Integrand size = 16, antiderivative size = 73 \[ \int F^{c (a+b x)} \sin (d+e x) \, dx=-\frac {e F^{c (a+b x)} \cos (d+e x)}{e^2+b^2 c^2 \log ^2(F)}+\frac {b c F^{c (a+b x)} \log (F) \sin (d+e x)}{e^2+b^2 c^2 \log ^2(F)} \]
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Time = 0.02 (sec) , antiderivative size = 73, normalized size of antiderivative = 1.00, number of steps used = 1, number of rules used = 1, \(\frac {\text {number of rules}}{\text {integrand size}}\) = 0.062, Rules used = {4517} \[ \int F^{c (a+b x)} \sin (d+e x) \, dx=\frac {b c \log (F) \sin (d+e x) F^{c (a+b x)}}{b^2 c^2 \log ^2(F)+e^2}-\frac {e \cos (d+e x) F^{c (a+b x)}}{b^2 c^2 \log ^2(F)+e^2} \]
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Rule 4517
Rubi steps \begin{align*} \text {integral}& = -\frac {e F^{c (a+b x)} \cos (d+e x)}{e^2+b^2 c^2 \log ^2(F)}+\frac {b c F^{c (a+b x)} \log (F) \sin (d+e x)}{e^2+b^2 c^2 \log ^2(F)} \\ \end{align*}
Time = 0.08 (sec) , antiderivative size = 48, normalized size of antiderivative = 0.66 \[ \int F^{c (a+b x)} \sin (d+e x) \, dx=\frac {F^{c (a+b x)} (-e \cos (d+e x)+b c \log (F) \sin (d+e x))}{e^2+b^2 c^2 \log ^2(F)} \]
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Time = 0.36 (sec) , antiderivative size = 49, normalized size of antiderivative = 0.67
method | result | size |
parallelrisch | \(\frac {F^{c \left (x b +a \right )} \left (b c \ln \left (F \right ) \sin \left (e x +d \right )-e \cos \left (e x +d \right )\right )}{e^{2}+b^{2} c^{2} \ln \left (F \right )^{2}}\) | \(49\) |
risch | \(-\frac {e \,F^{c \left (x b +a \right )} \cos \left (e x +d \right )}{e^{2}+b^{2} c^{2} \ln \left (F \right )^{2}}+\frac {b c \,F^{c \left (x b +a \right )} \ln \left (F \right ) \sin \left (e x +d \right )}{e^{2}+b^{2} c^{2} \ln \left (F \right )^{2}}\) | \(74\) |
norman | \(\frac {\frac {e \,{\mathrm e}^{c \left (x b +a \right ) \ln \left (F \right )} \tan \left (\frac {e x}{2}+\frac {d}{2}\right )^{2}}{e^{2}+b^{2} c^{2} \ln \left (F \right )^{2}}-\frac {e \,{\mathrm e}^{c \left (x b +a \right ) \ln \left (F \right )}}{e^{2}+b^{2} c^{2} \ln \left (F \right )^{2}}+\frac {2 b c \ln \left (F \right ) {\mathrm e}^{c \left (x b +a \right ) \ln \left (F \right )} \tan \left (\frac {e x}{2}+\frac {d}{2}\right )}{e^{2}+b^{2} c^{2} \ln \left (F \right )^{2}}}{1+\tan \left (\frac {e x}{2}+\frac {d}{2}\right )^{2}}\) | \(130\) |
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Time = 0.24 (sec) , antiderivative size = 49, normalized size of antiderivative = 0.67 \[ \int F^{c (a+b x)} \sin (d+e x) \, dx=\frac {{\left (b c \log \left (F\right ) \sin \left (e x + d\right ) - e \cos \left (e x + d\right )\right )} F^{b c x + a c}}{b^{2} c^{2} \log \left (F\right )^{2} + e^{2}} \]
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Result contains complex when optimal does not.
Time = 0.58 (sec) , antiderivative size = 347, normalized size of antiderivative = 4.75 \[ \int F^{c (a+b x)} \sin (d+e x) \, dx=\begin {cases} x \sin {\left (d \right )} & \text {for}\: F = 1 \wedge e = 0 \\F^{a c} x \sin {\left (d \right )} & \text {for}\: b = 0 \wedge e = 0 \\x \sin {\left (d \right )} & \text {for}\: c = 0 \wedge e = 0 \\- \frac {F^{a c + b c x} x \sin {\left (i b c x \log {\left (F \right )} - d \right )}}{2} + \frac {i F^{a c + b c x} x \cos {\left (i b c x \log {\left (F \right )} - d \right )}}{2} + \frac {F^{a c + b c x} \sin {\left (i b c x \log {\left (F \right )} - d \right )}}{2 b c \log {\left (F \right )}} - \frac {i F^{a c + b c x} \cos {\left (i b c x \log {\left (F \right )} - d \right )}}{b c \log {\left (F \right )}} & \text {for}\: e = - i b c \log {\left (F \right )} \\\frac {F^{a c + b c x} x \sin {\left (i b c x \log {\left (F \right )} + d \right )}}{2} - \frac {i F^{a c + b c x} x \cos {\left (i b c x \log {\left (F \right )} + d \right )}}{2} - \frac {F^{a c + b c x} \sin {\left (i b c x \log {\left (F \right )} + d \right )}}{2 b c \log {\left (F \right )}} + \frac {i F^{a c + b c x} \cos {\left (i b c x \log {\left (F \right )} + d \right )}}{b c \log {\left (F \right )}} & \text {for}\: e = i b c \log {\left (F \right )} \\\frac {F^{a c + b c x} b c \log {\left (F \right )} \sin {\left (d + e x \right )}}{b^{2} c^{2} \log {\left (F \right )}^{2} + e^{2}} - \frac {F^{a c + b c x} e \cos {\left (d + e x \right )}}{b^{2} c^{2} \log {\left (F \right )}^{2} + e^{2}} & \text {otherwise} \end {cases} \]
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Leaf count of result is larger than twice the leaf count of optimal. 194 vs. \(2 (73) = 146\).
Time = 0.22 (sec) , antiderivative size = 194, normalized size of antiderivative = 2.66 \[ \int F^{c (a+b x)} \sin (d+e x) \, dx=-\frac {{\left (F^{a c} b c \log \left (F\right ) \sin \left (d\right ) + F^{a c} e \cos \left (d\right )\right )} F^{b c x} \cos \left (e x + 2 \, d\right ) - {\left (F^{a c} b c \log \left (F\right ) \sin \left (d\right ) - F^{a c} e \cos \left (d\right )\right )} F^{b c x} \cos \left (e x\right ) - {\left (F^{a c} b c \cos \left (d\right ) \log \left (F\right ) - F^{a c} e \sin \left (d\right )\right )} F^{b c x} \sin \left (e x + 2 \, d\right ) - {\left (F^{a c} b c \cos \left (d\right ) \log \left (F\right ) + F^{a c} e \sin \left (d\right )\right )} F^{b c x} \sin \left (e x\right )}{2 \, {\left (b^{2} c^{2} \cos \left (d\right )^{2} \log \left (F\right )^{2} + b^{2} c^{2} \log \left (F\right )^{2} \sin \left (d\right )^{2} + {\left (\cos \left (d\right )^{2} + \sin \left (d\right )^{2}\right )} e^{2}\right )}} \]
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Result contains complex when optimal does not.
Time = 0.29 (sec) , antiderivative size = 634, normalized size of antiderivative = 8.68 \[ \int F^{c (a+b x)} \sin (d+e x) \, dx=\text {Too large to display} \]
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Time = 28.20 (sec) , antiderivative size = 50, normalized size of antiderivative = 0.68 \[ \int F^{c (a+b x)} \sin (d+e x) \, dx=-\frac {F^{a\,c+b\,c\,x}\,\left (e\,\cos \left (d+e\,x\right )-b\,c\,\sin \left (d+e\,x\right )\,\ln \left (F\right )\right )}{b^2\,c^2\,{\ln \left (F\right )}^2+e^2} \]
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