Help showing bound for magnitude of complex log fcn

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The discussion centers on proving the bound for the magnitude of the complex logarithm function, specifically for the expression |log(1 - 1/L^s)| ≤ L^(-σ) with s defined as σ + it and σ > 1. The approach begins with the Taylor series expansion of log(1 - z) for |z| < 1, leading to the formulation |log(1 - 1/L^s)| = | -∑(L^(-js)/j)|. The series converges, allowing the inequality |log(1 - 1/L^s)| to be expressed as a sum that can be bounded by ∑(L^(-jσ)/j). The context of L approaching infinity is crucial for establishing the validity of the bound. This analysis provides a pathway to demonstrate the desired inequality effectively.
benorin
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I'm working through an example problem wherein this bound is used:

\left| \log \left( 1-\frac{1}{L^s}\right) \right| \leq L^{-\sigma},

where s:=\sigma +it and it is known that \sigma &gt;1. How do I prove this? Should I assume the principle brach is taken?
 
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It is perhaps important to note that in the context, L\rightarrow\infty

I think I got a start:

For \left| z\right| &lt;1, the Taylor series about z=0 is

\log (1-z)=-\sum_{j=1}^{\infty}\frac{z^j}{j}

so that

\left| \log \left( 1-\frac{1}{L^s}\right) \right| =\left| -\sum_{j=1}^{\infty}\frac{L^{-js}}{j} \right| \leq \sum_{j=1}^{\infty}\left| \frac{L^{-js}}{j}\right| = \sum_{j=1}^{\infty} \frac{L^{-j\sigma}}{j}
 
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Question: A clock's minute hand has length 4 and its hour hand has length 3. What is the distance between the tips at the moment when it is increasing most rapidly?(Putnam Exam Question) Answer: Making assumption that both the hands moves at constant angular velocities, the answer is ## \sqrt{7} .## But don't you think this assumption is somewhat doubtful and wrong?

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