In this exercise we prove that for any positive reals a1,…,an, we have limx→0(na1x+⋯+anx)1/x=(a1⋯an)1/n, or in other words that "the geometric mean is the 0th power mean". (See also here.)
Why is this an exponential indeterminate form?
Because ax→1 (as x→0) for any positive real a, we have limx→0(na1x+⋯+anx)=1.
So for x≈0, the "base" na1x+⋯+anx≈1, and the exponent 1/x is either "very positive" or "very negative" (since x is small). So we have an exponential indeterminate form 1±∞.
We could take logarithms and use l'Hopital's rule, but below we present a more instructive approach using linear approximation.
So we'll need to be more precise to evaluate the limit: for instance, by linear approximation, ax≈1+(lna)x for small x≈0 (we can worry about the error later, but it's not so important here).
Averaging the n linear approximations for a1x,…,anx gives us a more precise estimate on the "base", i.e. na1x+⋯+anx≈1+Cx, where C=nlna1+⋯+lnan is the average of the "slopes" in the approximation.
So we basically want to find limx→0(1+Cx)1/x. Recall from another exercise that the difficulty is that (1+Cx)1/x is hard to work with algebraically (it's hard to simultaneously account for the base and exponent); there are a couple standard ways to deal with this.
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For instance, we could use the classical linear vs. exponential approximation 1+Cx≈eCx (which is good when x≈0 is small), so that as x→0 we have (1+Cx)1/x≈(eCx)1/x=eC→eC.
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Alternatively, since fractions are often easier to think about the exponentials, we can take logarithms: limx→0(1+Cx)1/x=exp(limx→0xlog(1+Cx)). And we know log(1+Cx)≈Cx for small x, by linear approximation (alternatively, this is equivalent to 1+Cx≈eCx). So limx→0(1+Cx)1/x=exp(C).
Finally, eC=enlna1+⋯+lnan=(elna1+⋯+lnan)1/n=(a1⋯an)1/n, establishing the desired limit from the beginning.