Integrand size = 41, antiderivative size = 122 \[ \int (a+b \tan (d+e x)) \sqrt {b^2+2 a b \tan (d+e x)+a^2 \tan ^2(d+e x)} \, dx=-\frac {\left (a^2+b^2\right ) \log (\cos (d+e x)) \sqrt {b^2+2 a b \tan (d+e x)+a^2 \tan ^2(d+e x)}}{e (b+a \tan (d+e x))}+\frac {a^2 b \tan (d+e x) \sqrt {b^2+2 a b \tan (d+e x)+a^2 \tan ^2(d+e x)}}{e \left (a b+a^2 \tan (d+e x)\right )} \]
-(a^2+b^2)*ln(cos(e*x+d))*(b^2+2*a*b*tan(e*x+d)+a^2*tan(e*x+d)^2)^(1/2)/e/ (b+a*tan(e*x+d))+a^2*b*(b^2+2*a*b*tan(e*x+d)+a^2*tan(e*x+d)^2)^(1/2)*tan(e *x+d)/e/(a*b+a^2*tan(e*x+d))
Time = 0.24 (sec) , antiderivative size = 58, normalized size of antiderivative = 0.48 \[ \int (a+b \tan (d+e x)) \sqrt {b^2+2 a b \tan (d+e x)+a^2 \tan ^2(d+e x)} \, dx=\frac {\sqrt {(b+a \tan (d+e x))^2} \left (-\left (\left (a^2+b^2\right ) \log (\cos (d+e x))\right )+a b \tan (d+e x)\right )}{e (b+a \tan (d+e x))} \]
(Sqrt[(b + a*Tan[d + e*x])^2]*(-((a^2 + b^2)*Log[Cos[d + e*x]]) + a*b*Tan[ d + e*x]))/(e*(b + a*Tan[d + e*x]))
Time = 0.45 (sec) , antiderivative size = 82, normalized size of antiderivative = 0.67, number of steps used = 7, number of rules used = 7, \(\frac {\text {number of rules}}{\text {integrand size}}\) = 0.171, Rules used = {3042, 4193, 27, 3042, 4008, 3042, 3956}
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.
\(\displaystyle \int (a+b \tan (d+e x)) \sqrt {a^2 \tan ^2(d+e x)+2 a b \tan (d+e x)+b^2} \, dx\) |
\(\Big \downarrow \) 3042 |
\(\displaystyle \int (a+b \tan (d+e x)) \sqrt {a^2 \tan (d+e x)^2+2 a b \tan (d+e x)+b^2}dx\) |
\(\Big \downarrow \) 4193 |
\(\displaystyle \frac {\sqrt {a^2 \tan ^2(d+e x)+2 a b \tan (d+e x)+b^2} \int 2 \left (\tan (d+e x) a^2+b a\right ) (a+b \tan (d+e x))dx}{2 \left (a^2 \tan (d+e x)+a b\right )}\) |
\(\Big \downarrow \) 27 |
\(\displaystyle \frac {\sqrt {a^2 \tan ^2(d+e x)+2 a b \tan (d+e x)+b^2} \int \left (\tan (d+e x) a^2+b a\right ) (a+b \tan (d+e x))dx}{a^2 \tan (d+e x)+a b}\) |
\(\Big \downarrow \) 3042 |
\(\displaystyle \frac {\sqrt {a^2 \tan ^2(d+e x)+2 a b \tan (d+e x)+b^2} \int \left (\tan (d+e x) a^2+b a\right ) (a+b \tan (d+e x))dx}{a^2 \tan (d+e x)+a b}\) |
\(\Big \downarrow \) 4008 |
\(\displaystyle \frac {\sqrt {a^2 \tan ^2(d+e x)+2 a b \tan (d+e x)+b^2} \left (a \left (a^2+b^2\right ) \int \tan (d+e x)dx+\frac {a^2 b \tan (d+e x)}{e}\right )}{a^2 \tan (d+e x)+a b}\) |
\(\Big \downarrow \) 3042 |
\(\displaystyle \frac {\sqrt {a^2 \tan ^2(d+e x)+2 a b \tan (d+e x)+b^2} \left (a \left (a^2+b^2\right ) \int \tan (d+e x)dx+\frac {a^2 b \tan (d+e x)}{e}\right )}{a^2 \tan (d+e x)+a b}\) |
\(\Big \downarrow \) 3956 |
\(\displaystyle \frac {\sqrt {a^2 \tan ^2(d+e x)+2 a b \tan (d+e x)+b^2} \left (\frac {a^2 b \tan (d+e x)}{e}-\frac {a \left (a^2+b^2\right ) \log (\cos (d+e x))}{e}\right )}{a^2 \tan (d+e x)+a b}\) |
((-((a*(a^2 + b^2)*Log[Cos[d + e*x]])/e) + (a^2*b*Tan[d + e*x])/e)*Sqrt[b^ 2 + 2*a*b*Tan[d + e*x] + a^2*Tan[d + e*x]^2])/(a*b + a^2*Tan[d + e*x])
3.6.15.3.1 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[tan[(c_.) + (d_.)*(x_)], x_Symbol] :> Simp[-Log[RemoveContent[Cos[c + d *x], x]]/d, x] /; FreeQ[{c, d}, x]
Int[((a_) + (b_.)*tan[(e_.) + (f_.)*(x_)])*((c_.) + (d_.)*tan[(e_.) + (f_.) *(x_)]), x_Symbol] :> Simp[(a*c - b*d)*x, x] + (Simp[b*d*(Tan[e + f*x]/f), x] + Simp[(b*c + a*d) Int[Tan[e + f*x], x], x]) /; FreeQ[{a, b, c, d, e, f}, x] && NeQ[b*c - a*d, 0] && NeQ[b*c + a*d, 0]
Int[((A_) + (B_.)*tan[(d_.) + (e_.)*(x_)])*((a_) + (b_.)*tan[(d_.) + (e_.)* (x_)] + (c_.)*tan[(d_.) + (e_.)*(x_)]^2)^(n_), x_Symbol] :> Simp[(a + b*Tan [d + e*x] + c*Tan[d + e*x]^2)^n/(b + 2*c*Tan[d + e*x])^(2*n) Int[(A + B*T an[d + e*x])*(b + 2*c*Tan[d + e*x])^(2*n), x], x] /; FreeQ[{a, b, c, d, e, A, B}, x] && EqQ[b^2 - 4*a*c, 0] && !IntegerQ[n]
Result contains higher order function than in optimal. Order 9 vs. order 3.
Time = 1.17 (sec) , antiderivative size = 75, normalized size of antiderivative = 0.61
method | result | size |
derivativedivides | \(\frac {\operatorname {csgn}\left (b +a \tan \left (e x +d \right )\right ) \left (\ln \left (a^{2} \tan \left (e x +d \right )^{2}+a^{2}\right ) a^{2}+\ln \left (a^{2} \tan \left (e x +d \right )^{2}+a^{2}\right ) b^{2}+2 a b \tan \left (e x +d \right )+2 b^{2}\right )}{2 e}\) | \(75\) |
default | \(\frac {\operatorname {csgn}\left (b +a \tan \left (e x +d \right )\right ) \left (\ln \left (a^{2} \tan \left (e x +d \right )^{2}+a^{2}\right ) a^{2}+\ln \left (a^{2} \tan \left (e x +d \right )^{2}+a^{2}\right ) b^{2}+2 a b \tan \left (e x +d \right )+2 b^{2}\right )}{2 e}\) | \(75\) |
parts | \(\frac {a \,\operatorname {csgn}\left (b +a \tan \left (e x +d \right )\right ) \left (\ln \left (a^{2} \tan \left (e x +d \right )^{2}+a^{2}\right ) a +2 b \arctan \left (\tan \left (e x +d \right )\right )\right )}{2 e}+\frac {b \,\operatorname {csgn}\left (b +a \tan \left (e x +d \right )\right ) \left (b \ln \left (a^{2} \tan \left (e x +d \right )^{2}+a^{2}\right )-2 a \arctan \left (\tan \left (e x +d \right )\right )+2 a \tan \left (e x +d \right )+2 b \right )}{2 e}\) | \(108\) |
1/2/e*csgn(b+a*tan(e*x+d))*(ln(a^2*tan(e*x+d)^2+a^2)*a^2+ln(a^2*tan(e*x+d) ^2+a^2)*b^2+2*a*b*tan(e*x+d)+2*b^2)
Time = 0.26 (sec) , antiderivative size = 38, normalized size of antiderivative = 0.31 \[ \int (a+b \tan (d+e x)) \sqrt {b^2+2 a b \tan (d+e x)+a^2 \tan ^2(d+e x)} \, dx=\frac {2 \, a b \tan \left (e x + d\right ) - {\left (a^{2} + b^{2}\right )} \log \left (\frac {1}{\tan \left (e x + d\right )^{2} + 1}\right )}{2 \, e} \]
integrate((b^2+2*a*b*tan(e*x+d)+a^2*tan(e*x+d)^2)^(1/2)*(a+b*tan(e*x+d)),x , algorithm="fricas")
\[ \int (a+b \tan (d+e x)) \sqrt {b^2+2 a b \tan (d+e x)+a^2 \tan ^2(d+e x)} \, dx=\int \left (a + b \tan {\left (d + e x \right )}\right ) \sqrt {\left (a \tan {\left (d + e x \right )} + b\right )^{2}}\, dx \]
Time = 0.31 (sec) , antiderivative size = 65, normalized size of antiderivative = 0.53 \[ \int (a+b \tan (d+e x)) \sqrt {b^2+2 a b \tan (d+e x)+a^2 \tan ^2(d+e x)} \, dx=\frac {{\left (2 \, {\left (e x + d\right )} b + a \log \left (\tan \left (e x + d\right )^{2} + 1\right )\right )} a - {\left (2 \, {\left (e x + d\right )} a - b \log \left (\tan \left (e x + d\right )^{2} + 1\right ) - 2 \, a \tan \left (e x + d\right )\right )} b}{2 \, e} \]
integrate((b^2+2*a*b*tan(e*x+d)+a^2*tan(e*x+d)^2)^(1/2)*(a+b*tan(e*x+d)),x , algorithm="maxima")
1/2*((2*(e*x + d)*b + a*log(tan(e*x + d)^2 + 1))*a - (2*(e*x + d)*a - b*lo g(tan(e*x + d)^2 + 1) - 2*a*tan(e*x + d))*b)/e
Leaf count of result is larger than twice the leaf count of optimal. 323 vs. \(2 (118) = 236\).
Time = 0.40 (sec) , antiderivative size = 323, normalized size of antiderivative = 2.65 \[ \int (a+b \tan (d+e x)) \sqrt {b^2+2 a b \tan (d+e x)+a^2 \tan ^2(d+e x)} \, dx=-\frac {a^{2} \log \left (\frac {4 \, {\left (\tan \left (e x\right )^{2} \tan \left (d\right )^{2} - 2 \, \tan \left (e x\right ) \tan \left (d\right ) + 1\right )}}{\tan \left (e x\right )^{2} \tan \left (d\right )^{2} + \tan \left (e x\right )^{2} + \tan \left (d\right )^{2} + 1}\right ) \mathrm {sgn}\left (a \tan \left (e x + d\right ) + b\right ) \tan \left (e x\right ) \tan \left (d\right ) + b^{2} \log \left (\frac {4 \, {\left (\tan \left (e x\right )^{2} \tan \left (d\right )^{2} - 2 \, \tan \left (e x\right ) \tan \left (d\right ) + 1\right )}}{\tan \left (e x\right )^{2} \tan \left (d\right )^{2} + \tan \left (e x\right )^{2} + \tan \left (d\right )^{2} + 1}\right ) \mathrm {sgn}\left (a \tan \left (e x + d\right ) + b\right ) \tan \left (e x\right ) \tan \left (d\right ) - a^{2} \log \left (\frac {4 \, {\left (\tan \left (e x\right )^{2} \tan \left (d\right )^{2} - 2 \, \tan \left (e x\right ) \tan \left (d\right ) + 1\right )}}{\tan \left (e x\right )^{2} \tan \left (d\right )^{2} + \tan \left (e x\right )^{2} + \tan \left (d\right )^{2} + 1}\right ) \mathrm {sgn}\left (a \tan \left (e x + d\right ) + b\right ) - b^{2} \log \left (\frac {4 \, {\left (\tan \left (e x\right )^{2} \tan \left (d\right )^{2} - 2 \, \tan \left (e x\right ) \tan \left (d\right ) + 1\right )}}{\tan \left (e x\right )^{2} \tan \left (d\right )^{2} + \tan \left (e x\right )^{2} + \tan \left (d\right )^{2} + 1}\right ) \mathrm {sgn}\left (a \tan \left (e x + d\right ) + b\right ) + 2 \, a b \mathrm {sgn}\left (a \tan \left (e x + d\right ) + b\right ) \tan \left (e x\right ) + 2 \, a b \mathrm {sgn}\left (a \tan \left (e x + d\right ) + b\right ) \tan \left (d\right )}{2 \, {\left (e \tan \left (e x\right ) \tan \left (d\right ) - e\right )}} \]
integrate((b^2+2*a*b*tan(e*x+d)+a^2*tan(e*x+d)^2)^(1/2)*(a+b*tan(e*x+d)),x , algorithm="giac")
-1/2*(a^2*log(4*(tan(e*x)^2*tan(d)^2 - 2*tan(e*x)*tan(d) + 1)/(tan(e*x)^2* tan(d)^2 + tan(e*x)^2 + tan(d)^2 + 1))*sgn(a*tan(e*x + d) + b)*tan(e*x)*ta n(d) + b^2*log(4*(tan(e*x)^2*tan(d)^2 - 2*tan(e*x)*tan(d) + 1)/(tan(e*x)^2 *tan(d)^2 + tan(e*x)^2 + tan(d)^2 + 1))*sgn(a*tan(e*x + d) + b)*tan(e*x)*t an(d) - a^2*log(4*(tan(e*x)^2*tan(d)^2 - 2*tan(e*x)*tan(d) + 1)/(tan(e*x)^ 2*tan(d)^2 + tan(e*x)^2 + tan(d)^2 + 1))*sgn(a*tan(e*x + d) + b) - b^2*log (4*(tan(e*x)^2*tan(d)^2 - 2*tan(e*x)*tan(d) + 1)/(tan(e*x)^2*tan(d)^2 + ta n(e*x)^2 + tan(d)^2 + 1))*sgn(a*tan(e*x + d) + b) + 2*a*b*sgn(a*tan(e*x + d) + b)*tan(e*x) + 2*a*b*sgn(a*tan(e*x + d) + b)*tan(d))/(e*tan(e*x)*tan(d ) - e)
Timed out. \[ \int (a+b \tan (d+e x)) \sqrt {b^2+2 a b \tan (d+e x)+a^2 \tan ^2(d+e x)} \, dx=\int \left (a+b\,\mathrm {tan}\left (d+e\,x\right )\right )\,\sqrt {a^2\,{\mathrm {tan}\left (d+e\,x\right )}^2+2\,a\,b\,\mathrm {tan}\left (d+e\,x\right )+b^2} \,d x \]