Abstract
Many studies have attempted to understand the true nature of COVID-19 and the factors influencing the spread of the virus. This paper investigates the possible effect the COVID-19 pandemic spreading in Iraq considering certain factors, that include isolation and weather. A mathematical model of cases representing inpatients, recovery, and mortality was used in formulating the control variable in this study to describe the spread of COVID-19 through changing weather conditions between 17th March and 15th May, 2020. Two models having deterministic and an uncertain number of daily cases were used in which the solution for the model using the Pontryagin maximum principle (PMP) was derived. Additionally, an optimal control model for isolation and each factor of the weather factors was also achieved. The results simulated the reality of such an event in that the cases increased by 118%, with an increase in the number of people staying outside of their house by 25%. Further, the wind speed and temperature had an inverse effect on the spread of COVID-19 by 1.28% and 0.23%, respectively. The possible effect of the weather factors with the uncertain number of cases was higher than the deterministic number of cases. Accordingly, the model developed in this study could be applied in other countries using the same factors or by introducing other factors.
Keywords
Introduction
The COVID-19 pandemic has resulted in a huge loss of human life and affected economies worldwide. Most nations have entered into a “lockdown” situation, isolating their economies from others in facing the virus and decrease the loss of human life. Several studies have investigated COVID-19 to understand the composition of the virus and determine the most suitable treatment. However, the danger of COVID-19 is represented by its spread without any clinical symptoms during the early stages of contracting the virus and long period incubation [19]. Chen et al. [2] compared two groups of patients; COVID-19 and SARS-CoV-2-negative, where it was revealed that COVID-19 patients suffered from high fever and cough more than SARS-CoV-2 patients. Procalcitonin (PCT) levels of SARS-CoV-2 patients (approximately 2 out of 5 patients) were shown to be higher compared to COVID-19 patients. Also, COVID-19 patients had lower creatinine levels compared with SARS-CoV-2 patients. In the case of those at a young age, the distinction between the two diseases can be diagnosed depending on the fever, cough, urea and creatinine levels, and parameters associated with routine blood workup. COVID-19, SARS and MERS have mostly similar pathological features [23]. However, the harm caused by COVID-19 may be caused by SARS-CoV-2 or through liver damage. Ai et al. [1] compared chest CT scans and reverse-transcription chain reaction to diagnose the virus in a sample of patients (1,014 patients) in China. Chest CT scans were shown to be highly sensitive in the diagnosis of the virus. X. Chen et al. [3] assessed the state of pregnant women, having a positive test for COVID-19, in which fever and cough were the main symptoms that were evident in the pregnant women without vertical transmission of the virus in late pregnancy. The World Health Organisation (WHO) confirmed the effect of COVID-19 on the mental health of human; especially children and the elderly [22].
The drug used for the treatment of malaria (Chloroquine phosphate) has found to be effective in the treatment of COVID-19 in some 100 patients through clinical trials conducted in hospitals across seven cities in China [6]. Lipsitch et al. [10] discussed the approach adopted in the treatment of an influenza pandemic (2009). While this approach may possibly be used in the treatment of Covid-19, it depends on many factors, such as existing surveillance systems. In a separate case, viral RNA samples were collected from survivors and people who had died to explore the factors that caused patients to die in a hospital setting by employing multivariable logistic regression [24].
In fact, several studies have formulated mathematical models to simulate actual cases of epidemics and pandemics around the world. In some studies, the optimal control model was widely used to determine the effect of vaccination and isolation. Lee et al. [9] clarified the effect of treatment and isolation on the control of fast transmitting diseases, such as influenza. In their study, they discussed isolation strategies having insufficient antiviral resources. Three models of optimal control, namely, vaccination, isolation and the mixed model of the SIR epidemic were investigated by Hansen and Day [8] to minimise the magnitude of the outbreak. Tuite et al. [18] explored control strategies that could aid in understanding the spreading processes associated with the cholera epidemic in Haiti to reduce the potential effects. Rodrigues et al. [15] discussed a dengue vaccine as a control variable with distinct levels and two methods of treatment. The first method was for paediatric patients, and the second method was for random mass vaccination. A comparison between a different scenario regarding tuberculosis epidemiological features was conducted by P. Rodrigues et al. [16], aiming to reduce total implementation costs and the number of infected cases. Also, regarding tuberculosis, Moualeu et al. [11] formulated a mathematical model that considers infection (diagnosed and undiagnosed), lost-sight, and latently infected aspects. Pang et al. [12] formulated a mathematical model that simulated the actual cases of measles transmission in the United States (US) for the period between 1951 and 1962 to determine the optimal strategy for vaccination. The spread of the Ebola virus in West Africa was investigated by Rachah and Torres [13, 14]. The first paper investigated the effect of different cases of vaccination on the virus spreading over time, while the second paper addressed in addition to vaccination, several strategies to reduce the number of infected and exposed individuals. In another study by Gao and Huang, they incorporated three controls as part of a strategy from among several initially developed strategies to minimise intervention costs and reduce the burden of tuberculosis [5].
The structure of this paper is organised into five sections. The first section, already discussed, provided a brief introduction and background information on COVID-19. Section 2 provides further information on the spread of COVID-19, followed by Section 3 that presents two models; the optimal control model and a model presenting an explicit solution using the Pontryagin maximum principle (PMP). The results and explanation of several models are presented and discussed in Section 4. Lastly, Section 5 presents the overall conclusions and recommendations for future research.
The spread of COViD-19
In December 2019, the first cases of COVID-19 surfaced in Wuhan, Hubei, China [2]. Since then, four other Asian countries confirmed a further 282 cases of the virus on 20th January 2020, two cases in Thailand, one case Japan and South Korea, and the remaining number of cases were reported in China. All cases originated from Wuhan City [20].
After several months, the virus spread to other cities in China, and another 33 countries worldwide. On 24th February, the number of deaths reported in China amounted to 2,663, and 33 in other countries [1]. Towards the end of February 2020, the population in Europe and North America showed signs of the virus, albeit a different strain or foci of the virus, including countries in Asia, and the Middle East.
At the same time, the first case of COVID-19 was recorded in Africa and Latin America [21]. At the beginning of March 2020, more than 10,000 patients had died from the virus in 10 countries, including Iran, Italy, and South Korea [19]. A significant increase in the harm caused by the was in the Middle East was confirmed during the middle of March. As a result of the rapid spread of the virus, the WHO classified the COVID-19 epidemic as a global pandemic [21].
The first case of COVID-19 in Iraq appeared in the Najaf province, south of the capital Baghdad on 24th February 2020; an Iranian student studying Islamic science in Najaf. Many Iraqi people travel to Iran to visit many of the holy shrines and enjoy tourist attractions. It was believed that the virus originated from Iran. On 26th February, four new cases were reported with the number increasing to 13 on 1st March, before reporting 93 further cases in the middle of March with nine deaths.
Optimal control model
This section presents two models having a known and uncertain number of new daily cases; the deterministic model and the chance-constrained model, respectively.
Deterministic model
Optimal control for optimization is defined by:
Subject to the state equations of cases, inpatients, recovered cases and death:
where,
y(t): The control variable.
C(t): Percent of confirmed cases.
I(t): Percent of inpatients.
R(t): Percent of recovered cases.
D(t): Percent of death cases.
β(t): Percent of the new cases to the inpatient cases.
μ(t): Percent of the recover cases to the inpatient cases.
ΔC(t) = C(t)-C(t-1)
Equation (2) signifies the total number of cases that increased based on new cases daily. The total number of inpatients increases by the addition of new cases and decreases by the number of recovery and deaths each day (Equation 3). Equations 5) represent the total number of recovered patients and deaths, respectively. The control variable represents the percentage of isolation or each weather factor.
By using the PMP, determining the solution of the optimal control model can be achieved. The Lagrangian function is expressed as follows [17]:
A Hamiltonian function is expressed as:
Substituting Equation (7) into Equation (6), gives:
Deriving Equation (8) concerning C (t) , I (t) , R (t) , D (t), separately, gives:
By rearranging Equations (9–12), we can determine the adjoint equations as:
Rearranging Equation (13), yields:
By substituting Equation (19) into Equation (2), it yields:
From Equation (20), we can determine the total number of cases over time as follows:
By substituting Equation (19) into Equation (3), it yields:
From Equation (22), we then get:
Then, substituting Equation (21) into Equation (23), it yields:
Equation (24) represents the total number of inpatients over time. We can determine the total number of recovered cases over time by substituting Equation (24) into Equation (4) as follows:
Substituting Equation (24) into Equation (5) yields the total number of death cases over time as follows:
Thus, the value of the control variable is as follows:
From Equation (27), y (t) = -1 means:
Initially the value of the control variable is zero, which means the model represents the actual cases registered in Iraq with the real percentage of new cases, recovered, and deaths as follows:
Next, by introducing the effect of wind (for example): changing the value of the control variable and cases depending on the wind degree (W) and transition matrix (φ) (see Appendix) we get:
Where ABS = absolute value.
The elements of the transition matrix can be calculated as follows (for example, humidity):
Where
Finally, the next tasks include incorporating the value of the control variable into an optimal control model to obtain the solution. The solution of the optimal control model relies on Equations (15–18, 21, 24–26). The solution is found by using the goal seek function in Microsoft Excel with λ(T) = 0. Hence, achieving the condition λ(T) = 0 by changing the value of λ(0).
The number of new cases reported in Iraq depends on the number of samples tested. Therefore, the actual cases may be is greater than those recorded cases. In this model, the number of new cases is uncertain given by the equation representing chance-constrained:
Where α takes values between zero and one (1) and NC is a random variable (new cases).
In determining the solution, chance-constrained must be converted to deterministic constrained. Here, the value of α is equal to zero or one (1) representing an extremely risky or extremely conservative attitude, respectively. The minimum acceptable to achieve the constraint is α, while (1 - α) is the maximum acceptable risks [7].
If NC is a random variable that adheres to a normal distribution with mean
Where ∅ is the cumulative distribution function (CDF) of the standard normal distribution.
The number of daily cases can be found from Eq. (37) with the initial value of cases C (0). To determine the effect of the weather factors, we apply the deterministic model (Equations 1–5) with the daily cases of chance-constrained (Equation 37).
Table 1 (see Appendix) shows the number of COVID-19 cases and degrees of temperature, humidity, wind and pressure from 17th March to 15th May. First, we determine the values of (β,μ,N) by using Equation (31) to fit the actual cases reported in Table (1) with a zero (0) value of the control variable (see Table 2 in the Appendix).
Next, we change the control variable value to determine the results that represent the effect of isolation and weather.
The effect of isolation is determined by presenting the value of the control variable given below:
Figure (1) shows the effect of isolation on the results, with the actual cases (A.C.), increased cases (I.C.), and decreased cases (D.C.). From Fig. (1), we can conclude that the number of cases increases, due to increase in the number of people that did not commit to staying at home (y(t) = 0.25), and vice versa.

The effect of isolation.
The increase in the per cent of people that did not commit to staying at home by 25% led to an increase in the number of COVID-19 cases by 118%, while, the proportion of COVID-19 cases decreased by 53.4% with an increase in the number of citizens staying at home by 25%. The numbers of inpatients (A.I, I.I, D.I), recoverd (A.R, I.R, D.R) and deaths (A.D, I.D, D.D) follow the number of cases.
According to the WHO, symptoms of infection first appear between 2 and 14 days, usually 5 days. In this case, we take the weather for the last 5 days (see Table 3 in the Appendix). We can then find the transition matrix for each factor of the weather (see Tables 4–7 in the Appendix) from Table (3). The values of the main diagonal are zero (0) (without effect) and the other values are negative (cases decrease) and positive (cases increase). The values of the transition matrix represent an increase (or decrease) of COVID-19 cases with an increase (or decrease) for every one (1) degree of the weather.
From Equations (32–34), and Table (4), we can determine the value of the control variable, according to the effect of humidity. Figure (2) shows the possible effect of humidity on the number of new cases.

Numbers of new cases with and without the effect of humidity.
The white colour represents the number of new cases without the effect of humidityt, which means the default number. Meanwhile, the actual number of cases, affected by the humidity, is represented by gray colour. The explanation for Fig. (2) is as follows:
Two colours having the same value signifies no change in humidity, thus having no effect.
The white colour higher than the gray colour means humidity increases, while for new cases is decreases.
The other case means a decrease in humidity and an increase in new cases.
Similarly, we determine the possible effect of other weather factors, as can be seen in Figs. (3–5):

Numbers of new cases with and without the effect of temperature.

Numbers of new cases with and without the effect of wind.

Numbers of new cases with and without the effect of pressure.
As evident in Figs. (2–5), the wind shows as having the highest effect on the number of new COVID-19 cases. Figure (6) shows the possible effect of the weather factors at the end of period.

Weather factors and effect.
Figure (6) shows the possible effect of weather on the number of new COVID-19 cases. Wind (W.E) and pressure (P.E.) represent the highest and lowest effect, respectively. However, the effect of isolation (see Fig. 1) is more important compared to the weather factors. Figure (7) shows the results at the end of the period without the effect of the weather.

The results of optimal control model with different values of the control variable.
From Fig. (7), it can be seen that the increase in wind speed (W) and temperature (T) has led to a decrease in the number of COVID-19 cases. For example, the number of cases is 3,346 and 3,204 without the possible effect of both wind and temperature, respectively. Whereas the number of cases slightly increased with an increase in humidity (H) and pressure (P) compared to the number of actual cases (A).
For the chance-constraint model, the β value is changed according to Eq. (36). At first, we divide the study period into 12 sub-periods with 5 days for each sub-period. Next, a normality test of observations of the sub-periods is conducted, in which all sub-periods adhere to a normal distribution (see Table 8). Eq. (36) is then applied to determine the daily cases with α = 0.90 and ∅-1 (α) = 1.28. Finally, the same steps of the deterministic model are used to find the solution. From Equations (32–34), and Table (9), we can find the value of the control variable and the possible effect of the weather factors, as shown in Figs. (8–11).

Number of new cases with and without the effect of humidity (chance-constrained).

Number of new cases with and without the wind effect (chance-constrained).

Number of new cases with and without the pressure effect (chance-constrained).

Number of new cases with and without the pressure effect (chance-constrained).
By observing Figs. (8–11), the pressure signifies the highest effect on the number of new COVID-19 cases. Whereas, the wind represents the second-highest effect, but with an inverse relation to COVID-19 cases. Figure (12) below illustrates the possible proportional effect of the weather factors at the end of the period.

Proportion, (as a percentage) due to the effect of weather (chance-constrained).
From observing Fig. (12), we can see that the pressure (P.E) and temperature (T.E.) represent the highest and lowest effect, respectively. The effect of the weather in the chance-constrained model is higher than the deterministic model because the increase in the number of COVID-19 cases is according to the chance-constrained model.
In this paper, the possible effect of both weather factors and isolation on the spread of COVID-19 in the context of Iraq was investigated, finding that temperature, humidity, wind, and pressure had a noticeable effect on the spread of the virus. An optimal control model was developed to describe the spread of COVID-19 cases, Deterministic and chance-constrained models were also developed, and the solution of the model using the PMP was also derived. The transition matrix for each of the factor factors was addressed.
Initially, a control variable y(t) representing the percentage of isolation and weather factors was determined. The zero value of the control variable represented the actual data of COVID-19 cases in Iraq, while the optimal solution was determined with y = –1. Next, was determining the value of the control variable with respect to five models, before finally, clarifying the possible effect of isolation and the weather factors on the spread of COVID-19.
Accordingly, it was shown that isolation was significant in containing COVID-19 from contagion. On the other hand, the number of cases increased by 118% attributed to an increase in the number of people who ignored the need to stay at home, which rose by 25%. In contrast, the cases reduced by 53.4% for the opposite case where people stayed at home.
These statistics also support the nature of the virus in reality since it is highly contagious, spreading from one person to many. Weather factors also had a noticeable effect on the spread of COVID-19, though lower than self-isolation. Likewise, both wind speed and temperature had the highest effect compared with other weather factors. Further, the wind speed and temperature had an inverse effect on the spread of COVID-19 by 1.28% and 0.23%, respectively, while a positive relationship with humidity and pressure. Humidity and temperature had a similar effect but opposingly. Moreover, increasing the number of daily cases of COVID-19, according to the chance-constrained model, weather factors had a greater effect.
Accordingly, the model developed in this study could be applied in other countries using the same factors or by introducing other factors, such as communication, transportation, and payment.
Footnotes
Appendix
The number of COVID-19 cases and weather degrees in Iraq The ministry of health/ Iraq. https://www.timeanddate.com/weather/iraq/baghdad/historic?month=4&year=2020. The values of the model parameters The average of COVID-19 cases, according to humidity, temperature, wind and pressure The transition matrix of the number of COVID-19 cases, according to humidity The transition matrix of the number of COVID-19 cases, according to temperature The transition matrix of the number of COVID-19 cases, according to wind The transition matrix of the number of COVID-19 cases, according to pressure The number of cases, according to chance-constrained model The average of COVID-19 cases, according to humidity, temperature, wind and pressure (chance-constrained) The transition matrix of the number of COVID-19 cases, according to humidity (chance-constrained) The transition matrix of the number of COVID-19 cases, according to temperature (chance-constrained) The transition matrix of the number of COVID-19 cases, according to wind (chance-constrained) The transition matrix of the number of COVID-19 cases, according to pressure (chance-constrained)
Date
Cases
Recover
Death
New Cases
Temp.
Wind
Humid.
Pres.
17 March
165
43
12
11
26
7
40
1015
18
177
49
12
12
22
13
39
1010
19
192
49
13
15
18
7
57
1016
20
208
49
17
16
23
9
32
1014
21
214
52
17
6
22
7
45
1006
22
233
57
20
19
17
2
52
1011
23
266
62
23
33
20
9
46
1015
24
316
75
27
50
24
4
34
1014
25
346
103
29
30
27
13
29
1009
26
382
105
36
36
28
20
30
1010
27
458
122
40
76
24
11
40
1014
28
506
131
42
48
24
7
46
1009
29
547
143
42
41
22
7
50
1014
30
630
152
46
83
23
9
33
1012
31
694
170
50
64
26
4
26
1017
1 April
728
182
52
34
28
26
29
1007
2
772
202
54
44
26
9
28
1012
3
820
226
54
48
25
4
33
1016
4
878
259
56
58
25
9
37
1018
5
961
259
61
83
26
4
29
1021
6
1031
344
64
70
29
9
30
1014
7
1122
373
65
91
26
9
37
1012
8
1202
452
69
80
30
7
27
1010
9
1232
496
69
30
26
4
54
1006
10
1279
550
70
47
25
7
35
1008
11
1318
601
72
39
25
9
30
1012
12
1352
640
76
34
26
6
29
1016
13
1378
717
78
26
27
10
33
1017
14
1400
766
78
22
27
13
15
1017
15
1415
812
79
15
29
17
11
1016
16
1434
856
80
19
30
2
17
1013
17
1482
906
81
48
32
7
14
1011
18
1513
953
82
31
31
4
21
1011
19
1539
1009
82
26
28
7
29
1015
20
1574
1043
82
35
32
4
21
1013
21
1602
1096
83
28
33
4
20
1012
22
1631
1146
83
29
33
4
25
1010
23
1677
1171
83
46
37
6
18
1004
24
1708
1204
86
31
29
6
29
1008
25
1763
1224
87
55
32
13
21
1001
26
1820
1263
87
57
26
13
33
1008
27
1847
1286
88
27
28
6
23
1013
28
1928
1319
90
81
31
9
17
1011
29
2003
1346
92
75
24
4
29
1008
30
2085
1375
93
82
24
6
40
1009
1 May
2153
1414
94
68
31
6
26
1014
2
2219
1473
95
66
36
2
16
1011
3
2296
1490
97
77
33
11
20
1013
4
2346
1544
97
50
26
15
45
1011
5
2431
1571
102
85
29
11
21
1018
6
2480
1602
102
49
31
7
20
1016
7
2543
1626
102
63
37
4
13
1009
8
2603
1661
104
60
29
9
33
1008
9
2679
1702
107
76
29
13
20
1008
10
2767
1734
109
88
29
9
21
1010
11
2818
1790
110
51
32
6
17
1015
12
2913
1903
112
95
35
4
13
1013
13
3032
1966
115
119
39
9
8
1011
14
3143
2028
115
111
40
11
10
1009
15
3193
2089
117
50
41
15
10
1008
Date
β
μ
17 March
0.066667
0.100000
0.009091
18
0.067797
0.051724
0.000000
19
0.078125
0.000000
0.007692
20
0.076923
0.000000
0.028169
21
0.028037
0.020690
0.000000
22
0.081545
0.032051
0.019231
23
0.124060
0.027624
0.016575
24
0.158228
0.060748
0.018692
25
0.086705
0.130841
0.009346
26
0.094241
0.008299
0.029046
27
0.165939
0.057432
0.013514
28
0.094862
0.027027
0.006006
29
0.074954
0.033149
0.000000
30
0.131746
0.020833
0.009259
31
0.092219
0.037975
0.008439
1 April
0.046703
0.024291
0.004049
2
0.056995
0.038760
0.003876
3
0.058537
0.044444
0.000000
4
0.066059
0.058615
0.003552
5
0.086368
0.000000
0.007800
6
0.067895
0.136437
0.004815
7
0.081105
0.042398
0.001462
8
0.066556
0.116006
0.005874
9
0.024351
0.065967
0.000000
10
0.036747
0.081942
0.001517
11
0.029590
0.079070
0.003101
12
0.025148
0.061321
0.006289
13
0.018868
0.132075
0.003431
14
0.015714
0.088129
0.000000
15
0.010601
0.087786
0.001908
16
0.013250
0.088353
0.002008
17
0.032389
0.101010
0.002020
18
0.020489
0.098326
0.002092
19
0.016894
0.125000
0.000000
20
0.022236
0.075724
0.000000
21
0.0174781
0.125295
0.002364
22
0.0177805
0.124378
0
23
0.0274299
0.059101
0
24
0.0181498
0.078947
0.007177
25
0.0311968
0.044247
0.002212
26
0.0313186
0.082978
0
27
0.0146183
0.048625
0.002114
28
0.0420124
0.063583
0.003853
29
0.0374438
0.047787
0.003539
30
0.0393285
0.047001
0.001620
1 May
0.0315838
0.060465
0.001550
2
0.0297431
0.090629
0.001536
3
0.0335365
0.023977
0.002820
4
0.0213128
0.076595
0
5
0.0349650
0.035620
0.006596
6
0.0197580
0.039948
0
7
0.0247738
0.029447
0
8
0.0230503
0.041766
0.002386
9
0.0283687
0.047126
0.003448
10
0.0318033
0.034632
0.002164
11
0.0180979
0.061002
0.001089
12
0.0326124
0.125835
0.002227
13
0.0392480
0.066246
0.003154
14
0.035316
0.062
0
15
0.015659
0.061803
0.002026
Humid.
Temp.
Wind
Pres.
56–75
50
91–100
55
21–25
40
5026–5035
55
76–100
51
101–110
23
26–30
52
5036–5045
79
101–125
60
111–120
31
31–35
54
5046–5055
57
126–150
56
121–130
53
36–40
41
5056–5065
50
151–175
67
131–140
51
41–45
59
5066–5075
38
176–200
48
141–150
58
46–50
61
5076–5085
60
201–225
28
151–160
62
51–55
53
226–250
22
161–170
64
56–60
34
251–275
12
171–180
50
State
75
100
125
150
175
200
225
250
275
75
0.000
0.030
0.208
0.084
0.170
–0.013
–0.147
–0.160
–0.190
100
–0.030
0.000
0.386
0.111
0.217
–0.024
–0.182
–0.192
–0.221
125
–0.208
–0.386
0.000
–0.164
0.132
–0.161
–0.324
–0.307
–0.323
150
–0.084
–0.111
0.164
0.000
0.428
–0.159
–0.377
–0.343
–0.354
175
–0.170
–0.217
–0.132
–0.428
0.000
–0.745
–0.780
–0.600
–0.550
200
0.013
0.024
0.161
0.159
0.745
0.000
–0.815
–0.527
–0.485
225
0.147
0.182
0.324
0.377
0.780
0.815
0.000
–0.240
–0.320
250
0.160
0.192
0.307
0.343
0.600
0.527
0.240
0.000
–0.400
275
0.190
0.221
0.323
0.354
0.550
0.485
0.320
0.400
0.000
State
100
110
120
130
140
150
160
170
180
100
0.000
–3.167
–1.200
–0.070
–0.107
0.053
0.652
0.464
–0.036
110
3.167
0.000
0.767
2.958
1.370
1.143
1.143
0.803
0.444
120
1.200
–0.767
0.000
2.191
0.986
0.888
0.787
0.650
0.317
130
0.070
–2.958
–2.191
0.000
–0.218
0.236
0.318
0.265
–0.058
140
0.107
–1.370
–0.986
0.218
0.000
0.690
0.587
0.426
–0.018
150
–0.053
–1.143
–0.888
–0.236
–0.690
0.000
0.484
0.294
–0.254
160
–0.652
–0.978
–0.787
–0.318
–0.587
–0.484
0.000
0.104
–0.623
170
–0.464
–0.803
–0.650
–0.265
–0.426
–0.294
–0.104
0.000
–1.350
180
0.036
–0.444
–0.317
0.058
0.018
0.254
0.623
1.350
0.000
State
25
30
35
40
45
50
55
60
25
0.000
2.400
1.367
0.036
0.958
0.851
0.446
–0.177
30
–2.400
0.000
0.333
–1.145
0.477
0.464
0.055
–0.607
35
–1.367
–0.333
0.000
–2.624
0.549
0.508
–0.015
–0.795
40
–0.036
1.145
2.624
0.000
3.722
2.074
0.855
–0.337
45
–0.958
–0.477
–0.549
–3.722
0.000
0.426
–0.578
–1.690
50
–0.851
–0.464
–0.508
–2.074
–0.426
0.000
–1.582
–2.749
55
–0.446
–0.055
0.015
–0.855
0.578
1.582
0.000
–3.915
60
0.177
0.607
0.795
0.337
1.690
2.749
3.915
0.000
State
5035
5045
5055
5065
5075
5085
5035
0.000
2.350
0.123
–0.158
–0.436
0.090
5045
–2.350
0.000
–2.104
–1.413
–1.364
–0.475
5055
–0.123
2.104
0.000
–0.721
–0.995
0.068
5065
0.158
1.413
0.721
0.000
–1.268
0.463
5075
0.436
1.364
0.995
1.268
0.000
2.193
5085
–0.090
0.475
–0.068
–0.463
–2.193
0.000
Date
Cases
β
Mean
S.D.
17 March
165
0.066667
12.00
3.94
18
182
0.093407
19
199
0.085427
20
216
0.078704
21
233
0.072961
22
281
0.170819
33.60
11.19
23
329
0.145897
24
377
0.127321
25
425
0.112941
26
473
0.10148
27
558
0.15233
62.40
17.87
28
643
0.132193
29
728
0.116758
30
813
0.104551
31
898
0.094655
1 April
975
0.078974
53.40
18.65
2
1052
0.073194
3
1129
0.068202
4
1206
0.063847
5
1283
0.060016
6
1378
0.06894
63.60
24.83
7
1473
0.064494
8
1568
0.060587
9
1663
0.057126
10
1758
0.054039
11
1797
0.021703
27.20
9.52
12
1836
0.021242
13
1875
0.0208
14
1914
0.020376
15
1953
0.019969
16
1999
0.023012
31.80
10.85
17
2045
0.022494
18
2091
0.021999
19
2137
0.021526
20
2183
0.021072
21
2236
0.023703
37.80
12.07
22
2289
0.023154
23
2342
0.02263
24
2395
0.022129
25
2448
0.02165
26
2542
0.036979
64.40
23.19
27
2636
0.03566
28
2730
0.034432
29
2824
0.033286
30
2918
0.032214
1 May
3004
0.028628
69.20
13.14
2
3090
0.027832
3
3176
0.027078
4
3262
0.026364
5
3348
0.025687
6
3435
0.025328
67.20
15.09
7
3522
0.024702
8
3609
0.024106
9
3696
0.023539
10
3783
0.022998
11
3910
0.032481
85.20
32.84
12
4037
0.031459
13
4164
0.0305
14
4291
0.029597
15
4418
0.028746
Humid.
Temp.
Wind
Pres.
51–75
127
91–100
48
21–25
53
5026–5035
94
76–100
66
101–110
36
26–30
75
5036–5045
94
101–125
81
111–120
43
31–35
72
5046–5055
77
126–150
81
121–130
75
36–40
64
5056–5065
73
151–175
89
131–140
69
41–45
86
5066–5075
56
176–200
69
141–150
70
46–50
76
5076–5085
71
201–225
28
151–160
89
51–55
77
226–250
25
161–170
84
56–60
43
251–275
17
171–180
127
State
75
100
125
150
175
200
225
250
275
75
0.000
–2.430
–0.922
–0.608
–0.380
–0.463
–0.660
–0.583
–0.550
100
2.430
0.000
0.585
0.303
0.303
0.029
–0.306
–0.275
–0.281
125
0.922
–0.585
0.000
0.021
0.162
–0.156
–0.529
–0.447
–0.426
150
0.608
–0.303
–0.021
0.000
0.304
–0.245
–0.712
–0.564
–0.515
175
0.380
–0.303
–0.162
–0.304
0.000
–0.793
–1.220
–0.853
–0.720
200
0.463
–0.029
0.156
0.245
0.793
0.000
–1.647
–0.883
–0.696
225
0.660
0.306
0.529
0.712
1.220
1.647
0.000
–0.120
–0.220
250
0.583
0.275
0.447
0.564
0.853
0.883
0.120
0.000
–0.320
275
0.550
0.281
0.426
0.515
0.720
0.696
0.220
0.320
0.000
State
100
110
120
130
140
150
160
170
180
100
0.000
–1.240
–0.275
0.888
0.530
0.440
0.898
0.596
0.655
110
1.240
0.000
0.690
3.904
1.679
1.147
1.147
0.972
1.523
120
0.275
–0.690
0.000
3.214
1.334
0.917
1.174
0.834
1.408
130
–0.888
–3.904
–3.214
0.000
–0.545
–0.232
0.494
0.239
1.047
140
–0.530
–1.679
–1.334
0.545
0.000
0.082
1.014
0.501
1.445
150
–0.440
–1.147
–0.917
0.232
–0.082
0.000
1.946
0.710
1.900
160
–0.898
–1.347
–1.174
–0.494
–1.014
–1.946
0.000
–0.526
1.877
170
–0.596
–0.972
–0.834
–0.239
–0.501
–0.710
0.526
0.000
4.280
180
–0.655
–1.523
–1.408
–1.047
–1.445
–1.900
–1.877
–4.280
0.000
State
25
30
35
40
45
50
55
60
25
0.000
4.400
1.900
0.703
1.635
0.920
0.813
–0.286
30
–4.400
0.000
–0.600
–1.145
0.713
0.050
0.095
–1.067
35
–1.900
0.600
0.000
–1.691
1.369
0.267
0.269
–1.160
40
–0.703
1.145
1.691
0.000
4.429
1.245
0.922
–1.027
45
–1.635
–0.713
–1.369
–4.429
0.000
–1.938
–0.832
–2.846
50
–0.920
–0.050
–0.267
–1.245
1.938
0.000
0.275
–3.300
55
–0.813
–0.095
–0.269
–0.922
0.832
–0.275
0.000
–6.875
60
0.286
1.067
1.160
1.027
2.846
3.300
6.875
0.000
State
5035
5045
5055
5065
5075
5085
5035
0.000
0.000
–0.869
–0.710
–0.943
–0.470
5045
0.000
0.000
–1.738
–1.065
–1.258
–0.588
5055
0.869
1.738
0.000
–0.392
–1.017
–0.204
5065
0.710
1.065
0.392
0.000
–1.643
–0.110
5075
0.943
1.258
1.017
1.643
0.000
1.423
5085
0.470
0.588
0.204
0.110
–1.423
0.000
