/d+1/2*b^2*ln(c*f-d*e+d*(f*x+e))/d-1/2*b^2*Si(2*f*x+2*e+2*(c* f-d*e)/d)*sin(2*(c*f-d*e)/d)/d-1/2*b^2*Ci(2*f*x+2*e+2*(c*f-d*e)/d)*cos(2*( c*f-d*e)/d)/d+2*a*b*(Si(f*x+e+(c*f-d*e)/d)*cos((c*f-d*e)/d)/d-Ci(f*x+e+(c* f-d*e)/d)*sin((c*f-d*e)/d)/d)
Time = 0.27 (sec) , antiderivative size = 149, normalized size of antiderivative = 0.96 \[ \int \frac {(a+b \sin (e+f x))^2}{c+d x} \, dx=-\frac {b^{2} \cos \left (-\frac {2 \, {\left (d e - c f\right )}}{d}\right ) \operatorname {Ci}\left (\frac {2 \, {\left (d f x + c f\right )}}{d}\right ) + 4 \, a b \operatorname {Ci}\left (\frac {d f x + c f}{d}\right ) \sin \left (-\frac {d e - c f}{d}\right ) + b^{2} \sin \left (-\frac {2 \, {\left (d e - c f\right )}}{d}\right ) \operatorname {Si}\left (\frac {2 \, {\left (d f x + c f\right )}}{d}\right ) - 4 \, a b \cos \left (-\frac {d e - c f}{d}\right ) \operatorname {Si}\left (\frac {d f x + c f}{d}\right ) - {\left (2 \, a^{2} + b^{2}\right )} \log \left (d x + c\right )}{2 \, d} \]
-1/2*(b^2*cos(-2*(d*e - c*f)/d)*cos_integral(2*(d*f*x + c*f)/d) + 4*a*b*co s_integral((d*f*x + c*f)/d)*sin(-(d*e - c*f)/d) + b^2*sin(-2*(d*e - c*f)/d )*sin_integral(2*(d*f*x + c*f)/d) - 4*a*b*cos(-(d*e - c*f)/d)*sin_integral ((d*f*x + c*f)/d) - (2*a^2 + b^2)*log(d*x + c))/d
\[ \int \frac {(a+b \sin (e+f x))^2}{c+d x} \, dx=\int \frac {\left (a + b \sin {\left (e + f x \right )}\right )^{2}}{c + d x}\, dx \]
Result contains complex when optimal does not.
Time = 0.29 (sec) , antiderivative size = 336, normalized size of antiderivative = 2.15 \[ \int \frac {(a+b \sin (e+f x))^2}{c+d x} \, dx=\frac {\frac {4 \, a^{2} f \log \left (c + \frac {{\left (f x + e\right )} d}{f} - \frac {d e}{f}\right )}{d} + \frac {4 \, {\left (f {\left (-i \, E_{1}\left (\frac {i \, {\left (f x + e\right )} d - i \, d e + i \, c f}{d}\right ) + i \, E_{1}\left (-\frac {i \, {\left (f x + e\right )} d - i \, d e + i \, c f}{d}\right )\right )} \cos \left (-\frac {d e - c f}{d}\right ) + f {\left (E_{1}\left (\frac {i \, {\left (f x + e\right )} d - i \, d e + i \, c f}{d}\right ) + E_{1}\left (-\frac {i \, {\left (f x + e\right )} d - i \, d e + i \, c f}{d}\right )\right )} \sin \left (-\frac {d e - c f}{d}\right )\right )} a b}{d} + \frac {{\left (f {\left (E_{1}\left (\frac {2 \, {\left (-i \, {\left (f x + e\right )} d + i \, d e - i \, c f\right )}}{d}\right ) + E_{1}\left (-\frac {2 \, {\left (-i \, {\left (f x + e\right )} d + i \, d e - i \, c f\right )}}{d}\right )\right )} \cos \left (-\frac {2 \, {\left (d e - c f\right )}}{d}\right ) + f {\left (-i \, E_{1}\left (\frac {2 \, {\left (-i \, {\left (f x + e\right )} d + i \, d e - i \, c f\right )}}{d}\right ) + i \, E_{1}\left (-\frac {2 \, {\left (-i \, {\left (f x + e\right )} d + i \, d e - i \, c f\right )}}{d}\right )\right )} \sin \left (-\frac {2 \, {\left (d e - c f\right )}}{d}\right ) + 2 \, f \log \left ({\left (f x + e\right )} d - d e + c f\right )\right )} b^{2}}{d}}{4 \, f} \]
1/4*(4*a^2*f*log(c + (f*x + e)*d/f - d*e/f)/d + 4*(f*(-I*exp_integral_e(1, (I*(f*x + e)*d - I*d*e + I*c*f)/d) + I*exp_integral_e(1, -(I*(f*x + e)*d - I*d*e + I*c*f)/d))*cos(-(d*e - c*f)/d) + f*(exp_integral_e(1, (I*(f*x + e)*d - I*d*e + I*c*f)/d) + exp_integral_e(1, -(I*(f*x + e)*d - I*d*e + I*c *f)/d))*sin(-(d*e - c*f)/d))*a*b/d + (f*(exp_integral_e(1, 2*(-I*(f*x + e) *d + I*d*e - I*c*f)/d) + exp_integral_e(1, -2*(-I*(f*x + e)*d + I*d*e - I* c*f)/d))*cos(-2*(d*e - c*f)/d) + f*(-I*exp_integral_e(1, 2*(-I*(f*x + e)*d + I*d*e - I*c*f)/d) + I*exp_integral_e(1, -2*(-I*(f*x + e)*d + I*d*e - I* c*f)/d))*sin(-2*(d*e - c*f)/d) + 2*f*log((f*x + e)*d - d*e + c*f))*b^2/d)/ f
Result contains higher order function than in optimal. Order 9 vs. order 4.
Time = 0.50 (sec) , antiderivative size = 7139, normalized size of antiderivative = 45.76 \[ \int \frac {(a+b \sin (e+f x))^2}{c+d x} \, dx=\text {Too large to display} \]
1/4*(4*a*b*imag_part(cos_integral(f*x + c*f/d))*tan(1/2*e)^2*tan(e)^2*tan( c*f/d)^2*tan(1/2*c*f/d)^2 - 4*a*b*imag_part(cos_integral(-f*x - c*f/d))*ta n(1/2*e)^2*tan(e)^2*tan(c*f/d)^2*tan(1/2*c*f/d)^2 + 4*a^2*log(abs(d*x + c) )*tan(1/2*e)^2*tan(e)^2*tan(c*f/d)^2*tan(1/2*c*f/d)^2 + 2*b^2*log(abs(d*x + c))*tan(1/2*e)^2*tan(e)^2*tan(c*f/d)^2*tan(1/2*c*f/d)^2 - b^2*real_part( cos_integral(2*f*x + 2*c*f/d))*tan(1/2*e)^2*tan(e)^2*tan(c*f/d)^2*tan(1/2* c*f/d)^2 - b^2*real_part(cos_integral(-2*f*x - 2*c*f/d))*tan(1/2*e)^2*tan( e)^2*tan(c*f/d)^2*tan(1/2*c*f/d)^2 + 8*a*b*sin_integral((d*f*x + c*f)/d)*t an(1/2*e)^2*tan(e)^2*tan(c*f/d)^2*tan(1/2*c*f/d)^2 + 8*a*b*real_part(cos_i ntegral(f*x + c*f/d))*tan(1/2*e)^2*tan(e)^2*tan(c*f/d)^2*tan(1/2*c*f/d) + 8*a*b*real_part(cos_integral(-f*x - c*f/d))*tan(1/2*e)^2*tan(e)^2*tan(c*f/ d)^2*tan(1/2*c*f/d) + 2*b^2*imag_part(cos_integral(2*f*x + 2*c*f/d))*tan(1 /2*e)^2*tan(e)^2*tan(c*f/d)*tan(1/2*c*f/d)^2 - 2*b^2*imag_part(cos_integra l(-2*f*x - 2*c*f/d))*tan(1/2*e)^2*tan(e)^2*tan(c*f/d)*tan(1/2*c*f/d)^2 + 4 *b^2*sin_integral(2*(d*f*x + c*f)/d)*tan(1/2*e)^2*tan(e)^2*tan(c*f/d)*tan( 1/2*c*f/d)^2 - 2*b^2*imag_part(cos_integral(2*f*x + 2*c*f/d))*tan(1/2*e)^2 *tan(e)*tan(c*f/d)^2*tan(1/2*c*f/d)^2 + 2*b^2*imag_part(cos_integral(-2*f* x - 2*c*f/d))*tan(1/2*e)^2*tan(e)*tan(c*f/d)^2*tan(1/2*c*f/d)^2 - 4*b^2*si n_integral(2*(d*f*x + c*f)/d)*tan(1/2*e)^2*tan(e)*tan(c*f/d)^2*tan(1/2*c*f /d)^2 - 8*a*b*real_part(cos_integral(f*x + c*f/d))*tan(1/2*e)*tan(e)^2*...
Timed out. \[ \int \frac {(a+b \sin (e+f x))^2}{c+d x} \, dx=\int \frac {{\left (a+b\,\sin \left (e+f\,x\right )\right )}^2}{c+d\,x} \,d x \]