Integrand size = 20, antiderivative size = 76 \[ \int \cos ^2(a+b x) \sin ^4(2 a+2 b x) \, dx=\frac {3 x}{16}-\frac {3 \cos (2 a+2 b x) \sin (2 a+2 b x)}{32 b}-\frac {\cos (2 a+2 b x) \sin ^3(2 a+2 b x)}{16 b}+\frac {\sin ^5(2 a+2 b x)}{20 b} \]
3/16*x-3/32*cos(2*b*x+2*a)*sin(2*b*x+2*a)/b-1/16*cos(2*b*x+2*a)*sin(2*b*x+ 2*a)^3/b+1/20*sin(2*b*x+2*a)^5/b
Time = 0.14 (sec) , antiderivative size = 62, normalized size of antiderivative = 0.82 \[ \int \cos ^2(a+b x) \sin ^4(2 a+2 b x) \, dx=\frac {120 b x+20 \sin (2 (a+b x))-40 \sin (4 (a+b x))-10 \sin (6 (a+b x))+5 \sin (8 (a+b x))+2 \sin (10 (a+b x))}{640 b} \]
(120*b*x + 20*Sin[2*(a + b*x)] - 40*Sin[4*(a + b*x)] - 10*Sin[6*(a + b*x)] + 5*Sin[8*(a + b*x)] + 2*Sin[10*(a + b*x)])/(640*b)
Time = 0.38 (sec) , antiderivative size = 86, normalized size of antiderivative = 1.13, number of steps used = 10, number of rules used = 9, \(\frac {\text {number of rules}}{\text {integrand size}}\) = 0.450, Rules used = {3042, 4773, 3042, 3044, 15, 3115, 3042, 3115, 24}
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.
\(\displaystyle \int \sin ^4(2 a+2 b x) \cos ^2(a+b x) \, dx\) |
\(\Big \downarrow \) 3042 |
\(\displaystyle \int \sin (2 a+2 b x)^4 \cos (a+b x)^2dx\) |
\(\Big \downarrow \) 4773 |
\(\displaystyle \frac {1}{2} \int \sin ^4(2 a+2 b x)dx+\frac {1}{2} \int \cos (2 a+2 b x) \sin ^4(2 a+2 b x)dx\) |
\(\Big \downarrow \) 3042 |
\(\displaystyle \frac {1}{2} \int \sin (2 a+2 b x)^4dx+\frac {1}{2} \int \cos (2 a+2 b x) \sin (2 a+2 b x)^4dx\) |
\(\Big \downarrow \) 3044 |
\(\displaystyle \frac {\int \sin ^4(2 a+2 b x)d\sin (2 a+2 b x)}{4 b}+\frac {1}{2} \int \sin (2 a+2 b x)^4dx\) |
\(\Big \downarrow \) 15 |
\(\displaystyle \frac {1}{2} \int \sin (2 a+2 b x)^4dx+\frac {\sin ^5(2 a+2 b x)}{20 b}\) |
\(\Big \downarrow \) 3115 |
\(\displaystyle \frac {1}{2} \left (\frac {3}{4} \int \sin ^2(2 a+2 b x)dx-\frac {\sin ^3(2 a+2 b x) \cos (2 a+2 b x)}{8 b}\right )+\frac {\sin ^5(2 a+2 b x)}{20 b}\) |
\(\Big \downarrow \) 3042 |
\(\displaystyle \frac {1}{2} \left (\frac {3}{4} \int \sin (2 a+2 b x)^2dx-\frac {\sin ^3(2 a+2 b x) \cos (2 a+2 b x)}{8 b}\right )+\frac {\sin ^5(2 a+2 b x)}{20 b}\) |
\(\Big \downarrow \) 3115 |
\(\displaystyle \frac {1}{2} \left (\frac {3}{4} \left (\frac {\int 1dx}{2}-\frac {\sin (2 a+2 b x) \cos (2 a+2 b x)}{4 b}\right )-\frac {\sin ^3(2 a+2 b x) \cos (2 a+2 b x)}{8 b}\right )+\frac {\sin ^5(2 a+2 b x)}{20 b}\) |
\(\Big \downarrow \) 24 |
\(\displaystyle \frac {\sin ^5(2 a+2 b x)}{20 b}+\frac {1}{2} \left (\frac {3}{4} \left (\frac {x}{2}-\frac {\sin (2 a+2 b x) \cos (2 a+2 b x)}{4 b}\right )-\frac {\sin ^3(2 a+2 b x) \cos (2 a+2 b x)}{8 b}\right )\) |
Sin[2*a + 2*b*x]^5/(20*b) + (-1/8*(Cos[2*a + 2*b*x]*Sin[2*a + 2*b*x]^3)/b + (3*(x/2 - (Cos[2*a + 2*b*x]*Sin[2*a + 2*b*x])/(4*b)))/4)/2
3.2.42.3.1 Defintions of rubi rules used
Int[(a_.)*(x_)^(m_.), x_Symbol] :> Simp[a*(x^(m + 1)/(m + 1)), x] /; FreeQ[ {a, m}, x] && NeQ[m, -1]
Int[cos[(e_.) + (f_.)*(x_)]^(n_.)*((a_.)*sin[(e_.) + (f_.)*(x_)])^(m_.), x_ Symbol] :> Simp[1/(a*f) Subst[Int[x^m*(1 - x^2/a^2)^((n - 1)/2), x], x, a *Sin[e + f*x]], x] /; FreeQ[{a, e, f, m}, x] && IntegerQ[(n - 1)/2] && !(I ntegerQ[(m - 1)/2] && LtQ[0, m, n])
Int[((b_.)*sin[(c_.) + (d_.)*(x_)])^(n_), x_Symbol] :> Simp[(-b)*Cos[c + d* x]*((b*Sin[c + d*x])^(n - 1)/(d*n)), x] + Simp[b^2*((n - 1)/n) Int[(b*Sin [c + d*x])^(n - 2), x], x] /; FreeQ[{b, c, d}, x] && GtQ[n, 1] && IntegerQ[ 2*n]
Int[cos[(a_.) + (b_.)*(x_)]^2*((g_.)*sin[(c_.) + (d_.)*(x_)])^(p_), x_Symbo l] :> Simp[1/2 Int[(g*Sin[c + d*x])^p, x], x] + Simp[1/2 Int[Cos[c + d* x]*(g*Sin[c + d*x])^p, x], x] /; FreeQ[{a, b, c, d, g}, x] && EqQ[b*c - a*d , 0] && EqQ[d/b, 2] && IGtQ[p/2, 0]
Time = 1.65 (sec) , antiderivative size = 66, normalized size of antiderivative = 0.87
method | result | size |
parallelrisch | \(\frac {120 x b +20 \sin \left (2 x b +2 a \right )-40 \sin \left (4 x b +4 a \right )-10 \sin \left (6 x b +6 a \right )+5 \sin \left (8 x b +8 a \right )+2 \sin \left (10 x b +10 a \right )}{640 b}\) | \(66\) |
default | \(\frac {3 x}{16}+\frac {\sin \left (2 x b +2 a \right )}{32 b}-\frac {\sin \left (4 x b +4 a \right )}{16 b}-\frac {\sin \left (6 x b +6 a \right )}{64 b}+\frac {\sin \left (8 x b +8 a \right )}{128 b}+\frac {\sin \left (10 x b +10 a \right )}{320 b}\) | \(75\) |
risch | \(\frac {3 x}{16}+\frac {\sin \left (2 x b +2 a \right )}{32 b}-\frac {\sin \left (4 x b +4 a \right )}{16 b}-\frac {\sin \left (6 x b +6 a \right )}{64 b}+\frac {\sin \left (8 x b +8 a \right )}{128 b}+\frac {\sin \left (10 x b +10 a \right )}{320 b}\) | \(75\) |
1/640*(120*x*b+20*sin(2*b*x+2*a)-40*sin(4*b*x+4*a)-10*sin(6*b*x+6*a)+5*sin (8*b*x+8*a)+2*sin(10*b*x+10*a))/b
Time = 0.25 (sec) , antiderivative size = 66, normalized size of antiderivative = 0.87 \[ \int \cos ^2(a+b x) \sin ^4(2 a+2 b x) \, dx=\frac {15 \, b x + {\left (128 \, \cos \left (b x + a\right )^{9} - 176 \, \cos \left (b x + a\right )^{7} + 8 \, \cos \left (b x + a\right )^{5} + 10 \, \cos \left (b x + a\right )^{3} + 15 \, \cos \left (b x + a\right )\right )} \sin \left (b x + a\right )}{80 \, b} \]
1/80*(15*b*x + (128*cos(b*x + a)^9 - 176*cos(b*x + a)^7 + 8*cos(b*x + a)^5 + 10*cos(b*x + a)^3 + 15*cos(b*x + a))*sin(b*x + a))/b
Leaf count of result is larger than twice the leaf count of optimal. 434 vs. \(2 (70) = 140\).
Time = 4.91 (sec) , antiderivative size = 434, normalized size of antiderivative = 5.71 \[ \int \cos ^2(a+b x) \sin ^4(2 a+2 b x) \, dx=\begin {cases} \frac {3 x \sin ^{2}{\left (a + b x \right )} \sin ^{4}{\left (2 a + 2 b x \right )}}{16} + \frac {3 x \sin ^{2}{\left (a + b x \right )} \sin ^{2}{\left (2 a + 2 b x \right )} \cos ^{2}{\left (2 a + 2 b x \right )}}{8} + \frac {3 x \sin ^{2}{\left (a + b x \right )} \cos ^{4}{\left (2 a + 2 b x \right )}}{16} + \frac {3 x \sin ^{4}{\left (2 a + 2 b x \right )} \cos ^{2}{\left (a + b x \right )}}{16} + \frac {3 x \sin ^{2}{\left (2 a + 2 b x \right )} \cos ^{2}{\left (a + b x \right )} \cos ^{2}{\left (2 a + 2 b x \right )}}{8} + \frac {3 x \cos ^{2}{\left (a + b x \right )} \cos ^{4}{\left (2 a + 2 b x \right )}}{16} + \frac {7 \sin ^{2}{\left (a + b x \right )} \sin ^{3}{\left (2 a + 2 b x \right )} \cos {\left (2 a + 2 b x \right )}}{160 b} + \frac {19 \sin ^{2}{\left (a + b x \right )} \sin {\left (2 a + 2 b x \right )} \cos ^{3}{\left (2 a + 2 b x \right )}}{480 b} + \frac {\sin {\left (a + b x \right )} \sin ^{4}{\left (2 a + 2 b x \right )} \cos {\left (a + b x \right )}}{10 b} + \frac {2 \sin {\left (a + b x \right )} \sin ^{2}{\left (2 a + 2 b x \right )} \cos {\left (a + b x \right )} \cos ^{2}{\left (2 a + 2 b x \right )}}{5 b} + \frac {4 \sin {\left (a + b x \right )} \cos {\left (a + b x \right )} \cos ^{4}{\left (2 a + 2 b x \right )}}{15 b} - \frac {57 \sin ^{3}{\left (2 a + 2 b x \right )} \cos ^{2}{\left (a + b x \right )} \cos {\left (2 a + 2 b x \right )}}{160 b} - \frac {109 \sin {\left (2 a + 2 b x \right )} \cos ^{2}{\left (a + b x \right )} \cos ^{3}{\left (2 a + 2 b x \right )}}{480 b} & \text {for}\: b \neq 0 \\x \sin ^{4}{\left (2 a \right )} \cos ^{2}{\left (a \right )} & \text {otherwise} \end {cases} \]
Piecewise((3*x*sin(a + b*x)**2*sin(2*a + 2*b*x)**4/16 + 3*x*sin(a + b*x)** 2*sin(2*a + 2*b*x)**2*cos(2*a + 2*b*x)**2/8 + 3*x*sin(a + b*x)**2*cos(2*a + 2*b*x)**4/16 + 3*x*sin(2*a + 2*b*x)**4*cos(a + b*x)**2/16 + 3*x*sin(2*a + 2*b*x)**2*cos(a + b*x)**2*cos(2*a + 2*b*x)**2/8 + 3*x*cos(a + b*x)**2*co s(2*a + 2*b*x)**4/16 + 7*sin(a + b*x)**2*sin(2*a + 2*b*x)**3*cos(2*a + 2*b *x)/(160*b) + 19*sin(a + b*x)**2*sin(2*a + 2*b*x)*cos(2*a + 2*b*x)**3/(480 *b) + sin(a + b*x)*sin(2*a + 2*b*x)**4*cos(a + b*x)/(10*b) + 2*sin(a + b*x )*sin(2*a + 2*b*x)**2*cos(a + b*x)*cos(2*a + 2*b*x)**2/(5*b) + 4*sin(a + b *x)*cos(a + b*x)*cos(2*a + 2*b*x)**4/(15*b) - 57*sin(2*a + 2*b*x)**3*cos(a + b*x)**2*cos(2*a + 2*b*x)/(160*b) - 109*sin(2*a + 2*b*x)*cos(a + b*x)**2 *cos(2*a + 2*b*x)**3/(480*b), Ne(b, 0)), (x*sin(2*a)**4*cos(a)**2, True))
Time = 0.21 (sec) , antiderivative size = 65, normalized size of antiderivative = 0.86 \[ \int \cos ^2(a+b x) \sin ^4(2 a+2 b x) \, dx=\frac {120 \, b x + 2 \, \sin \left (10 \, b x + 10 \, a\right ) + 5 \, \sin \left (8 \, b x + 8 \, a\right ) - 10 \, \sin \left (6 \, b x + 6 \, a\right ) - 40 \, \sin \left (4 \, b x + 4 \, a\right ) + 20 \, \sin \left (2 \, b x + 2 \, a\right )}{640 \, b} \]
1/640*(120*b*x + 2*sin(10*b*x + 10*a) + 5*sin(8*b*x + 8*a) - 10*sin(6*b*x + 6*a) - 40*sin(4*b*x + 4*a) + 20*sin(2*b*x + 2*a))/b
Time = 0.30 (sec) , antiderivative size = 68, normalized size of antiderivative = 0.89 \[ \int \cos ^2(a+b x) \sin ^4(2 a+2 b x) \, dx=\frac {120 \, b x + 120 \, a + 2 \, \sin \left (10 \, b x + 10 \, a\right ) + 5 \, \sin \left (8 \, b x + 8 \, a\right ) - 10 \, \sin \left (6 \, b x + 6 \, a\right ) - 40 \, \sin \left (4 \, b x + 4 \, a\right ) + 20 \, \sin \left (2 \, b x + 2 \, a\right )}{640 \, b} \]
1/640*(120*b*x + 120*a + 2*sin(10*b*x + 10*a) + 5*sin(8*b*x + 8*a) - 10*si n(6*b*x + 6*a) - 40*sin(4*b*x + 4*a) + 20*sin(2*b*x + 2*a))/b
Time = 21.14 (sec) , antiderivative size = 109, normalized size of antiderivative = 1.43 \[ \int \cos ^2(a+b x) \sin ^4(2 a+2 b x) \, dx=\frac {3\,x}{16}+\frac {\frac {3\,{\mathrm {tan}\left (a+b\,x\right )}^9}{16}+\frac {7\,{\mathrm {tan}\left (a+b\,x\right )}^7}{8}+\frac {8\,{\mathrm {tan}\left (a+b\,x\right )}^5}{5}-\frac {7\,{\mathrm {tan}\left (a+b\,x\right )}^3}{8}-\frac {3\,\mathrm {tan}\left (a+b\,x\right )}{16}}{b\,\left ({\mathrm {tan}\left (a+b\,x\right )}^{10}+5\,{\mathrm {tan}\left (a+b\,x\right )}^8+10\,{\mathrm {tan}\left (a+b\,x\right )}^6+10\,{\mathrm {tan}\left (a+b\,x\right )}^4+5\,{\mathrm {tan}\left (a+b\,x\right )}^2+1\right )} \]