Abstract
Discussion and debate on the application of Allen’s arc elasticity has continued into the 21st century. This note demonstrates three points. First, perceived differences between Allen’s geometric mean elasticity and a constant demand elasticity based on an assumed isoelastic demand curve are negligible for small changes in price and quantity, which comprise the vast majority of such changes. Second, in some cases of rapid security or commodity price movements, the harmonic mean may provide the most accurate elasticity estimates across measures of central tendency. Third, because the arithmetic and harmonic means serve as bounds for the geometric mean, an elasticity based on the geometric mean may be considered a prudent choice among these three on this basis alone.
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Notes
Phillips (1994, Daellenbach 319) notes the similarity in the results between the two approaches for small changes in price, but asserts that an argument for isoelastic demand curves “is referenced here only for comparison purposes.” Apart from the debate, Vázquez (1995) formulates a measure of arc elasticity that is in line with the characteristics of point elasticity and Haque (2005) shows the potential of using arithmetic means to approximate harmonic means in the computation of elasticity.
When p U diverges toward infinity, we can divide both numerator and denominator by p U and take the limit. We find that the \( \lim \left[ {{{{2{p_U}{p_L}}} \left/ {{\left( {{p_U} + {p_L}} \right)}} \right.}} \right] = \lim \left[ {{{{2{p_L}}} \left/ {{(1 + {{{{p_L}}} \left/ {{{p_U}}} \right.})}} \right.}} \right] = 2{p_L} \). In contrast, both the arithmetic and geometric means are undefined in this situation.
The result is \( {\left( {{{{dq}} \left/ {{dp}} \right.}} \right)^2}\left( {{{{\overline{p}_G^2}} \left/ {{\overline{q}_G^2}} \right.}} \right) = \left( {{{{dq}} \left/ {{dp}} \right.}} \right)\left( {{{{{{\overline{p}}_A}{{\overline{p}}_H}}} \left/ {{{{\overline{q}}_A}{{\overline{q}}_H}}} \right.}} \right)\left( {{{{dq}} \left/ {{dp}} \right.}} \right) \). However, the fact that \( \eta_G^2 = {\eta_A} \cdot {\eta_H} \) does not imply that the absolute values of the elasticity measures follow the order of \( {\eta_A} > {\eta_G} > {\eta_H} \). That is, although the geometric mean price and quantity values are bounded by the arithmetic and harmonic means, their respective ratios (e.g.,\( {{{{{\overline{p}}_A}}} \left/ {{{{\overline{q}}_A}}} \right.} \)) need not follow this order.
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Appendix
Appendix
To expand Eq. (3), first note that:
This reduces to the following:
Expanding \( {\left( {1 + r} \right)^{{ - 0.5}}} \) of Eq. (4) around \( \overline{r} = 0 \) readily yields:
Subtracting (2A) from (lA) gives rise to the difference in the percent change in quantity, or the numerators of \( {\eta_G} \)and \( {\eta_{{iso}}} \) , as follows:
By exactly the same procedure, the difference in the percent change in price, or the numerators of \( {\eta_G} \) and \( {\eta_{{iso}}} \) , is as follows (where s is a small percent):
Eqs. (3A) and (4A) represent alternating series for small r and s values which are of negligible magnitudes.
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Yang, C.W., Loviscek, A.L., Cheng, H.W. et al. A Note on Allen’s Arc Elasticity with Arithmetic, Geometric and Harmonic Means. Atl Econ J 40, 161–171 (2012). https://doi.org/10.1007/s11293-012-9315-5
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DOI: https://doi.org/10.1007/s11293-012-9315-5