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CHAPTER XI THE LOGARITHMIC SPIRAL

Then, if ö¡ increase by 2ü€, while r increases to rÿ£¢1ã€₤,

which leads, by subtraction to

Now, as öÝ tends to 0, k (i.e. cotã€₤öÝ) tends to ㈞, and therefore, as kã€₤㆒ã€₤㈞, log(rÿ£¢1ã€₤いã€₤r)ã€₤㆒ã€₤㈞ and also rÿ£¢1ã€₤いã€₤rã€₤㆒ã€₤㈞.

Therefore if one whorl exists, the radius vector of the other is infinite; in other words, there is nowhere, even in the near neighbourhood of the pole, a complete revolution of the spire. Our spiral shells of small constant angle, such as Dentalium, may accordingly be considered to represent sufficiently well the true commencement

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