Integrand size = 14, antiderivative size = 26 \[ \int x \left (a+b \csc \left (c+d x^2\right )\right ) \, dx=\frac {a x^2}{2}-\frac {b \text {arctanh}\left (\cos \left (c+d x^2\right )\right )}{2 d} \]
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Time = 0.03 (sec) , antiderivative size = 26, normalized size of antiderivative = 1.00, number of steps used = 4, number of rules used = 3, \(\frac {\text {number of rules}}{\text {integrand size}}\) = 0.214, Rules used = {14, 4290, 3855} \[ \int x \left (a+b \csc \left (c+d x^2\right )\right ) \, dx=\frac {a x^2}{2}-\frac {b \text {arctanh}\left (\cos \left (c+d x^2\right )\right )}{2 d} \]
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Rule 14
Rule 3855
Rule 4290
Rubi steps \begin{align*} \text {integral}& = \int \left (a x+b x \csc \left (c+d x^2\right )\right ) \, dx \\ & = \frac {a x^2}{2}+b \int x \csc \left (c+d x^2\right ) \, dx \\ & = \frac {a x^2}{2}+\frac {1}{2} b \text {Subst}\left (\int \csc (c+d x) \, dx,x,x^2\right ) \\ & = \frac {a x^2}{2}-\frac {b \text {arctanh}\left (\cos \left (c+d x^2\right )\right )}{2 d} \\ \end{align*}
Leaf count is larger than twice the leaf count of optimal. \(57\) vs. \(2(26)=52\).
Time = 0.09 (sec) , antiderivative size = 57, normalized size of antiderivative = 2.19 \[ \int x \left (a+b \csc \left (c+d x^2\right )\right ) \, dx=\frac {a x^2}{2}-\frac {b \log \left (\cos \left (\frac {c}{2}+\frac {d x^2}{2}\right )\right )}{2 d}+\frac {b \log \left (\sin \left (\frac {c}{2}+\frac {d x^2}{2}\right )\right )}{2 d} \]
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Time = 0.22 (sec) , antiderivative size = 26, normalized size of antiderivative = 1.00
method | result | size |
norman | \(\frac {a \,x^{2}}{2}+\frac {b \ln \left (\tan \left (\frac {d \,x^{2}}{2}+\frac {c}{2}\right )\right )}{2 d}\) | \(26\) |
parallelrisch | \(\frac {a \,x^{2} d +b \ln \left (\tan \left (\frac {d \,x^{2}}{2}+\frac {c}{2}\right )\right )}{2 d}\) | \(27\) |
parts | \(\frac {a \,x^{2}}{2}-\frac {b \ln \left (\csc \left (d \,x^{2}+c \right )+\cot \left (d \,x^{2}+c \right )\right )}{2 d}\) | \(32\) |
derivativedivides | \(\frac {\left (d \,x^{2}+c \right ) a -b \ln \left (\csc \left (d \,x^{2}+c \right )+\cot \left (d \,x^{2}+c \right )\right )}{2 d}\) | \(37\) |
default | \(\frac {\left (d \,x^{2}+c \right ) a -b \ln \left (\csc \left (d \,x^{2}+c \right )+\cot \left (d \,x^{2}+c \right )\right )}{2 d}\) | \(37\) |
risch | \(\frac {a \,x^{2}}{2}+\frac {b \ln \left ({\mathrm e}^{i \left (d \,x^{2}+c \right )}-1\right )}{2 d}-\frac {b \ln \left ({\mathrm e}^{i \left (d \,x^{2}+c \right )}+1\right )}{2 d}\) | \(48\) |
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none
Time = 0.24 (sec) , antiderivative size = 44, normalized size of antiderivative = 1.69 \[ \int x \left (a+b \csc \left (c+d x^2\right )\right ) \, dx=\frac {2 \, a d x^{2} - b \log \left (\frac {1}{2} \, \cos \left (d x^{2} + c\right ) + \frac {1}{2}\right ) + b \log \left (-\frac {1}{2} \, \cos \left (d x^{2} + c\right ) + \frac {1}{2}\right )}{4 \, d} \]
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Leaf count of result is larger than twice the leaf count of optimal. 42 vs. \(2 (20) = 40\).
Time = 2.57 (sec) , antiderivative size = 42, normalized size of antiderivative = 1.62 \[ \int x \left (a+b \csc \left (c+d x^2\right )\right ) \, dx=\begin {cases} \frac {a \left (c + d x^{2}\right ) - b \log {\left (\cot {\left (c + d x^{2} \right )} + \csc {\left (c + d x^{2} \right )} \right )}}{2 d} & \text {for}\: d \neq 0 \\\frac {x^{2} \left (a + b \csc {\left (c \right )}\right )}{2} & \text {otherwise} \end {cases} \]
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Time = 0.18 (sec) , antiderivative size = 31, normalized size of antiderivative = 1.19 \[ \int x \left (a+b \csc \left (c+d x^2\right )\right ) \, dx=\frac {1}{2} \, a x^{2} - \frac {b \log \left (\cot \left (d x^{2} + c\right ) + \csc \left (d x^{2} + c\right )\right )}{2 \, d} \]
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Time = 0.27 (sec) , antiderivative size = 30, normalized size of antiderivative = 1.15 \[ \int x \left (a+b \csc \left (c+d x^2\right )\right ) \, dx=\frac {{\left (d x^{2} + c\right )} a + b \log \left ({\left | \tan \left (\frac {1}{2} \, d x^{2} + \frac {1}{2} \, c\right ) \right |}\right )}{2 \, d} \]
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Time = 0.56 (sec) , antiderivative size = 69, normalized size of antiderivative = 2.65 \[ \int x \left (a+b \csc \left (c+d x^2\right )\right ) \, dx=\frac {a\,x^2}{2}-\frac {b\,\ln \left (-b\,x\,2{}\mathrm {i}-b\,x\,{\mathrm {e}}^{d\,x^2\,1{}\mathrm {i}}\,{\mathrm {e}}^{c\,1{}\mathrm {i}}\,2{}\mathrm {i}\right )}{2\,d}+\frac {b\,\ln \left (b\,x\,2{}\mathrm {i}-b\,x\,{\mathrm {e}}^{d\,x^2\,1{}\mathrm {i}}\,{\mathrm {e}}^{c\,1{}\mathrm {i}}\,2{}\mathrm {i}\right )}{2\,d} \]
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