Half time (physics)
The half time is the time taken by a quantity to reach one half of its extremal value, where the rate of change is proportional to the difference between the present value and the extremal value (i.e. in exponential decay processes). It is synonymous with half-life, but used in slightly different contexts.
The diagram shows the increase in the quantity (red) in response to a step-change in the motive force that changes it (blue). The time-axis is in multiples of the half time. It can be seen that the quantity increases to one-half of its final value after one half time, to three-quarters after two half times, to seven-eighths after three half times, and so on.
The relationship between the quantity (Q) and time (t) is described by the mathematical formula:
where Qf is the extremal value and λ is a constant, approximately equal to 0.69 divided by the half time – more precisely: loge(2) / (half time).
Where the quantity decreases in response to a step-decrease in the motive force that changes it, the curve is mirrored in the time-axis and may be referred to as exponential decay.
The concept of half time is used in diving physiology where body tissues take up and release inert gases (usually nitrogen) following changes in depth. Different tissue types have different half times for a given inert gas, and modelling the uptake and release of gases by the tissues is important to avoid decompression sickness.
- capacitor is charged or discharged via a resistor, the voltage on the capacitor follows the above formula, with the half time approximately equal to 0.69 times the time constant, which is equal to the product of the resistance and the capacitance.
- The first models of nitrogen uptake and release in the body of a diver used five parallel compartments with half times from 5 minutes to 75 minutes. Later models refined this by considering more compartments and a wider range of half times. The U.S. Navy tables used six compartments with half times of 5, 10, 20, 40, 80 and 120 minutes. The Bühlmann tables use twelve of the sixteen compartments in the ZH-L16 algorithm, which uses half times from 4 to 635 minutes.
- Tikuisis, Peter; Gerth, Wayne A. (2003). "10.1: Decompression Theory". In Brubakk, Alf O; Neuman, Tom S. Bennett and Elliott's physiology and medicine of diving, 5th Revised edition. United States: Saunders Ltd. p. 439. ISBN 0-7020-2571-2. OCLC 51607923.
- Boycott A. E., Damant G. C. C., Haldane John Scott (1908). "Prevention of compressed air illness". Journal of Hygiene. 8 (3): 342–443. doi:10.1017/S0022172400003399. PMC . PMID 20474365. Retrieved 2009-06-15.
- Lippmann, John; Mitchell, Simon J (October 2005). "15". Deeper into Diving (2 ed.). Victoria, Australia: J.L. Publications. p. 215. ISBN 0-9752290-1-X. OCLC 66524750.
- des Granges, M (1957). "Standard Air Decompression Table". United States Navy Experimental Diving Unit Technical Report. NEDU-RR-5-57. Retrieved 2009-06-15.
- Lippmann, John; Mitchell, Simon (October 2005). "17". Deeper into Diving (2 ed.). Victoria, Australia: J.L. Publications. p. 226. ISBN 0-9752290-1-X. OCLC 66524750.
- Bühlmann, Albert A. (1984). Decompression-Decompression Sickness. Berlin New York: Springer-Verlag. ISBN 0-387-13308-9.