Integrand size = 20, antiderivative size = 301 \[ \int (a+b \cosh (c+d x) \sinh (c+d x))^{5/2} \, dx=\frac {2 \sqrt {2} a b \cosh (2 c+2 d x) \sqrt {2 a+b \sinh (2 c+2 d x)}}{15 d}+\frac {b \cosh (2 c+2 d x) (2 a+b \sinh (2 c+2 d x))^{3/2}}{20 \sqrt {2} d}-\frac {i \left (92 a^2-9 b^2\right ) E\left (\frac {1}{2} \left (2 i c-\frac {\pi }{2}+2 i d x\right )|\frac {2 b}{2 i a+b}\right ) \sqrt {2 a+b \sinh (2 c+2 d x)}}{60 \sqrt {2} d \sqrt {\frac {2 a+b \sinh (2 c+2 d x)}{2 a-i b}}}+\frac {2 i \sqrt {2} a \left (4 a^2+b^2\right ) \operatorname {EllipticF}\left (\frac {1}{2} \left (2 i c-\frac {\pi }{2}+2 i d x\right ),\frac {2 b}{2 i a+b}\right ) \sqrt {\frac {2 a+b \sinh (2 c+2 d x)}{2 a-i b}}}{15 d \sqrt {2 a+b \sinh (2 c+2 d x)}} \]
1/40*b*cosh(2*d*x+2*c)*(2*a+b*sinh(2*d*x+2*c))^(3/2)/d*2^(1/2)+2/15*a*b*co sh(2*d*x+2*c)*2^(1/2)*(2*a+b*sinh(2*d*x+2*c))^(1/2)/d+1/120*I*(92*a^2-9*b^ 2)*(sin(I*c+1/4*Pi+I*d*x)^2)^(1/2)/sin(I*c+1/4*Pi+I*d*x)*EllipticE(cos(I*c +1/4*Pi+I*d*x),2^(1/2)*(b/(2*I*a+b))^(1/2))*(2*a+b*sinh(2*d*x+2*c))^(1/2)/ d*2^(1/2)/((2*a+b*sinh(2*d*x+2*c))/(2*a-I*b))^(1/2)-2/15*I*a*(4*a^2+b^2)*( sin(I*c+1/4*Pi+I*d*x)^2)^(1/2)/sin(I*c+1/4*Pi+I*d*x)*EllipticF(cos(I*c+1/4 *Pi+I*d*x),2^(1/2)*(b/(2*I*a+b))^(1/2))*2^(1/2)*((2*a+b*sinh(2*d*x+2*c))/( 2*a-I*b))^(1/2)/d/(2*a+b*sinh(2*d*x+2*c))^(1/2)
Time = 1.47 (sec) , antiderivative size = 239, normalized size of antiderivative = 0.79 \[ \int (a+b \cosh (c+d x) \sinh (c+d x))^{5/2} \, dx=\frac {2 \left (184 i a^3+92 a^2 b-18 i a b^2-9 b^3\right ) E\left (\frac {1}{4} (-4 i c+\pi -4 i d x)|-\frac {2 i b}{2 a-i b}\right ) \sqrt {\frac {2 a+b \sinh (2 (c+d x))}{2 a-i b}}-32 i a \left (4 a^2+b^2\right ) \operatorname {EllipticF}\left (\frac {1}{4} (-4 i c+\pi -4 i d x),-\frac {2 i b}{2 a-i b}\right ) \sqrt {\frac {2 a+b \sinh (2 (c+d x))}{2 a-i b}}+b \left (88 a^2 \cosh (2 (c+d x))+b (28 a+3 b \sinh (2 (c+d x))) \sinh (4 (c+d x))\right )}{120 d \sqrt {4 a+2 b \sinh (2 (c+d x))}} \]
(2*((184*I)*a^3 + 92*a^2*b - (18*I)*a*b^2 - 9*b^3)*EllipticE[((-4*I)*c + P i - (4*I)*d*x)/4, ((-2*I)*b)/(2*a - I*b)]*Sqrt[(2*a + b*Sinh[2*(c + d*x)]) /(2*a - I*b)] - (32*I)*a*(4*a^2 + b^2)*EllipticF[((-4*I)*c + Pi - (4*I)*d* x)/4, ((-2*I)*b)/(2*a - I*b)]*Sqrt[(2*a + b*Sinh[2*(c + d*x)])/(2*a - I*b) ] + b*(88*a^2*Cosh[2*(c + d*x)] + b*(28*a + 3*b*Sinh[2*(c + d*x)])*Sinh[4* (c + d*x)]))/(120*d*Sqrt[4*a + 2*b*Sinh[2*(c + d*x)]])
Time = 1.31 (sec) , antiderivative size = 297, normalized size of antiderivative = 0.99, number of steps used = 17, number of rules used = 17, \(\frac {\text {number of rules}}{\text {integrand size}}\) = 0.850, Rules used = {3042, 3145, 3042, 3135, 27, 3042, 3232, 27, 3042, 3231, 3042, 3134, 3042, 3132, 3142, 3042, 3140}
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.
\(\displaystyle \int (a+b \sinh (c+d x) \cosh (c+d x))^{5/2} \, dx\) |
\(\Big \downarrow \) 3042 |
\(\displaystyle \int (a-i b \sin (i c+i d x) \cos (i c+i d x))^{5/2}dx\) |
\(\Big \downarrow \) 3145 |
\(\displaystyle \int \left (a+\frac {1}{2} b \sinh (2 c+2 d x)\right )^{5/2}dx\) |
\(\Big \downarrow \) 3042 |
\(\displaystyle \int \left (a-\frac {1}{2} i b \sin (2 i c+2 i d x)\right )^{5/2}dx\) |
\(\Big \downarrow \) 3135 |
\(\displaystyle \frac {2}{5} \int \frac {\sqrt {2 a+b \sinh (2 c+2 d x)} \left (20 a^2+16 b \sinh (2 c+2 d x) a-3 b^2\right )}{8 \sqrt {2}}dx+\frac {b \cosh (2 c+2 d x) (2 a+b \sinh (2 c+2 d x))^{3/2}}{20 \sqrt {2} d}\) |
\(\Big \downarrow \) 27 |
\(\displaystyle \frac {\int \sqrt {2 a+b \sinh (2 c+2 d x)} \left (20 a^2+16 b \sinh (2 c+2 d x) a-3 b^2\right )dx}{20 \sqrt {2}}+\frac {b \cosh (2 c+2 d x) (2 a+b \sinh (2 c+2 d x))^{3/2}}{20 \sqrt {2} d}\) |
\(\Big \downarrow \) 3042 |
\(\displaystyle \frac {b \cosh (2 c+2 d x) (2 a+b \sinh (2 c+2 d x))^{3/2}}{20 \sqrt {2} d}+\frac {\int \sqrt {2 a-i b \sin (2 i c+2 i d x)} \left (20 a^2-16 i b \sin (2 i c+2 i d x) a-3 b^2\right )dx}{20 \sqrt {2}}\) |
\(\Big \downarrow \) 3232 |
\(\displaystyle \frac {\frac {2}{3} \int \frac {2 a \left (60 a^2-17 b^2\right )+b \left (92 a^2-9 b^2\right ) \sinh (2 c+2 d x)}{2 \sqrt {2 a+b \sinh (2 c+2 d x)}}dx+\frac {16 a b \cosh (2 c+2 d x) \sqrt {2 a+b \sinh (2 c+2 d x)}}{3 d}}{20 \sqrt {2}}+\frac {b \cosh (2 c+2 d x) (2 a+b \sinh (2 c+2 d x))^{3/2}}{20 \sqrt {2} d}\) |
\(\Big \downarrow \) 27 |
\(\displaystyle \frac {\frac {1}{3} \int \frac {2 a \left (60 a^2-17 b^2\right )+b \left (92 a^2-9 b^2\right ) \sinh (2 c+2 d x)}{\sqrt {2 a+b \sinh (2 c+2 d x)}}dx+\frac {16 a b \cosh (2 c+2 d x) \sqrt {2 a+b \sinh (2 c+2 d x)}}{3 d}}{20 \sqrt {2}}+\frac {b \cosh (2 c+2 d x) (2 a+b \sinh (2 c+2 d x))^{3/2}}{20 \sqrt {2} d}\) |
\(\Big \downarrow \) 3042 |
\(\displaystyle \frac {b \cosh (2 c+2 d x) (2 a+b \sinh (2 c+2 d x))^{3/2}}{20 \sqrt {2} d}+\frac {\frac {16 a b \cosh (2 c+2 d x) \sqrt {2 a+b \sinh (2 c+2 d x)}}{3 d}+\frac {1}{3} \int \frac {2 a \left (60 a^2-17 b^2\right )-i b \left (92 a^2-9 b^2\right ) \sin (2 i c+2 i d x)}{\sqrt {2 a-i b \sin (2 i c+2 i d x)}}dx}{20 \sqrt {2}}\) |
\(\Big \downarrow \) 3231 |
\(\displaystyle \frac {\frac {1}{3} \left (\left (92 a^2-9 b^2\right ) \int \sqrt {2 a+b \sinh (2 c+2 d x)}dx-16 a \left (4 a^2+b^2\right ) \int \frac {1}{\sqrt {2 a+b \sinh (2 c+2 d x)}}dx\right )+\frac {16 a b \cosh (2 c+2 d x) \sqrt {2 a+b \sinh (2 c+2 d x)}}{3 d}}{20 \sqrt {2}}+\frac {b \cosh (2 c+2 d x) (2 a+b \sinh (2 c+2 d x))^{3/2}}{20 \sqrt {2} d}\) |
\(\Big \downarrow \) 3042 |
\(\displaystyle \frac {b \cosh (2 c+2 d x) (2 a+b \sinh (2 c+2 d x))^{3/2}}{20 \sqrt {2} d}+\frac {\frac {16 a b \cosh (2 c+2 d x) \sqrt {2 a+b \sinh (2 c+2 d x)}}{3 d}+\frac {1}{3} \left (\left (92 a^2-9 b^2\right ) \int \sqrt {2 a-i b \sin (2 i c+2 i d x)}dx-16 a \left (4 a^2+b^2\right ) \int \frac {1}{\sqrt {2 a-i b \sin (2 i c+2 i d x)}}dx\right )}{20 \sqrt {2}}\) |
\(\Big \downarrow \) 3134 |
\(\displaystyle \frac {b \cosh (2 c+2 d x) (2 a+b \sinh (2 c+2 d x))^{3/2}}{20 \sqrt {2} d}+\frac {\frac {16 a b \cosh (2 c+2 d x) \sqrt {2 a+b \sinh (2 c+2 d x)}}{3 d}+\frac {1}{3} \left (\frac {\left (92 a^2-9 b^2\right ) \sqrt {2 a+b \sinh (2 c+2 d x)} \int \sqrt {\frac {2 a}{2 a-i b}+\frac {b \sinh (2 c+2 d x)}{2 a-i b}}dx}{\sqrt {\frac {2 a+b \sinh (2 c+2 d x)}{2 a-i b}}}-16 a \left (4 a^2+b^2\right ) \int \frac {1}{\sqrt {2 a-i b \sin (2 i c+2 i d x)}}dx\right )}{20 \sqrt {2}}\) |
\(\Big \downarrow \) 3042 |
\(\displaystyle \frac {b \cosh (2 c+2 d x) (2 a+b \sinh (2 c+2 d x))^{3/2}}{20 \sqrt {2} d}+\frac {\frac {16 a b \cosh (2 c+2 d x) \sqrt {2 a+b \sinh (2 c+2 d x)}}{3 d}+\frac {1}{3} \left (\frac {\left (92 a^2-9 b^2\right ) \sqrt {2 a+b \sinh (2 c+2 d x)} \int \sqrt {\frac {2 a}{2 a-i b}-\frac {i b \sin (2 i c+2 i d x)}{2 a-i b}}dx}{\sqrt {\frac {2 a+b \sinh (2 c+2 d x)}{2 a-i b}}}-16 a \left (4 a^2+b^2\right ) \int \frac {1}{\sqrt {2 a-i b \sin (2 i c+2 i d x)}}dx\right )}{20 \sqrt {2}}\) |
\(\Big \downarrow \) 3132 |
\(\displaystyle \frac {b \cosh (2 c+2 d x) (2 a+b \sinh (2 c+2 d x))^{3/2}}{20 \sqrt {2} d}+\frac {\frac {16 a b \cosh (2 c+2 d x) \sqrt {2 a+b \sinh (2 c+2 d x)}}{3 d}+\frac {1}{3} \left (-16 a \left (4 a^2+b^2\right ) \int \frac {1}{\sqrt {2 a-i b \sin (2 i c+2 i d x)}}dx-\frac {i \left (92 a^2-9 b^2\right ) \sqrt {2 a+b \sinh (2 c+2 d x)} E\left (\frac {1}{2} \left (2 i c+2 i d x-\frac {\pi }{2}\right )|\frac {2 b}{2 i a+b}\right )}{d \sqrt {\frac {2 a+b \sinh (2 c+2 d x)}{2 a-i b}}}\right )}{20 \sqrt {2}}\) |
\(\Big \downarrow \) 3142 |
\(\displaystyle \frac {b \cosh (2 c+2 d x) (2 a+b \sinh (2 c+2 d x))^{3/2}}{20 \sqrt {2} d}+\frac {\frac {16 a b \cosh (2 c+2 d x) \sqrt {2 a+b \sinh (2 c+2 d x)}}{3 d}+\frac {1}{3} \left (-\frac {16 a \left (4 a^2+b^2\right ) \sqrt {\frac {2 a+b \sinh (2 c+2 d x)}{2 a-i b}} \int \frac {1}{\sqrt {\frac {2 a}{2 a-i b}+\frac {b \sinh (2 c+2 d x)}{2 a-i b}}}dx}{\sqrt {2 a+b \sinh (2 c+2 d x)}}-\frac {i \left (92 a^2-9 b^2\right ) \sqrt {2 a+b \sinh (2 c+2 d x)} E\left (\frac {1}{2} \left (2 i c+2 i d x-\frac {\pi }{2}\right )|\frac {2 b}{2 i a+b}\right )}{d \sqrt {\frac {2 a+b \sinh (2 c+2 d x)}{2 a-i b}}}\right )}{20 \sqrt {2}}\) |
\(\Big \downarrow \) 3042 |
\(\displaystyle \frac {b \cosh (2 c+2 d x) (2 a+b \sinh (2 c+2 d x))^{3/2}}{20 \sqrt {2} d}+\frac {\frac {16 a b \cosh (2 c+2 d x) \sqrt {2 a+b \sinh (2 c+2 d x)}}{3 d}+\frac {1}{3} \left (-\frac {16 a \left (4 a^2+b^2\right ) \sqrt {\frac {2 a+b \sinh (2 c+2 d x)}{2 a-i b}} \int \frac {1}{\sqrt {\frac {2 a}{2 a-i b}-\frac {i b \sin (2 i c+2 i d x)}{2 a-i b}}}dx}{\sqrt {2 a+b \sinh (2 c+2 d x)}}-\frac {i \left (92 a^2-9 b^2\right ) \sqrt {2 a+b \sinh (2 c+2 d x)} E\left (\frac {1}{2} \left (2 i c+2 i d x-\frac {\pi }{2}\right )|\frac {2 b}{2 i a+b}\right )}{d \sqrt {\frac {2 a+b \sinh (2 c+2 d x)}{2 a-i b}}}\right )}{20 \sqrt {2}}\) |
\(\Big \downarrow \) 3140 |
\(\displaystyle \frac {b \cosh (2 c+2 d x) (2 a+b \sinh (2 c+2 d x))^{3/2}}{20 \sqrt {2} d}+\frac {\frac {16 a b \cosh (2 c+2 d x) \sqrt {2 a+b \sinh (2 c+2 d x)}}{3 d}+\frac {1}{3} \left (\frac {16 i a \left (4 a^2+b^2\right ) \sqrt {\frac {2 a+b \sinh (2 c+2 d x)}{2 a-i b}} \operatorname {EllipticF}\left (\frac {1}{2} \left (2 i c+2 i d x-\frac {\pi }{2}\right ),\frac {2 b}{2 i a+b}\right )}{d \sqrt {2 a+b \sinh (2 c+2 d x)}}-\frac {i \left (92 a^2-9 b^2\right ) \sqrt {2 a+b \sinh (2 c+2 d x)} E\left (\frac {1}{2} \left (2 i c+2 i d x-\frac {\pi }{2}\right )|\frac {2 b}{2 i a+b}\right )}{d \sqrt {\frac {2 a+b \sinh (2 c+2 d x)}{2 a-i b}}}\right )}{20 \sqrt {2}}\) |
(b*Cosh[2*c + 2*d*x]*(2*a + b*Sinh[2*c + 2*d*x])^(3/2))/(20*Sqrt[2]*d) + ( (16*a*b*Cosh[2*c + 2*d*x]*Sqrt[2*a + b*Sinh[2*c + 2*d*x]])/(3*d) + (((-I)* (92*a^2 - 9*b^2)*EllipticE[((2*I)*c - Pi/2 + (2*I)*d*x)/2, (2*b)/((2*I)*a + b)]*Sqrt[2*a + b*Sinh[2*c + 2*d*x]])/(d*Sqrt[(2*a + b*Sinh[2*c + 2*d*x]) /(2*a - I*b)]) + ((16*I)*a*(4*a^2 + b^2)*EllipticF[((2*I)*c - Pi/2 + (2*I) *d*x)/2, (2*b)/((2*I)*a + b)]*Sqrt[(2*a + b*Sinh[2*c + 2*d*x])/(2*a - I*b) ])/(d*Sqrt[2*a + b*Sinh[2*c + 2*d*x]]))/3)/(20*Sqrt[2])
3.9.61.3.1 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[Sqrt[(a_) + (b_.)*sin[(c_.) + (d_.)*(x_)]], x_Symbol] :> Simp[2*(Sqrt[a + b]/d)*EllipticE[(1/2)*(c - Pi/2 + d*x), 2*(b/(a + b))], x] /; FreeQ[{a, b, c, d}, x] && NeQ[a^2 - b^2, 0] && GtQ[a + b, 0]
Int[Sqrt[(a_) + (b_.)*sin[(c_.) + (d_.)*(x_)]], x_Symbol] :> Simp[Sqrt[a + b*Sin[c + d*x]]/Sqrt[(a + b*Sin[c + d*x])/(a + b)] Int[Sqrt[a/(a + b) + ( b/(a + b))*Sin[c + d*x]], x], x] /; FreeQ[{a, b, c, d}, x] && NeQ[a^2 - b^2 , 0] && !GtQ[a + b, 0]
Int[((a_) + (b_.)*sin[(c_.) + (d_.)*(x_)])^(n_), x_Symbol] :> Simp[(-b)*Cos [c + d*x]*((a + b*Sin[c + d*x])^(n - 1)/(d*n)), x] + Simp[1/n Int[(a + b* Sin[c + d*x])^(n - 2)*Simp[a^2*n + b^2*(n - 1) + a*b*(2*n - 1)*Sin[c + d*x] , x], x], x] /; FreeQ[{a, b, c, d}, x] && NeQ[a^2 - b^2, 0] && GtQ[n, 1] && IntegerQ[2*n]
Int[1/Sqrt[(a_) + (b_.)*sin[(c_.) + (d_.)*(x_)]], x_Symbol] :> Simp[(2/(d*S qrt[a + b]))*EllipticF[(1/2)*(c - Pi/2 + d*x), 2*(b/(a + b))], x] /; FreeQ[ {a, b, c, d}, x] && NeQ[a^2 - b^2, 0] && GtQ[a + b, 0]
Int[1/Sqrt[(a_) + (b_.)*sin[(c_.) + (d_.)*(x_)]], x_Symbol] :> Simp[Sqrt[(a + b*Sin[c + d*x])/(a + b)]/Sqrt[a + b*Sin[c + d*x]] Int[1/Sqrt[a/(a + b) + (b/(a + b))*Sin[c + d*x]], x], x] /; FreeQ[{a, b, c, d}, x] && NeQ[a^2 - b^2, 0] && !GtQ[a + b, 0]
Int[((a_) + cos[(c_.) + (d_.)*(x_)]*(b_.)*sin[(c_.) + (d_.)*(x_)])^(n_), x_ Symbol] :> Int[(a + b*(Sin[2*c + 2*d*x]/2))^n, x] /; FreeQ[{a, b, c, d, n}, x]
Int[((c_.) + (d_.)*sin[(e_.) + (f_.)*(x_)])/Sqrt[(a_) + (b_.)*sin[(e_.) + ( f_.)*(x_)]], x_Symbol] :> Simp[(b*c - a*d)/b Int[1/Sqrt[a + b*Sin[e + f*x ]], x], x] + Simp[d/b Int[Sqrt[a + b*Sin[e + f*x]], x], x] /; FreeQ[{a, b , c, d, e, f}, x] && NeQ[b*c - a*d, 0] && NeQ[a^2 - b^2, 0]
Int[((a_) + (b_.)*sin[(e_.) + (f_.)*(x_)])^(m_)*((c_.) + (d_.)*sin[(e_.) + (f_.)*(x_)]), x_Symbol] :> Simp[(-d)*Cos[e + f*x]*((a + b*Sin[e + f*x])^m/( f*(m + 1))), x] + Simp[1/(m + 1) Int[(a + b*Sin[e + f*x])^(m - 1)*Simp[b* d*m + a*c*(m + 1) + (a*d*m + b*c*(m + 1))*Sin[e + f*x], x], x], x] /; FreeQ [{a, b, c, d, e, f}, x] && NeQ[b*c - a*d, 0] && NeQ[a^2 - b^2, 0] && GtQ[m, 0] && IntegerQ[2*m]
Both result and optimal contain complex but leaf count of result is larger than twice the leaf count of optimal. 1259 vs. \(2 (331 ) = 662\).
Time = 6.30 (sec) , antiderivative size = 1260, normalized size of antiderivative = 4.19
1/60*(64*I*(-(2*a+b*sinh(2*d*x+2*c))/(I*b-2*a))^(1/2)*((-sinh(2*d*x+2*c)+I )*b/(I*b+2*a))^(1/2)*((sinh(2*d*x+2*c)+I)*b/(I*b-2*a))^(1/2)*EllipticF((-( 2*a+b*sinh(2*d*x+2*c))/(I*b-2*a))^(1/2),(-(I*b-2*a)/(I*b+2*a))^(1/2))*a^3* b+16*I*(-(2*a+b*sinh(2*d*x+2*c))/(I*b-2*a))^(1/2)*((-sinh(2*d*x+2*c)+I)*b/ (I*b+2*a))^(1/2)*((sinh(2*d*x+2*c)+I)*b/(I*b-2*a))^(1/2)*EllipticF((-(2*a+ b*sinh(2*d*x+2*c))/(I*b-2*a))^(1/2),(-(I*b-2*a)/(I*b+2*a))^(1/2))*a*b^3+24 0*(-(2*a+b*sinh(2*d*x+2*c))/(I*b-2*a))^(1/2)*((-sinh(2*d*x+2*c)+I)*b/(I*b+ 2*a))^(1/2)*((sinh(2*d*x+2*c)+I)*b/(I*b-2*a))^(1/2)*EllipticF((-(2*a+b*sin h(2*d*x+2*c))/(I*b-2*a))^(1/2),(-(I*b-2*a)/(I*b+2*a))^(1/2))*a^4+24*(-(2*a +b*sinh(2*d*x+2*c))/(I*b-2*a))^(1/2)*((-sinh(2*d*x+2*c)+I)*b/(I*b+2*a))^(1 /2)*((sinh(2*d*x+2*c)+I)*b/(I*b-2*a))^(1/2)*EllipticF((-(2*a+b*sinh(2*d*x+ 2*c))/(I*b-2*a))^(1/2),(-(I*b-2*a)/(I*b+2*a))^(1/2))*a^2*b^2-9*(-(2*a+b*si nh(2*d*x+2*c))/(I*b-2*a))^(1/2)*((-sinh(2*d*x+2*c)+I)*b/(I*b+2*a))^(1/2)*( (sinh(2*d*x+2*c)+I)*b/(I*b-2*a))^(1/2)*EllipticF((-(2*a+b*sinh(2*d*x+2*c)) /(I*b-2*a))^(1/2),(-(I*b-2*a)/(I*b+2*a))^(1/2))*b^4-368*(-(2*a+b*sinh(2*d* x+2*c))/(I*b-2*a))^(1/2)*((-sinh(2*d*x+2*c)+I)*b/(I*b+2*a))^(1/2)*((sinh(2 *d*x+2*c)+I)*b/(I*b-2*a))^(1/2)*EllipticE((-(2*a+b*sinh(2*d*x+2*c))/(I*b-2 *a))^(1/2),(-(I*b-2*a)/(I*b+2*a))^(1/2))*a^4-56*(-(2*a+b*sinh(2*d*x+2*c))/ (I*b-2*a))^(1/2)*((-sinh(2*d*x+2*c)+I)*b/(I*b+2*a))^(1/2)*((sinh(2*d*x+2*c )+I)*b/(I*b-2*a))^(1/2)*EllipticE((-(2*a+b*sinh(2*d*x+2*c))/(I*b-2*a))^...
\[ \int (a+b \cosh (c+d x) \sinh (c+d x))^{5/2} \, dx=\int { {\left (b \cosh \left (d x + c\right ) \sinh \left (d x + c\right ) + a\right )}^{\frac {5}{2}} \,d x } \]
integral((b^2*cosh(d*x + c)^2*sinh(d*x + c)^2 + 2*a*b*cosh(d*x + c)*sinh(d *x + c) + a^2)*sqrt(b*cosh(d*x + c)*sinh(d*x + c) + a), x)
Timed out. \[ \int (a+b \cosh (c+d x) \sinh (c+d x))^{5/2} \, dx=\text {Timed out} \]
\[ \int (a+b \cosh (c+d x) \sinh (c+d x))^{5/2} \, dx=\int { {\left (b \cosh \left (d x + c\right ) \sinh \left (d x + c\right ) + a\right )}^{\frac {5}{2}} \,d x } \]
Exception generated. \[ \int (a+b \cosh (c+d x) \sinh (c+d x))^{5/2} \, dx=\text {Exception raised: TypeError} \]
Exception raised: TypeError >> an error occurred running a Giac command:IN PUT:sage2:=int(sage0,sageVARx):;OUTPUT:index.cc index_m i_lex_is_greater E rror: Bad Argument Value
Timed out. \[ \int (a+b \cosh (c+d x) \sinh (c+d x))^{5/2} \, dx=\int {\left (a+b\,\mathrm {cosh}\left (c+d\,x\right )\,\mathrm {sinh}\left (c+d\,x\right )\right )}^{5/2} \,d x \]