During stable nighttime conditions, in the absence of a frontal weather system and with cool, calm, cloud- and mist-free conditions, air temperature decreases continually reaching a minimum at around sunrise. For such conditions, Parton and Logan (1981) used a three-parameter model assuming that the air temperature T(t) (°C) at any time t (h) during the daytime can be determined from measurements of the daily maximum T
x (°C) and minimum T
n (°C) temperatures with nighttime temperatures determined using:
$$ T(t)={T}_{\mathrm{n}}+\left({T}_{\mathrm{ss}}-{T}_{\mathrm{n}}\right) \exp \left[\frac{-b\ \left(t-{t}_{\mathrm{ss}}\right)}{24-D}\right] $$
(1)
for time t before midnight where T
ss (°C) is the air temperature at sunset, denoted time t
ss (h), b = 2.2 is an empirically determined constant for air temperature measured about 1.5 m above ground, D (h) the day length for the site for the current day and 24 − D the night length. For times t after midnight, the period since sunset, t − t
ss, is replaced by t + 24 − t
ss. In Eq. (1), for the case of air temperature, the time lag between the minimum air temperature and that at sunrise has been ignored. Parton and Logan (1981) found this lag to be −0.17 h for air temperatures at a height of 1.5 m and −0.18 h at 0.1 m—that is, the minimum air temperatures occurred about 10 min before sunrise. Their sensitivity analysis showed that changes to this lag time resulted in only small increases in the air temperature estimation error. They further assumed that the daytime variation in air temperature is described by a truncated sine function:
$$ T(t)={T}_{\mathrm{n}}+\left({T}_{\mathrm{x}}-{T}_{\mathrm{n}}\right) \sin \left[\frac{\pi\ \left(t-{t}_{\mathrm{sr}}\right)}{D+2a}\right] $$
(2)
where t
sr is the sunrise time, and the time offset a (h), which has an approximate value of 1.86 h, is an empirically determined constant. The sunset temperature T
ss in Eq. (1) is estimated from T
n, T
x, D and a using Eq. (2):
$$ {T}_{\mathrm{ss}}={T}_{\mathrm{n}}+\left({T}_{\mathrm{x}}-{T}_{\mathrm{n}}\right) \sin \left(\frac{\pi\ D}{D+2a}\right). $$
(3)
For the square root model for nighttime air temperatures 2 h after sunset:
$$ T(t)=T\left({t}_{\mathrm{ss}+2}\right)-c\ \sqrt{t-{t}_{\mathrm{ss}+2}} $$
(4)
for t before midnight where T(t
ss + 2) is the measured air temperature at t
ss + 2, 2 h after sunset, c (°C h-0.5) is an empirically determined constant and t − t
ss + 2 is the duration between t and 2 h after sunset. In Eqs. (1) and (4), for times after midnight, t − t
ss + 2 is replaced by t + 24 − t
ss + 2. By rearrangement of Eq. (4), the constant c for the period between t
ss + 2 and t
sr may be determined from the (predicted) nowcasted air temperature minimum (T
pn) and the measured air temperature T(t
ss + 2):
$$ c=\left[{T}_{\mathrm{pn}}-T\left({t}_{\mathrm{ss}+2}\right)\right]/\sqrt{t_{\mathrm{sr}}+24-{t}_{\mathrm{ss}+2}} $$
(5)
where, for times t
ss + 2 before midnight, t
sr + 24 − t
ss + 2 is the period 2 h after sunset and before sunrise. The method is restricted to the period between 2 h after sunset t
ss + 2 and sunrise t
sr since the net irradiance is relatively constant between these two times (Snyder and de Melo-Abreu 2005).
Four nowcasting models were tested for estimating the minimum air/grass/grass-surface temperature, 2 and 4 h before sunrise, based on sub-hourly temperature measurements between 4 and 2 h before sunrise for the 2-h nowcast and between 6 and 4 h before sunrise for the 4-h nowcast:
-
Model 1:
by inverting the exponential decay function (Eq. (1)) to solve for T
n
-
Model 2:
by application of model 1 using b = 2.2
-
Model 3:
by application of the square root function based on temperature measurements 4 h before sunrise (Eq. 4)
-
Model 4:
by application of model 3 based on temperature measurements 2 h before sunrise.
These methods, applied in real-time either in a datalogger or in near real-time using a web-based system, may allow timely nowcasting of the minimum temperature based on sub-hourly temperature measurements. For this purpose, the nighttime exponential equation (Eq. (1)) was inverted and solved for T
n so as to nowcast the minimum temperature T
pn:
$$ {T}_{\mathrm{pn}}=\left\{T(t)-{T}_{\mathrm{ss}} \exp \left[\frac{-b\ \left(t-{t}_{\mathrm{ss}}\right)}{24-D}\right]\right\}/\left\{1- \exp \left[\frac{-b\ \left(t-{t}_{\mathrm{ss}}\right)}{24-D}\right]\right\} $$
(6)
given, as an input, the measurement of temperature at time t, T(t), after midnight where:
$$ b=-\left(\frac{24-D}{t-{t}_{\mathrm{ss}}}\right) \ln \left[\frac{T(t)-{T}_{\mathrm{n}}}{T_{\mathrm{ss}}-{T}_{\mathrm{n}}}\right]. $$
(7)
For sub-hourly diurnal temperature data, which include the minimum air temperature, regressing ln [T(t) − T
n] as a function of (t − t
ss)/(24 − D) was assumed to yield a straight line with a slope of −b. For nowcasting, the empirical constant b may be determined, during several calm and cloud-free nights, several days preceding the calculation of T
pn. Clouds and/or mist or rainfall and/or increased wind speed a few hours before sunrise could reverse or hinder the nighttime rate of air temperature decrease. A reversal of the expected temperature decrease for some of the time during the night could result in b < 0 and possibly an unreliable nowcast. Conversely, for the assumed b value, more rapid than expected temperature decreases could result in T
pn greater than T
n. Changes in atmospheric conditions from one night to another could also result in different b values and therefore reduce the accuracy of the method.
In this study, the inversion of the exponential and the square root models, applied to the expected nighttime decrease in temperature (Eqs. (1) and (4)), is investigated. It is proposed that the methods be used to routinely nowcast the minimum temperature, given real-time measurement inputs of air/grass/grass-surface temperature 6 to 4 h (4-h nowcast) and 4 to 2 h (2-h nowcast) prior to the occurrence of the minimum temperature.
Generalising the nighttime exponential model (Eqs. (1) and (6)) to two measured temperatures T(t
1) and T(t
2) instead of T(t) and T
ss, where T(t
2) is a measured temperature at a later time t
2 than temperature T(t
1), with the two times several hours apart:
$$ {T}_{\mathrm{pn}}=\left\{T\left({t}_2\right)-T\left({t}_1\right) \exp \left[\frac{-b\ \left({t}_2-{t}_1\right)}{t_{\mathrm{sr}}-{t}_1}\right]\right\}/\left\{1- \exp \left[\frac{-b\ \left({t}_2-{t}_1\right)}{t_{\mathrm{sr}}-{t}_1}\right]\right\} $$
(8)
if times t
1 and t
2 are both before midnight or both after midnight. If t
1 is before midnight and t
2 after midnight, then
$$ {T}_{\mathrm{pn}}=\left\{T\left({t}_2\right)-T\left({t}_1\right) \exp \left[\frac{-b\ \left({t}_2+24-{t}_1\right)}{t_{\mathrm{sr}}+24-{t}_1}\right]\right\}/\left\{1- \exp \left[\frac{-b\ \left({t}_2+24-{t}_1\right)}{t_{\mathrm{sr}}+24-{t}_1}\right]\right\}. $$
(9)
The following four models are proposed for determining T
pn, 2 or 4 h before sunrise, from pre-dawn sub-hourly temperature measurements.
This proposed method yields two model nowcasts using sub-hourly temperature measurement inputs between 6 and 4 h before sunrise for the first (4-h) nowcast and measurements 4 to 2 h before sunrise for the second (2-h) to determine the assumed exponential decrease in air temperature and hence to determine the exponential decay factor b. This factor together with the measured temperature inputs hours before sunrise are then used to obtain T
pn 4 and 2 h before sunrise. Modelled on the previous theory for a nighttime period (Eq. (8)) usually after midnight, for the 2-h-ahead nowcast, the sub-hourly temperature inputs T(t
sr − 4) and T(t
sr − 2) are used. At and between these times t, for which t
sr − 4 ≤ t ≤ t
sr − 2, the decay factor (b = b
sr − 4to−2) was determined from the slope of the plot of ln [T(t) − min (T
sr − 4to−2) + 0.01] vs \( \frac{t-{t}_{\mathrm{sr}-4}}{t_{\mathrm{sr}-2}-{t}_{\mathrm{sr}-4}} \) where min (T
sr − 4to−2) represents the minimum of the temperatures between the two times and t
sr − 2 − t
sr − 4 = 2 h. The constant of 0.01 °C ensures that the argument of the logarithm is always positive and hence defined when T(t) = min (T
sr − 4to−2). Using this model, unlike the Parton and Logan (1981) method, a different b = b
sr − 4to−2 value from b = 2.2 is determined for each early-morning period. Similar procedures were used for the 4-h ahead nowcasts using temperatures between times t
sr − 6 and t
sr − 4 and the decay factor b = b
sr − 6to−4 from the slope of the plot of ln [T(t) − min (T
sr − 6to− 4) + 0.01] vs \( \frac{t-{t}_{\mathrm{sr}-6}}{t_{\mathrm{sr}-4}-{t}_{\mathrm{sr}-6}} \).
By inversion of Eq. 1 (Eqs. (8) or (9)), and application to the period 4 to 2 h before sunrise for a nowcast 2 h before sunrise, T
pn was determined assuming a continued and exponential decay after t
sr − 2, at the same exponential rate:
$$ {T}_{\mathrm{pn}} = \left\{T\left({t}_{\mathrm{sr}-2}\right)-T\left({t}_{\mathrm{sr}-4}\right) \exp \left[\frac{-{b}_{\mathrm{sr}-4\mathrm{t}\mathrm{o}-2}\ \left({t}_{\mathrm{sr}-2}-{t}_{\mathrm{sr}-4}\right)}{t_{\mathrm{sr}}-{t}_{\mathrm{sr}-4}}\right]\right\}/\left\{1- \exp \left[\frac{-{b}_{\mathrm{sr}-4\mathrm{t}\mathrm{o}-2}\ \left({t}_{\mathrm{sr}-2}-{t}_{\mathrm{sr}-4}\right)}{t_{\mathrm{sr}}-{t}_{\mathrm{sr}-4}}\right]\right\} $$
(10)
which for this 2-h nowcast simplifies to:
$$ {T}_{\mathrm{pn}}=\left[T\left({t}_{\mathrm{sr}-2}\right)-T\left({t}_{\mathrm{sr}-4}\right) \exp\ \left(-{b}_{\mathrm{sr}-4\mathrm{t}\mathrm{o}-2}/2\right)\right]/\left[1- \exp\ \left(-{b}_{\mathrm{sr}-4\mathrm{t}\mathrm{o}-2}/2\right)\right]. $$
(11)
For a nowcast 4 h before sunrise:
$$ {T}_{\mathrm{pn}} = \left[T\left({t}_{\mathrm{sr}-4}\right)-T\left({t}_{\mathrm{sr}-6}\right) \exp\ \left(-{b}_{\mathrm{sr}-6\mathrm{t}\mathrm{o}-4}/3\right)\right]/\left[1- \exp\ \left(-{b}_{\mathrm{sr}-6\mathrm{t}\mathrm{o}-4}/3\right)\right]. $$
(12)
The equations and methods used for historic data or for an on-board datalogger 2-h before sunrise nowcast are shown in Table 1 and similarly using Eq. (12) applied for the minimum between 6 and 4 h before sunrise for the 4-h before sunrise nowcast. For the 2-h nowcast for times when the calculated b value was out of its expected range, typically |b| < 1, then Eq. (11) was applied using b
sr − 4to−2 = 2.2 and T(t
sr − 2) replaced by the minimum temperature between 4 and 2 h before sunrise. A similar procedure was followed for the 4-h nowcast using Eq. (12) and b
sr − 6to−4 = 2.2.
Table 1 Equations and datalogger methods used for the 2-h nowcasting of the daily minimum temperature
This proposed model, instead of the value for b (=b
sr − 4 to − 2 for the 2-h nowcast and b = b
sr − 6 to− 4 for the 4-h nowcast) determined by regression (Table 1), uses a fixed value of 2.2 (Parton and Logan 1981) in Eqs. (11) and (12), respectively. In the case of real-time analyses, this model is simple since no on-board datalogger real-time regression analysis is required. Model 2 is also used as part of model 1 when |b| < 1.
For this model, T
pn is determined for times 4 and 2 h before sunrise based on the square root model (Eq. 4) using the relationship:
$$ T(t)=T\left({t}_{t_{\mathrm{sr}-4}}\right)-{c}_{\mathrm{sr}-4\mathrm{t}\mathrm{o}-2}\ \sqrt{t-{t}_{\mathrm{sr}-4}}. $$
(13)
Therefore, using temperature measurements between 4 and 2 h before sunrise, a plot of T(t) − T(t
sr − 4) vs \( \sqrt{t-{t}_{\mathrm{sr}-4}} \) yields a slope of − c
sr − 4 to − 2 from which T
pn is determined using:
$$ {T}_{\mathrm{pn}}=T\left({t}_{\mathrm{sr}-4}\right)-{c}_{\mathrm{sr}-4\mathrm{t}\mathrm{o}-2}\ \sqrt{t_{\mathrm{sr}}-{t}_{\mathrm{sr}-4}} $$
(14)
which simplifies to
$$ {T}_{\mathrm{pn}}=T\left({t}_{\mathrm{sr}-4}\right)-2\ {c}_{\mathrm{sr}-4\mathrm{t}\mathrm{o}-2} $$
(15)
where it is assumed that the same c
sr − 4 to −2 can also be used for times 2 h before sunrise and sunrise. A modified version of Eq. (15) was used for the 4-h before sunrise nowcasts based on c
sr − 6 to − 4 and temperature measurements between times 6 and 4 h before sunrise.
This model is the same as model 3 for determining T
pn for times t between 4 and 2 h before sunrise but with T(t
sr − 2) replacing T(t
sr − 4):
$$ {T}_{\mathrm{pn}}=T\left({t}_{\mathrm{sr}-2}\right)-{c}_{\mathrm{sr}-4\mathrm{t}\mathrm{o}-2}\ \sqrt{t_{\mathrm{sr}}-{t}_{\mathrm{sr}-2}}. $$
(16)
This simplifies to
$$ {T}_{\mathrm{pn}}=T\left({t}_{\mathrm{sr}-2}\right)-\sqrt{2}\ {c}_{\mathrm{sr}-4\mathrm{t}\mathrm{o}-2} $$
(17)
where it is assumed that the same c
sr − 4 to −2 can be used for times between 2 h before sunrise and sunrise. As was the case for model 3 (square root), a modified version of Eq. (17) was used for the 4-h before sunrise nowcasts.
The various equations and datalogger protocols used in the datalogger for the web-based early-warning system used are outlined in Table 1. These protocols were also used for the spreadsheet calculations for the historic air temperature data for all sites.
All model nowcasts, a few hours before sunrise, are compromised by events such as transient clouds, increased wind speed, changes in atmospheric stability and precipitation with consequential likely disagreement between model nowcasts and measurements. Usually, in the case of frost, however, these events tend to reduce the chance of freezing conditions.