Integrand size = 23, antiderivative size = 41 \[ \int \frac {\left (1-\frac {e^2 x^2}{d^2}\right )^p}{d+e x} \, dx=\frac {2^p \left (\frac {d+e x}{d}\right )^p \operatorname {Hypergeometric2F1}\left (-p,p,1+p,\frac {d+e x}{2 d}\right )}{e p} \]
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Time = 0.03 (sec) , antiderivative size = 54, normalized size of antiderivative = 1.32, number of steps used = 2, number of rules used = 2, \(\frac {\text {number of rules}}{\text {integrand size}}\) = 0.087, Rules used = {690, 71} \[ \int \frac {\left (1-\frac {e^2 x^2}{d^2}\right )^p}{d+e x} \, dx=-\frac {2^{p-1} \left (\frac {d-e x}{d}\right )^{p+1} \operatorname {Hypergeometric2F1}\left (1-p,p+1,p+2,\frac {d-e x}{2 d}\right )}{e (p+1)} \]
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Rule 71
Rule 690
Rubi steps \begin{align*} \text {integral}& = \frac {\left (\left (\frac {d-e x}{d}\right )^{1+p} \left (\frac {1}{d}-\frac {e x}{d^2}\right )^{-1-p}\right ) \int \left (\frac {1}{d}-\frac {e x}{d^2}\right )^p \left (1+\frac {e x}{d}\right )^{-1+p} \, dx}{d^2} \\ & = -\frac {2^{-1+p} \left (\frac {d-e x}{d}\right )^{1+p} \, _2F_1\left (1-p,1+p;2+p;\frac {d-e x}{2 d}\right )}{e (1+p)} \\ \end{align*}
Time = 0.34 (sec) , antiderivative size = 76, normalized size of antiderivative = 1.85 \[ \int \frac {\left (1-\frac {e^2 x^2}{d^2}\right )^p}{d+e x} \, dx=-\frac {2^{-1+p} (d-e x) \left (1+\frac {e x}{d}\right )^{-p} \left (1-\frac {e^2 x^2}{d^2}\right )^p \operatorname {Hypergeometric2F1}\left (1-p,1+p,2+p,\frac {d-e x}{2 d}\right )}{d e (1+p)} \]
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\[\int \frac {\left (1-\frac {e^{2} x^{2}}{d^{2}}\right )^{p}}{e x +d}d x\]
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\[ \int \frac {\left (1-\frac {e^2 x^2}{d^2}\right )^p}{d+e x} \, dx=\int { \frac {{\left (-\frac {e^{2} x^{2}}{d^{2}} + 1\right )}^{p}}{e x + d} \,d x } \]
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Result contains complex when optimal does not.
Time = 3.29 (sec) , antiderivative size = 318, normalized size of antiderivative = 7.76 \[ \int \frac {\left (1-\frac {e^2 x^2}{d^2}\right )^p}{d+e x} \, dx=\begin {cases} \frac {0^{p} \log {\left (-1 + \frac {e^{2} x^{2}}{d^{2}} \right )}}{2 e} + \frac {0^{p} \operatorname {acoth}{\left (\frac {e x}{d} \right )}}{e} + \frac {d^{1 - 2 p} e^{2 p - 2} p x^{2 p - 1} e^{i \pi p} \Gamma \left (p\right ) \Gamma \left (\frac {1}{2} - p\right ) {{}_{2}F_{1}\left (\begin {matrix} 1 - p, \frac {1}{2} - p \\ \frac {3}{2} - p \end {matrix}\middle | {\frac {d^{2}}{e^{2} x^{2}}} \right )}}{2 \Gamma \left (\frac {3}{2} - p\right ) \Gamma \left (p + 1\right )} + \frac {e x^{2} \Gamma \left (p\right ) \Gamma \left (1 - p\right ) {{}_{3}F_{2}\left (\begin {matrix} 2, 1, 1 - p \\ 2, 2 \end {matrix}\middle | {\frac {e^{2} x^{2} e^{2 i \pi }}{d^{2}}} \right )}}{2 d^{2} \Gamma \left (- p\right ) \Gamma \left (p + 1\right )} & \text {for}\: \left |{\frac {e^{2} x^{2}}{d^{2}}}\right | > 1 \\\frac {0^{p} \log {\left (1 - \frac {e^{2} x^{2}}{d^{2}} \right )}}{2 e} + \frac {0^{p} \operatorname {atanh}{\left (\frac {e x}{d} \right )}}{e} + \frac {d^{1 - 2 p} e^{2 p - 2} p x^{2 p - 1} e^{i \pi p} \Gamma \left (p\right ) \Gamma \left (\frac {1}{2} - p\right ) {{}_{2}F_{1}\left (\begin {matrix} 1 - p, \frac {1}{2} - p \\ \frac {3}{2} - p \end {matrix}\middle | {\frac {d^{2}}{e^{2} x^{2}}} \right )}}{2 \Gamma \left (\frac {3}{2} - p\right ) \Gamma \left (p + 1\right )} + \frac {e x^{2} \Gamma \left (p\right ) \Gamma \left (1 - p\right ) {{}_{3}F_{2}\left (\begin {matrix} 2, 1, 1 - p \\ 2, 2 \end {matrix}\middle | {\frac {e^{2} x^{2} e^{2 i \pi }}{d^{2}}} \right )}}{2 d^{2} \Gamma \left (- p\right ) \Gamma \left (p + 1\right )} & \text {otherwise} \end {cases} \]
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\[ \int \frac {\left (1-\frac {e^2 x^2}{d^2}\right )^p}{d+e x} \, dx=\int { \frac {{\left (-\frac {e^{2} x^{2}}{d^{2}} + 1\right )}^{p}}{e x + d} \,d x } \]
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\[ \int \frac {\left (1-\frac {e^2 x^2}{d^2}\right )^p}{d+e x} \, dx=\int { \frac {{\left (-\frac {e^{2} x^{2}}{d^{2}} + 1\right )}^{p}}{e x + d} \,d x } \]
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Timed out. \[ \int \frac {\left (1-\frac {e^2 x^2}{d^2}\right )^p}{d+e x} \, dx=\int \frac {{\left (1-\frac {e^2\,x^2}{d^2}\right )}^p}{d+e\,x} \,d x \]
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