Start with the general polar vector field . Change this to Cartesian coordinates in which the expression for the divergence is known. Then restore polar coordinates.
Using the results of Example 9.2.13, the Cartesian form for F is the field
whose divergence is , where and are short notations for and , respectively. If , the quotient and product rules of differentiation lead to
The results in Table 9.3.3(a) and the chain rule lead to
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and
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Since , and . Hence, now becomes
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