atmos:citation:research:hail-1d_counts_to_concentration
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atmos:citation:research:hail-1d_counts_to_concentration [2024/05/14 16:02] – james.klinman | atmos:citation:research:hail-1d_counts_to_concentration [2024/05/14 16:08] – james.klinman | ||
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- | Time is at 1 hertz, and the counts are in 1-14. | + | Time is at 1 hertz, and the counts are in 1-14. The size ranges become more spread apart as the channels get larger since there are less large particles. |
Size ranges are, | Size ranges are, | ||
* 01 : 0.40 - 0.50 cm | * 01 : 0.40 - 0.50 cm | ||
Line 21: | Line 22: | ||
* 13 : 3.21 - 4.00 cm | * 13 : 3.21 - 4.00 cm | ||
* 14 : 4.00 - 5.00 cm | * 14 : 4.00 - 5.00 cm | ||
- | The size ranges become more spread apart as the channels get larger since there are less large particles. | + | |
+ | |||
+ | With the counts, concentration can be calculated. | ||
+ | |||
+ | Conc (#/m^4) = Counts / (SA * Airspeed * Binsize change) | ||
+ | |||
+ | Where, | ||
+ | * SA is sample area which is (probe arm length * height) | ||
+ | * Height is (number of diodes * diode size) | ||
+ | * Binsize change is the (Max_Size - Min_Size) for each channel. | ||
+ | * For channel 1, this would be 0.50 - 0.40 = 0.10 |
atmos/citation/research/hail-1d_counts_to_concentration.txt · Last modified: 2024/05/14 16:55 by james.klinman