Integrand size = 27, antiderivative size = 163 \[ \int \frac {(g x)^m \left (d^2-e^2 x^2\right )^p}{d+e x} \, dx=\frac {(g x)^{1+m} \left (d^2-e^2 x^2\right )^p \left (1-\frac {e^2 x^2}{d^2}\right )^{-p} \operatorname {Hypergeometric2F1}\left (\frac {1+m}{2},1-p,\frac {3+m}{2},\frac {e^2 x^2}{d^2}\right )}{d g (1+m)}-\frac {e (g x)^{2+m} \left (d^2-e^2 x^2\right )^p \left (1-\frac {e^2 x^2}{d^2}\right )^{-p} \operatorname {Hypergeometric2F1}\left (\frac {2+m}{2},1-p,\frac {4+m}{2},\frac {e^2 x^2}{d^2}\right )}{d^2 g^2 (2+m)} \]
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Time = 0.10 (sec) , antiderivative size = 163, normalized size of antiderivative = 1.00, number of steps used = 8, number of rules used = 5, \(\frac {\text {number of rules}}{\text {integrand size}}\) = 0.185, Rules used = {906, 83, 127, 372, 371} \[ \int \frac {(g x)^m \left (d^2-e^2 x^2\right )^p}{d+e x} \, dx=\frac {(g x)^{m+1} \left (d^2-e^2 x^2\right )^p \left (1-\frac {e^2 x^2}{d^2}\right )^{-p} \operatorname {Hypergeometric2F1}\left (\frac {m+1}{2},1-p,\frac {m+3}{2},\frac {e^2 x^2}{d^2}\right )}{d g (m+1)}-\frac {e (g x)^{m+2} \left (d^2-e^2 x^2\right )^p \left (1-\frac {e^2 x^2}{d^2}\right )^{-p} \operatorname {Hypergeometric2F1}\left (\frac {m+2}{2},1-p,\frac {m+4}{2},\frac {e^2 x^2}{d^2}\right )}{d^2 g^2 (m+2)} \]
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Rule 83
Rule 127
Rule 371
Rule 372
Rule 906
Rubi steps \begin{align*} \text {integral}& = \left ((d-e x)^{-p} (d+e x)^{-p} \left (d^2-e^2 x^2\right )^p\right ) \int (g x)^m (d-e x)^p (d+e x)^{-1+p} \, dx \\ & = \left (d (d-e x)^{-p} (d+e x)^{-p} \left (d^2-e^2 x^2\right )^p\right ) \int (g x)^m (d-e x)^{-1+p} (d+e x)^{-1+p} \, dx-\frac {\left (e (d-e x)^{-p} (d+e x)^{-p} \left (d^2-e^2 x^2\right )^p\right ) \int (g x)^{1+m} (d-e x)^{-1+p} (d+e x)^{-1+p} \, dx}{g} \\ & = d \int (g x)^m \left (d^2-e^2 x^2\right )^{-1+p} \, dx-\frac {e \int (g x)^{1+m} \left (d^2-e^2 x^2\right )^{-1+p} \, dx}{g} \\ & = \frac {\left (\left (d^2-e^2 x^2\right )^p \left (1-\frac {e^2 x^2}{d^2}\right )^{-p}\right ) \int (g x)^m \left (1-\frac {e^2 x^2}{d^2}\right )^{-1+p} \, dx}{d}-\frac {\left (e \left (d^2-e^2 x^2\right )^p \left (1-\frac {e^2 x^2}{d^2}\right )^{-p}\right ) \int (g x)^{1+m} \left (1-\frac {e^2 x^2}{d^2}\right )^{-1+p} \, dx}{d^2 g} \\ & = \frac {(g x)^{1+m} \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+m}{2},1-p;\frac {3+m}{2};\frac {e^2 x^2}{d^2}\right )}{d g (1+m)}-\frac {e (g x)^{2+m} \left (d^2-e^2 x^2\right )^p \left (1-\frac {e^2 x^2}{d^2}\right )^{-p} \, _2F_1\left (\frac {2+m}{2},1-p;\frac {4+m}{2};\frac {e^2 x^2}{d^2}\right )}{d^2 g^2 (2+m)} \\ \end{align*}
Time = 0.13 (sec) , antiderivative size = 124, normalized size of antiderivative = 0.76 \[ \int \frac {(g x)^m \left (d^2-e^2 x^2\right )^p}{d+e x} \, dx=\frac {x (g x)^m \left (d^2-e^2 x^2\right )^p \left (1-\frac {e^2 x^2}{d^2}\right )^{-p} \left (-e (1+m) x \operatorname {Hypergeometric2F1}\left (1+\frac {m}{2},1-p,2+\frac {m}{2},\frac {e^2 x^2}{d^2}\right )+d (2+m) \operatorname {Hypergeometric2F1}\left (\frac {1+m}{2},1-p,\frac {3+m}{2},\frac {e^2 x^2}{d^2}\right )\right )}{d^2 (1+m) (2+m)} \]
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\[\int \frac {\left (g x \right )^{m} \left (-e^{2} x^{2}+d^{2}\right )^{p}}{e x +d}d x\]
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\[ \int \frac {(g x)^m \left (d^2-e^2 x^2\right )^p}{d+e x} \, dx=\int { \frac {{\left (-e^{2} x^{2} + d^{2}\right )}^{p} \left (g x\right )^{m}}{e x + d} \,d x } \]
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Result contains complex when optimal does not.
Time = 5.23 (sec) , antiderivative size = 372, normalized size of antiderivative = 2.28 \[ \int \frac {(g x)^m \left (d^2-e^2 x^2\right )^p}{d+e x} \, dx=- \frac {0^{p} d^{1 - m} d^{m + 2 p} e^{- m - 1} e^{m - 1} g^{m} m x^{m - 1} \Phi \left (\frac {d^{2}}{e^{2} x^{2}}, 1, \frac {1}{2} - \frac {m}{2}\right ) \Gamma \left (\frac {1}{2} - \frac {m}{2}\right )}{4 \Gamma \left (\frac {3}{2} - \frac {m}{2}\right )} + \frac {0^{p} d^{1 - m} d^{m + 2 p} e^{- m - 1} e^{m - 1} g^{m} x^{m - 1} \Phi \left (\frac {d^{2}}{e^{2} x^{2}}, 1, \frac {1}{2} - \frac {m}{2}\right ) \Gamma \left (\frac {1}{2} - \frac {m}{2}\right )}{4 \Gamma \left (\frac {3}{2} - \frac {m}{2}\right )} + \frac {0^{p} d^{- m} d^{m + 2 p} e^{m} e^{- m - 1} g^{m} m x^{m} \Phi \left (\frac {d^{2}}{e^{2} x^{2}}, 1, \frac {m e^{i \pi }}{2}\right ) \Gamma \left (- \frac {m}{2}\right )}{4 \Gamma \left (1 - \frac {m}{2}\right )} + \frac {d e^{2 p - 2} g^{m} p x^{m + 2 p - 1} e^{i \pi p} \Gamma \left (p\right ) \Gamma \left (- \frac {m}{2} - p + \frac {1}{2}\right ) {{}_{2}F_{1}\left (\begin {matrix} 1 - p, - \frac {m}{2} - p + \frac {1}{2} \\ - \frac {m}{2} - p + \frac {3}{2} \end {matrix}\middle | {\frac {d^{2}}{e^{2} x^{2}}} \right )}}{2 \Gamma \left (p + 1\right ) \Gamma \left (- \frac {m}{2} - p + \frac {3}{2}\right )} - \frac {e^{2 p - 1} g^{m} p x^{m + 2 p} e^{i \pi p} \Gamma \left (p\right ) \Gamma \left (- \frac {m}{2} - p\right ) {{}_{2}F_{1}\left (\begin {matrix} 1 - p, - \frac {m}{2} - p \\ - \frac {m}{2} - p + 1 \end {matrix}\middle | {\frac {d^{2}}{e^{2} x^{2}}} \right )}}{2 \Gamma \left (p + 1\right ) \Gamma \left (- \frac {m}{2} - p + 1\right )} \]
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\[ \int \frac {(g x)^m \left (d^2-e^2 x^2\right )^p}{d+e x} \, dx=\int { \frac {{\left (-e^{2} x^{2} + d^{2}\right )}^{p} \left (g x\right )^{m}}{e x + d} \,d x } \]
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\[ \int \frac {(g x)^m \left (d^2-e^2 x^2\right )^p}{d+e x} \, dx=\int { \frac {{\left (-e^{2} x^{2} + d^{2}\right )}^{p} \left (g x\right )^{m}}{e x + d} \,d x } \]
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Timed out. \[ \int \frac {(g x)^m \left (d^2-e^2 x^2\right )^p}{d+e x} \, dx=\int \frac {{\left (d^2-e^2\,x^2\right )}^p\,{\left (g\,x\right )}^m}{d+e\,x} \,d x \]
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