Integrand size = 25, antiderivative size = 106 \[ \int \frac {\left (d^2-e^2 x^2\right )^p}{x^2 (d+e x)} \, dx=-\frac {\left (d^2-e^2 x^2\right )^p \left (1-\frac {e^2 x^2}{d^2}\right )^{-p} \operatorname {Hypergeometric2F1}\left (-\frac {1}{2},1-p,\frac {1}{2},\frac {e^2 x^2}{d^2}\right )}{d x}+\frac {e \left (d^2-e^2 x^2\right )^p \operatorname {Hypergeometric2F1}\left (1,p,1+p,1-\frac {e^2 x^2}{d^2}\right )}{2 d^2 p} \]
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Time = 0.05 (sec) , antiderivative size = 106, normalized size of antiderivative = 1.00, number of steps used = 6, number of rules used = 6, \(\frac {\text {number of rules}}{\text {integrand size}}\) = 0.240, Rules used = {864, 778, 372, 371, 272, 67} \[ \int \frac {\left (d^2-e^2 x^2\right )^p}{x^2 (d+e x)} \, dx=\frac {e \left (d^2-e^2 x^2\right )^p \operatorname {Hypergeometric2F1}\left (1,p,p+1,1-\frac {e^2 x^2}{d^2}\right )}{2 d^2 p}-\frac {\left (d^2-e^2 x^2\right )^p \left (1-\frac {e^2 x^2}{d^2}\right )^{-p} \operatorname {Hypergeometric2F1}\left (-\frac {1}{2},1-p,\frac {1}{2},\frac {e^2 x^2}{d^2}\right )}{d x} \]
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Rule 67
Rule 272
Rule 371
Rule 372
Rule 778
Rule 864
Rubi steps \begin{align*} \text {integral}& = \int \frac {(d-e x) \left (d^2-e^2 x^2\right )^{-1+p}}{x^2} \, dx \\ & = d \int \frac {\left (d^2-e^2 x^2\right )^{-1+p}}{x^2} \, dx-e \int \frac {\left (d^2-e^2 x^2\right )^{-1+p}}{x} \, dx \\ & = -\left (\frac {1}{2} e \text {Subst}\left (\int \frac {\left (d^2-e^2 x\right )^{-1+p}}{x} \, dx,x,x^2\right )\right )+\frac {\left (\left (d^2-e^2 x^2\right )^p \left (1-\frac {e^2 x^2}{d^2}\right )^{-p}\right ) \int \frac {\left (1-\frac {e^2 x^2}{d^2}\right )^{-1+p}}{x^2} \, dx}{d} \\ & = -\frac {\left (d^2-e^2 x^2\right )^p \left (1-\frac {e^2 x^2}{d^2}\right )^{-p} \, _2F_1\left (-\frac {1}{2},1-p;\frac {1}{2};\frac {e^2 x^2}{d^2}\right )}{d x}+\frac {e \left (d^2-e^2 x^2\right )^p \, _2F_1\left (1,p;1+p;1-\frac {e^2 x^2}{d^2}\right )}{2 d^2 p} \\ \end{align*}
Time = 0.31 (sec) , antiderivative size = 167, normalized size of antiderivative = 1.58 \[ \int \frac {\left (d^2-e^2 x^2\right )^p}{x^2 (d+e x)} \, dx=\frac {\left (d^2-e^2 x^2\right )^p \left (-\frac {2 d^2 \left (1-\frac {e^2 x^2}{d^2}\right )^{-p} \operatorname {Hypergeometric2F1}\left (-\frac {1}{2},-p,\frac {1}{2},\frac {e^2 x^2}{d^2}\right )}{x}+\frac {2^p e (-d+e x) \left (1+\frac {e x}{d}\right )^{-p} \operatorname {Hypergeometric2F1}\left (1-p,1+p,2+p,\frac {d-e x}{2 d}\right )}{1+p}-\frac {d e \left (1-\frac {d^2}{e^2 x^2}\right )^{-p} \operatorname {Hypergeometric2F1}\left (-p,-p,1-p,\frac {d^2}{e^2 x^2}\right )}{p}\right )}{2 d^3} \]
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\[\int \frac {\left (-e^{2} x^{2}+d^{2}\right )^{p}}{x^{2} \left (e x +d \right )}d x\]
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\[ \int \frac {\left (d^2-e^2 x^2\right )^p}{x^2 (d+e x)} \, dx=\int { \frac {{\left (-e^{2} x^{2} + d^{2}\right )}^{p}}{{\left (e x + d\right )} x^{2}} \,d x } \]
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Result contains complex when optimal does not.
Time = 4.91 (sec) , antiderivative size = 434, normalized size of antiderivative = 4.09 \[ \int \frac {\left (d^2-e^2 x^2\right )^p}{x^2 (d+e x)} \, dx=\begin {cases} - \frac {0^{p} d d^{2 p - 2}}{x} - \frac {0^{p} d^{2 p - 2} e \log {\left (\frac {e^{2} x^{2}}{d^{2}} \right )}}{2} + \frac {0^{p} d^{2 p - 2} e \log {\left (-1 + \frac {e^{2} x^{2}}{d^{2}} \right )}}{2} + 0^{p} d^{2 p - 2} e \operatorname {acoth}{\left (\frac {e x}{d} \right )} + \frac {d e^{2 p - 2} p x^{2 p - 3} e^{i \pi p} \Gamma \left (p\right ) \Gamma \left (\frac {3}{2} - p\right ) {{}_{2}F_{1}\left (\begin {matrix} 1 - p, \frac {3}{2} - p \\ \frac {5}{2} - p \end {matrix}\middle | {\frac {d^{2}}{e^{2} x^{2}}} \right )}}{2 \Gamma \left (\frac {5}{2} - p\right ) \Gamma \left (p + 1\right )} - \frac {e^{2 p - 1} p x^{2 p - 2} e^{i \pi p} \Gamma \left (p\right ) \Gamma \left (1 - p\right ) {{}_{2}F_{1}\left (\begin {matrix} 1 - p, 1 - p \\ 2 - p \end {matrix}\middle | {\frac {d^{2}}{e^{2} x^{2}}} \right )}}{2 \Gamma \left (2 - p\right ) \Gamma \left (p + 1\right )} & \text {for}\: \left |{\frac {e^{2} x^{2}}{d^{2}}}\right | > 1 \\- \frac {0^{p} d d^{2 p - 2}}{x} - \frac {0^{p} d^{2 p - 2} e \log {\left (\frac {e^{2} x^{2}}{d^{2}} \right )}}{2} + \frac {0^{p} d^{2 p - 2} e \log {\left (1 - \frac {e^{2} x^{2}}{d^{2}} \right )}}{2} + 0^{p} d^{2 p - 2} e \operatorname {atanh}{\left (\frac {e x}{d} \right )} + \frac {d e^{2 p - 2} p x^{2 p - 3} e^{i \pi p} \Gamma \left (p\right ) \Gamma \left (\frac {3}{2} - p\right ) {{}_{2}F_{1}\left (\begin {matrix} 1 - p, \frac {3}{2} - p \\ \frac {5}{2} - p \end {matrix}\middle | {\frac {d^{2}}{e^{2} x^{2}}} \right )}}{2 \Gamma \left (\frac {5}{2} - p\right ) \Gamma \left (p + 1\right )} - \frac {e^{2 p - 1} p x^{2 p - 2} e^{i \pi p} \Gamma \left (p\right ) \Gamma \left (1 - p\right ) {{}_{2}F_{1}\left (\begin {matrix} 1 - p, 1 - p \\ 2 - p \end {matrix}\middle | {\frac {d^{2}}{e^{2} x^{2}}} \right )}}{2 \Gamma \left (2 - p\right ) \Gamma \left (p + 1\right )} & \text {otherwise} \end {cases} \]
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\[ \int \frac {\left (d^2-e^2 x^2\right )^p}{x^2 (d+e x)} \, dx=\int { \frac {{\left (-e^{2} x^{2} + d^{2}\right )}^{p}}{{\left (e x + d\right )} x^{2}} \,d x } \]
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\[ \int \frac {\left (d^2-e^2 x^2\right )^p}{x^2 (d+e x)} \, dx=\int { \frac {{\left (-e^{2} x^{2} + d^{2}\right )}^{p}}{{\left (e x + d\right )} x^{2}} \,d x } \]
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Timed out. \[ \int \frac {\left (d^2-e^2 x^2\right )^p}{x^2 (d+e x)} \, dx=\int \frac {{\left (d^2-e^2\,x^2\right )}^p}{x^2\,\left (d+e\,x\right )} \,d x \]
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