Power Series Expansion for Real Area Hyperbolic Tangent
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Theorem
The (real) area hyperbolic tangent function has a Taylor series expansion:
\(\ds \artanh x\) | \(=\) | \(\ds \sum_{n \mathop = 0}^\infty \frac {x^{2 n + 1} } {2 n + 1}\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds x + \frac {x^3} 3 + \frac {x^5} 5 + \frac {x^7} 7 + \cdots\) |
for $\size x < 1$.
Proof
From Sum of Infinite Geometric Sequence:
- $(1): \quad \ds \frac 1 {1 - x^2} = \sum_{n \mathop = 0}^\infty \paren {x^2}^n$
for $-1 < x < 1$.
From Power Series is Termwise Integrable within Radius of Convergence, $(1)$ can be integrated term by term:
\(\ds \int_0^x \frac 1 {1 - t^2} \rd t\) | \(=\) | \(\ds \sum_{n \mathop = 0}^\infty \int_0^x \paren {t^2}^n \rd t\) | ||||||||||||
\(\ds \leadsto \ \ \) | \(\ds \artanh x\) | \(=\) | \(\ds \sum_{n \mathop = 0}^\infty \frac {x^{2 n + 1} } {2 n + 1}\) | Primitive of Reciprocal of $\dfrac 1 {1 - t^2}$, Integral of Power |
For $-1 < x < 1$, the sequence $\sequence {\dfrac {x^{2 n + 1} } {2 n + 1} }$ is decreasing and converges to zero.
Hence the result.
$\blacksquare$
Also see
- Power Series Expansion for Real Area Hyperbolic Sine
- Power Series Expansion for Real Area Hyperbolic Cosine
- Power Series Expansion for Real Area Hyperbolic Cotangent
- Power Series Expansion for Real Area Hyperbolic Secant
- Power Series Expansion for Real Area Hyperbolic Cosecant
Sources
- 1968: Murray R. Spiegel: Mathematical Handbook of Formulas and Tables ... (previous) ... (next): $\S 20$: Series for Hyperbolic Functions: $20.41$
- 1976: K. Weltner and W.J. Weber: Mathematics for Engineers and Scientists ... (previous) ... (next): $8$. Taylor Series and Power Series: Appendix: Table $8.2$: Power Series of Important Functions