Ozone Library
Half-life of Ozone
The half-life of ozone refers to the amount of time required for half of a given quantity of ozone to decay into oxygen. Ozone is an unstable gas and readily decomposes into oxygen. Therefore, the half-life of ozone is an essential factor to consider when determining its effectiveness in various applications.
Typical Gaseous Ozone Half-life time as a Function of Temperature
Half-life time | Temp |
---|---|
∼ 3 months | -50 ºC |
∼ 18 days | -35 ºC |
∼ 8 days | -25 ºC |
∼ 3 days | 20 ºC |
∼ 1.5 hours days | 120 ºC |
∼ 1.5 seconds | 250 ºC |
Typical Dissolved in Water Ozone (PH=7) Half-life time as a Function of Temperature
Half-life time | Temp |
---|---|
∼ 30 minutes | 15 ºC |
∼ 20 minutes | 20 ºC |
∼ 15 minutes | 25 ºC |
∼ 12 minutes | 30 ºC |
∼ 8 minutes | 35 ºC |
CHANGES IN OZONE OVER TIME
1. General equation
The equation that describes the temporal evolution of the ozone concentration has the following form:
dn/dt = −kn² + q (1)
Where t is the time, k is the reaction rate constant, which is independent of concentration but probably, depends on the temperature, and n is the concentration (number of the molecules per unit volume):
n= (M /μV)* NA (2)
μ is the molar weight of ozone, M is the mass of ozone inside the volume, V, in a given moment of time, NA is the Avogadro number
In Eq.(1), is the number of molecules delivered per unit of time into the volume and calculated per unit volume:
q= (m/μV) NA (3)
Where m is the mass of ozone delivered into volume, V, per unit of time.
2. Closed volume
Consider the case of q = 0. For such a case, integration of Eq. (1) yields
n= (no/1+no k t) (4)
where is the initial concentration. Using (2):
no = (Mo/ μV)* NA (5)
Where M0 is the initial mass of ozone. Eq.(4) can be rewritten as
n= no/ (1 + t / τ) (6)
where we introduced the time scale parameter τ: when t =τ, the concentration of molecules (and the mass of ozone, for a given volume) decreases by a factor of two. See Eq.(6). Comparing Eqs. (4) and (6) one obtains:
τ= 1 / no k (7)
Since k is independent of the concentration, we arrive at an important conclusion: the parameter τ depends on the initial concentration and, for a given volume and pressure, on the initial mass, M0.
τ= (μ / (NA Mo k) = k1 / Mo (8)
Stationary regime
Inspecting Eq.(1), one can conclude that the concentration does not change when
q = kn² (9)
When Eq.(9) is satisfied, the rate of concentration changes, dn/dt, becomes zero, see Eq.(1). Realizing that the concentration is maintained to be constant in time, i.e., and using Eqs. (7) we obtain from (9) that
q = no / τ (10)
Using Eqs. (3) and (5) one can rewrite (10) in terms of mass
m = Mo / τ (11)
Conclusion
Thus, to maintain a given mass of ozone, M0, within a fixed volume at a given temperature, one should deliver ozone with the rate (mass per unit time) given by Eq.(11). The time scale parameter m τ on the right-hand side of (11) is determined from an independent experiment. This experiment is to observe a decrease in the ozone mass with time in the same closed volume. The parameter τ coincides with the time corresponding to the ozone mass. It should be stressed that, for a given volume and temperature, the measured value of 0 M M= / 2 τ is strictly linked to the initial mass of ozone M0, which should be common for both experiments.