the Creative Commons Attribution 4.0 License.
the Creative Commons Attribution 4.0 License.
Technical note: Transit time distributions are not L-shaped
Abstract. A probability density function f(t) with origin at t = 0 is defined here as being "L-shaped" if f'(t) ≤ 0 for t ≥ 0. L-shaped probability density functions, especially exponential distributions, are often assumed as transit time distributions in hydrological studies. However, L-shaped transit time distributions are not possible. This is because the transit time of a particle must always be with reference to a store, the transit time being some finite duration of time between particle entry and exit. Tracer particles cannot transit through any part of a store in zero time so transit time distributions have the property f(0) = 0, which is incompatible with L-shaped probability density functions. This is a fundamental constraint on the form of transit time distributions, which must possess at least one mode at t > 0. Some L-shaped probability density functions may well approximate actual transit time distributions, but they are of different form to the true distributions. A call is therefore made for L-shaped probability density functions to be no longer employed in transit time modelling.
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RC1: 'modeling transit time distributions', Anonymous Referee #1, 02 Sep 2017
- AC1: 'Reply to referee #1', Earl Bardsley, 03 Sep 2017
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RC2: 'Transit Time Distributions have zero Density at Time Zero - Is this New?', Anonymous Referee #2, 07 Sep 2017
- AC2: 'Reply to Referee #2', Earl Bardsley, 08 Sep 2017
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RC3: '"Missing the point" for probability density functions', Anonymous Referee #3, 18 Sep 2017
- AC3: 'Reply to referee #3', Earl Bardsley, 20 Sep 2017
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RC4: 'Review of “Transit time distributions are no L-shaped,” by Earl Bardsley', Anonymous Referee #4, 19 Sep 2017
- AC4: 'Reply to referee #4', Earl Bardsley, 08 Oct 2017
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RC5: 'Interactive comment on „Technical note: Transit time distributions are not L-shaped“ by Earl Bradley', Anonymous Referee #5, 28 Sep 2017
- AC5: 'Reply to referee #5', Earl Bardsley, 08 Oct 2017
- AC6: 'Concluding reply to referees #4 and #5', Earl Bardsley, 10 Oct 2017
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SC1: 'The zero-time-to-peak characteristic of a probability density function', John Ding, 28 Sep 2017
- AC7: 'Reply', Earl Bardsley, 10 Oct 2017
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SC2: 'An arbitrary definition with no physical or mathematical implications', James Kirchner, 11 Oct 2017
- AC8: 'Acknowledgement', Earl Bardsley, 11 Oct 2017
- AC9: 'Reply to J Kirchner', Earl Bardsley, 14 Oct 2017
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RC1: 'modeling transit time distributions', Anonymous Referee #1, 02 Sep 2017
- AC1: 'Reply to referee #1', Earl Bardsley, 03 Sep 2017
-
RC2: 'Transit Time Distributions have zero Density at Time Zero - Is this New?', Anonymous Referee #2, 07 Sep 2017
- AC2: 'Reply to Referee #2', Earl Bardsley, 08 Sep 2017
-
RC3: '"Missing the point" for probability density functions', Anonymous Referee #3, 18 Sep 2017
- AC3: 'Reply to referee #3', Earl Bardsley, 20 Sep 2017
-
RC4: 'Review of “Transit time distributions are no L-shaped,” by Earl Bardsley', Anonymous Referee #4, 19 Sep 2017
- AC4: 'Reply to referee #4', Earl Bardsley, 08 Oct 2017
-
RC5: 'Interactive comment on „Technical note: Transit time distributions are not L-shaped“ by Earl Bradley', Anonymous Referee #5, 28 Sep 2017
- AC5: 'Reply to referee #5', Earl Bardsley, 08 Oct 2017
- AC6: 'Concluding reply to referees #4 and #5', Earl Bardsley, 10 Oct 2017
-
SC1: 'The zero-time-to-peak characteristic of a probability density function', John Ding, 28 Sep 2017
- AC7: 'Reply', Earl Bardsley, 10 Oct 2017
-
SC2: 'An arbitrary definition with no physical or mathematical implications', James Kirchner, 11 Oct 2017
- AC8: 'Acknowledgement', Earl Bardsley, 11 Oct 2017
- AC9: 'Reply to J Kirchner', Earl Bardsley, 14 Oct 2017
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