Diurnal Cycle of Heating and Water Vapor in the Metropolitan Area of Porto in Portugal

Abstract

In this work, it is investigated the Urban Heat Island (UHI) using conservative thermodynamic variables observed by surface weather stations on the Metropolitan Area of Porto (Oporto) in Portugal, under adiabatic conditions at the surface. These conditions are usually present and associated with the development of a mixture layer into the diurnal Convective Boundary Layer (CBL), which residual layer in the late afternoon defines the initial state for the development of the nocturnal UHI. Both the spatial structure and temporal variation of potential temperature and specific humidity were considered, along the hours and days of the year, from a statistical point of view, resulting in hourly climatology. Details of the hourly evolution of the meteorological variables on the Oporto surface are presented and discussed. Results show a seasonal variation of the potential temperature up to 17°C throughout the year, which is associated with horizontal thermal gradients that can control and trigger mesoscale circulations such as sea-land, urban and valley-mountain breezes.

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Karam, H. , Gonçalves, J. and Filho, A. (2022) Diurnal Cycle of Heating and Water Vapor in the Metropolitan Area of Porto in Portugal. Journal of Geographic Information System, 14, 61-77. doi: 10.4236/jgis.2022.141004.

1. Introduction

The total population of the world increased substantially in the last few decades [1]. For instance, the urban population of Europe corresponds to 72% or about 18% of the world’s urban population. A 2030 scenario indicates an increase of the urban population to 78% and a reduction to 11% of the rural population. Eventually, the urban population dwelling will be more dependent on job opportunities, services, infrastructure, and mobility, in a scenario of climatic change.

Urban areas have distinctive specific energy and water budgets tied to Urban Heat Island (UHI) effects such as lower specific humidity, higher air temperature, and precipitation, so that some mesoscale features are very important to understand atmospheric circulation in cities [2].

The Urban Heat Island also induces higher water and electrical energy consumption and a greater number of infrastructural and health hazards, particularly in association with heat waves occurrences such as that of 2003 in Europe. Indeed, local climate variability in cities and global changes require multidisciplinary studies in urban dwellings and time work schedule beyond increase of urban greening actions to mitigate not wanted urban heat island effects [3].

Oporto has 1.7 million inhabitants over an area of 1883 km2; 888 people km−2. Porto city is a major urban center with one of the highest population densities in Europe with 6400 people km−2. About 264 thousand people live in an urban area on the northern slope and plateau of 41 km2 on the Douro river valley with its highest altitude at 155 m above sea level [4] .

Some previous studies carried out for Porto City and Southern Portugal [5] [6] [7] [8] [9] focused on precipitation distribution and variability caused by surface winds, sea surface temperature (SST) along the coast of Southern Portugal, the North Atlantic Oscillation (NAO) and its bio-climatic classification [10] [11]. El Niño-Southern Oscillation (ENSO) and NAO have been studied as players in the Iberian Peninsula climate variability [12] [13] [14] [15] [16].

Heatwaves in Europe including Portugal are frequent. The relationship between atmospheric circulation, Sea Surface Temperature (SST), precipitation, and heatwave events over Western Europe have been investigated, as well the effect of extremely high temperatures on daily mortality rates in Lisbon and Madrid [17] [18]. A Watch Warning Surveillance System was built and updated for monitoring heat waves with potential impacts on morbidity and mortality, and a new approach to improve quantifying impacts of heat waves on mortality rates [19] [20].

The main features of Lisbon Urban Heat Island have been studied using a step-wise multiple regression and obtained a 2.5˚C difference value [21]. Another investigation has found temperature differences up to 7˚C due to the Oporto Urban Heat Island [22]. Additionally, the diurnal cycle of air pollutants and concentrations of CO, O3, NOx, and PM10 also has been carried out for the Oporto [23].

There are few published studies on the Oporto Urban Heat Island. Some researches point out that the Oporto Urban Heat Island is associated with the development of an Urban Boundary Layer (UBL) in a temperate climate zone. By hypothesis, the circulation cell generated by the Oporto Urban Heat Island can be coupled to the circulation cell of the sea-land breeze (SB) under favorable conditions. The coupling of the Oporto Urban Heat Island circulation with the SB circulation can occur in the absence of more intense synoptic flows (i.e., external forcing), for example, like those resulting from the movement of cold and warm fronts.

The interaction between the Oporto Urban Heat Island and SB circulations may be associated with the formation of storms over the urban conurbation or neighborhoods. These are theoretical aspects that can be better addressed from data analysis such as the one presented in this work. Observations and investigations of this type of UHI iterations exist for the Metropolitan Region of São Paulo (MASP) and the Metropolitan Region of Rio de Janeiro (MARJ) [24] [25] [26].

Noteworthy is the fact that the maximum intensity of the Urban Heat Island of the MASP and MARJ occurs in the afternoon and the morning, respectively, therefore in phase with the period of greatest heating of the surfaces by the density flux of solar radiation [27]. It is observed that the maximum of the MASP Urban Heat Island occurs almost synchronously with the entrance of the sea breeze, which brings relatively humid air with a lower temperature that advances over the urban conurbation of the MASP from Southeast to Northwest, in favorable feedback to the development of storms of greater vertical development over the city, so that it rains heavily on the city and not on the water sources that are located in the mountains to the north of the conurbation. Naturally, this has consequences for the availability of rain to recharge water sources, which can lead to a risk of shortages of drinking water in drier years (such as 2014) and erosion processes [28] [29].

Observational work and numerical modeling with mesoscale models for storm simulation show that these iterations are intense enough to intensify the vertical movement within the storms, thus generating severe storms, with hail and intense precipitation [30] [31].

Added to the higher urban temperature associated with the Oporto Urban Heat Island, the lower branch of the shallow circulation cell of the sea breeze that advects humid air over the urban area can reinforce the necessary conditions for the development of more intense storms (i.e., from a theoretical point of view). Studies by the Oporto Urban Heat Island are required to confirm these hypotheses.

Note the relevance of investigating the effects of the Oporto Urban Heat Island, given the increasing urbanization, the potential loss of thermal and environmental comfort, the worsening of the dangers associated with heat waves added to the higher temperatures of the urban surface and the increase in the frequency of severe storms under conditions of increased surface heating. Therefore, there is a need to investigate the hydrometeorological hazards associated not only with present and future global warming due to climate change (associated with the anthropogenic emission of greenhouse gases) but also due to surface land modifications. Urbanization is able to modify the energy and surface water balance [32] [33] [34] [35] [36].

In this way, carrying out systematic investigations on the Oporto Urban Heat Island can lead to a better understanding of the kinematics and dynamics of the Urban Heat Island itself and its interrelationships with the formation of intense storms, local and regional water availability, management of hydrometeorological hazards and epidemics, especially those associated with high temperatures such as the Dengue infectious disease, air pollution, hospitalizations, mortality. These issues have been evaluated by different researches, e.g., [37] [38] [39].

In this work, Oporto Urban Heat Island is analyzed using air potential temperature and air specific humidity under dry and adiabatic conditions. Database of automatic weather stations (AWS) mesonetwork is used to characterize the urban micro-climate of Oporto.

The need to investigate diurnal weather cycles in the Oporto originates from the fact that complex interactions in the Oporto Urban Heat Island often result from which interactions between mesoscale and synoptic weather processes. The joint analysis of diurnal and seasonal cycles of atmospheric variables has received increasing attention in the literature as data of higher sampling frequency (i.e., mesoscale) became available [40]. The main research purpose of this work is to show the importance of diurnal and seasonal variations in understanding the evolution of thermodynamic conservative variables during the Oporto Urban Heat Island evolution, evidencing the iterations between sea-land breeze and urban breeze cells associated with the development of the Oporto Urban Heat Island at diurnal and seasonal scales.

2. Methodology and Data

2.1. Conservative Thermodynamic Variables

The thermodynamics of the conservative variables under adiabatic conditions (for dry air) applied in this work were calculated using known from the atmospheric thermodynamic [41] [42].

2.2. Sazonal Surface Water Balance of Oporto

According to Köppen-Geiger’s climate classification (KGCC), Oporto has a subtropical climate Csb, of dry summer or the Mediterranean [42]. It is typical of western continental areas between latitudes 30˚ and 45˚N [43] [44].

The monthly averages of temperature T in (˚C) and precipitation P in (mm) for the city of Porto-PT, obtained from measurements in the period 1971-2000 [45] are shown in Figure 1. The temperature for summer varies between 10˚C and 22˚C and in winter between 0˚C and 18˚C. In the summer, precipitation accumulation is smaller than 40 mm and in the winter it increases up to 200 mm.

Oporto has a hot and dry summer due to the dominance of the subtropical high-pressure system. Oporto is located on the Northern coast of Portugal, being the Atlantic Ocean surface influenced by cold currents, associated with the frequency of fog occurrences.

Figure 1. Evolution of the monthly average of the temperature (˚C) and precipitation (mm) for Porto-PT, shown by continuous and dashed lines, respectively. Data source: [45].

The monthly average of the Surface Water Balance (SWB) [46] [47] can be written as

P S E Q = 0 (1)

where P is the precipitation rate; S ~ 0.05 P is the approximate infiltration rate responsible for the ground storage, E ~ 0.167 ETP represents the actual evaporation obtained as a function of the potential evapotranspiration (ETP) and Q is the surface runoff Here these fluxes are expressed in units of (mm month−1).

The monthly averaged surface water budget components for Oporto are presented in Figure 2. Precipitation (P) and surface runoff (Q) present almost the same magnitude because Oporto city surface is can be considered as being an impermeable surface due to the paved surface and small amount of surface vegetated in bare soil. Evaporation is higher during the hot and dry summer months, being modulated by the entry of the sea breeze of the Atlantic Ocean.

2.3. Study Area and Surface Weather Data

The study area in the center-north of Portugal includes the city of Porto and parts of the conurbations of Aveiro and Viseu. The geographic location of the network of surface weather stations (AWS) is shown by white stars in Figure 3. Available data between 1996-2009 were obtained concentrating data from the mirror Wunderground [48], reformatted to obtain with variables in columns and the sample time in rows.

The resulting file to each station presents a similar structure, which was employed in the analysis and comparisons. Unpaired data were excluded and the arithmetic averages and standard deviations were used for neglecting data with

Figure 2. Monthly evolution of the average surface water balance for Oporto-PT. The Key indicates the estimated values: potential evapotranspiration (EPT), precipitation (P), potential water availability (P-Ept), surface runoff (Q), and real evapotranspiration (E). Analysis: this work.

Figure 3. OPorto area (square symbol in the left side of the figure) and the location of the weather stations in this area, indicated by numbers and stars (in the right side of the figure). Key: (1) Braga; (2) Trofa; (3) Montes Burgos; (4) Pedras Rubras; (5) LPPR International Airport; (6) Farm of Chapel (Braga); (7) Leça da Palmeira; (8) Leça da Palmeira (Sardoal); (9) Guimarães; (10) Arada (Ovar).

large deviations from the mean (i.e., deviations bigger than two standard deviations). Following the equations proposed by Bolton [41], the development of conservative thermodynamic variables, for each day in the year and hour in the day, can be obtained and hourly values computed.

3. Results

3.1. The UHI and Thermal Atmospheric Circulation

The analysis of the micro-climates occurrences of Oporto was accomplished with temporal sections of conservative variables for adiabatic conditions along the year and hour of the day.

The LPPR AWS was used as a reference station because it presents the most complete dataset. This station is near to the international airport Francisco Sá Carneiro (longitude 41˚13'47.89"N; latitude 8˚40'47.90"W) at 64 m altitude (AMSL). The analysis of the variables for the LPPR station is shown in the present subsection. The statistical analysis was based on deviation fields is presented in the following subsection.

The surface air temperature presents similar characteristics to the potential temperature (Figure 4(a)). Since the surface air pressure is slightly higher than the reference air pressure (p0), the potential temperature is slightly smaller than the corresponding air temperature. The potential temperature variation during the summer is consistent with the solar radiation cycles (figure not shown), with variation between 7˚C and 12˚C in the winter, and 20˚C to 25˚C in the summer.

The surface air pressure, with a maximum during the winter (1020 - 1023 hPa) and almost constant on the rest of the year (1015 - 1018 hPa) (Figure 4(b)). High-pressure systems due to cold air masses in winter can cool the land surface faster than the ocean water surface. Fast warming of the surface in summer lowers surface air pressure conform the warm air ascends and produces surface convergence of the airflow. On the other hand, under dry conditions, convective rainfall is not frequent, but precipitation can occur when there is a low-pressure system centered over southern Iceland.

The specific humidity varies from 5 g·kg−1 in winter up to 12 g·kg−1 in summer (Figure 4(c)). Therefore, this variation in the surface water vapor content is responsible for the observed variations of the dew point temperature. The relative humidity (HR) (Figure 4(d)) is higher at night in summer (96%), mainly due to the decrease in the air temperature. On the other hand, RH is relatively lower (60%) during the afternoons. Air temperature decreases to a value near to the dew point temperature during the afternoons and evenings. A surface thermal inversion can yield a stable layer (i.e., the stable boundary layer) associated with fog conditions.

The equivalent potential temperature shows a strong seasonal oscillation from 20˚C in winter to 60˚C in summer (Figure 4(e)). It is an indication of hot and dry summers and rainy winters. The Oporto HR and the associated equivalent potential temperature (θe), a conservative variable under pseudo adiabatic conditions, are correlated in Oporto for both adiabatic and saturated conditions. High values of θe indicate the air parcel really must ascend more to reach the saturation condition (i.e., due to the adiabatic cooling). The surface HR is maximum

(a) (b) (c) (d) (e) (f)

Figure 4. Seasonal and diurnal cycle of measured meteorological variables for Oporto from 1996 to 2009: (a) potential temperature θ (˚C); (b) surface air pressure P (hPa); (c) specifics humidity q (g·kg−1); (d) relative humidity HR (%); (e) equivalent potential temperature θe (˚C); (f) and lift condensation level LCL (m).

in the afternoons of August (60%), which implies an increase in the frequency of the convective rainfall in this month.

The evolution of the lift condensation level (LCL) in Oporto inversely proportional to HR is presented in Figure 4(f). Late afternoon shows a height between 450 m and 650 m, and at night between 100 m and 200 m. The variations are as diurnal development of the atmospheric boundary layer, with the feature being a convective boundary layer (CBL) during the day and stable (SL) along the night. High solar radiation in the early afternoon further increases the height of the mixed layer in the CBL. Thus, the boundary-layer turbulence is efficient in mixing the water vapor from the surface into the mixing layer. At the same time, produces entrainment of relatively cool and dry air from the free atmosphere into the inside of the CBL, increasing the LCL height.

The wind field presents a major feature, which is the sea-land breeze, modulated by the seasons and presence of sloped terrain from west to east (Figure 5). In winter months the land breeze is prevailing during mornings and nights, associated with a thermal gradient, with negative signal, from the east for the west. In summer, and particularly in the afternoons, it is observed the circulation of the sea-land breeze, then associated with the reversion of the thermal gradient, now positive, from the east for the west. This positive gradient is increased due to the coupling of the sea-land breeze circulation with the valley-mountain circulation, being this last can be associated with the baroclinicity of the sloped terrain in mesoscale, elevating from the west for east. The temperature gradient is likely associated with the difference in the thermal capacity of the surfaces.

The wind direction is also influenced by the orientation of the coastline SW-NE. An almost constant phase of the sea breeze circulation is observed, from the morning (i.e., 1100 LT) to the end of the afternoon, with an intensification of the wind speed, which is likely a consequence of the increase of the surface temperature, particularly between March and October. A direct circulation intensity is proportional to the module of the horizontal thermal gradient, which implies

Figure 5. Climatology of the seasonal and diurnal cycle of the surface vector wind velocity for Oporto between 1996 and 2009. Colors indicate wind speed (m·s−1) and vectors, the horizontal wind direction.

the maximum wind speed of 3 m·s−1 from NW in the afternoon and 1.5 m·s−1 SE in the night.

3.2. Temporal Variability of the UHI of OPorto

In this subsection, the spatial variations of conservative variables are analyzed by comparing the time series of the network of AWS on OPorto, namely, potential temperature and relative humidity fields. The results for all AWS are compared. The AWS sites were separated using the annual average of the potential temperature (Figure 4) and the cross-correlation between each station and the LPPR station to the micro-climates discriminated due to the changes in surface use (e.g., urban to the rural area).

The discrimination criteria were defined by the simultaneous occurrence of ||<θ> − <θLPPR>|| > 2˚C and R2 > 0.95, where <θ> is the annual average of the potential temperature, for any weather station in the network, R2 is the coefficient of determination and <θLPPR> is the corresponding value for the reference station LPPR (Table 1). The AWS network was divided into just two groups of stations: group G1 = {LPPR, 2, 3, 4, 7, and 8} and group G2 = {1, 6, 9, and 10}. Figure 6 shows the average diurnal cycles for each AWS. The maximum potential temperature in group G2 (group G1) is 22˚C (18˚C) in the afternoons.

The stations of G2 have greater thermal amplitudes since they are further inland, where the sky view parameter is larger, which increases the shortwave incoming radiance flux during the day, as also the outgoing of thermal long-wave radiance along the night, under conditions of clear sky (i.e., in comparison with the shadows and the trapping long-wave radiance into urban canyons). Differences of 90 minutes of the phase of the thermal wave of groups G1 and G2 were observed, likely due to the large distance to the coast of group G2.

Figure 7 shows the seasonal and diurnal cycles of θ (left column) and HR

Table 1. Average potential temperature <θ> in (˚C) for each of the stations, the average thermal difference ||<θ> − <θLPPR>|| in (˚C), and the coefficient of determination (R2) about the reference station (LPPR).

(right column). Two well-defined seasons are evident: one relatively warm between June and September and a cold and rainy season between December and February. The relative humidity decreases in summer down to 60% (weather station G1) and 35% (for station G2) during the afternoons. The result indicates that the HR amplitude in spring (March to May) is higher than in autumn (October to November).

Figure 6. Diurnal evolution of the average potential temperature θ (˚C) between 1996 and 2009 as a function of the hour, for each AWS, as indicated in by the labels.

(a) (b) (c) (d) (e) (f)

Figure 7. Diurnal (x-axis) and seasonal (y-axis) mean cycles of the potential temperature (left column) and the relative humidity (right column) for AWS group G1 (a, b) and group G2 (c, d). The difference between the groups (G1 - G2) is shown in (e, f).

The diurnal cycle of potential temperature θ is forced by the net radiance density flux (Rn), which usually works as the major heat source at the surface. Observations of components of surface radiation balance are not available in the available data. The thermal amplitude reaches 4˚C for G1 and 12˚C for G2. The amplitude and the phase of the diurnal cycle of θ seem to be conditioned by the NW-SE orientation of the sea-land breeze circulation at the surface. The relative humidity shows values higher at night time and decreases to their minimum at near 1500 LT. The diurnal variation of HR in G2 is systematically higher than in group G1, being 45% for G1 and 20% for G2.

The UHI is commonly computed considering a) the spatial distribution of air temperature inside and outside of the urbanized area, or b) using just two characteristic weather stations, one for each land cover. However, three characteristic surfaces are present in Oporto: 1) sea surface, 2) urban surface, and 3) rural surface. On the other hand, the UHI of Oporto is also affected by this spatial distribution of surface sensible heat fluxes (H).

Theoretically, the heterogeneous distribution of H can create a UHI in a form of a dome over the city. Consequently, the urban breeze circulation can be formed and to couple with other mesoscale circulations present over there. Therefore, the circulation dynamics can be associated with the thermodynamic process. The sea breeze brings relatively dense, wet, and cold maritime air over the land surface, initially warm and dry, decreasing θ and increasing HR in G1.

The existence of a horizontal thermal gradient between the groups is analyzed based on the diurnal evolution of the average potential temperature θ (˚C) for each AWS. At 0400 LT, the thermal gradient is from G2 to G1, with a maximum intensity of 2˚C in 40 km from April to August and less in the other months. HR differences are small but in July is 10%. During afternoons (1500 LT), the θ structure is 7˚C smaller and HR is 25% greater. Thus, G1 is colder. In afternoons, Oporto presents better thermal comfort than further inland, but is subject to intense heat spells, as the one observed in 2003.

The spatial distribution of the potential temperature can be associated with thermal horizontal gradients. In the winter afternoons, it is observed a negative gradient of approximately −20˚C by 100 km, associated with larger SST about the continental surface temperature. Later spring and in the summer (i.e., from April to August), just before sunrise (0400 LT), there is a positive gradient of approximately 5˚C by 100 km, associated with the presence of the nocturnal UHI of Oporto and also of a smaller SST.

4. Conclusion

The main features of the Oporto Urban Heat Island were characterized by the potential temperature and relative humidity that have been analyzed between 1996 and 2009. Oporto results suggest hot and dry summer with temperatures between 17˚C and 25˚C and rainy winter with a mean temperature variation from 6˚C to 10˚C. Fog conditions were observed during summer mornings. The prevailing wind is from the southeast during the winter nights and mornings, from the northwest during summer afternoons. The maximum wind speed is 3 m·s−1 and is related to the local sea breeze circulation. Potential temperature difference reached 17˚C links to air mass sources effects. Two main thermal gradients were found during the year, the first from east to west of about 0.2˚C km−1 in summer afternoons, and a second one from west to east of 0.05˚C km−1 at 0400 LT between April and August. The analysis has shown the relevance of both the diurnal and seasonal cycles of thermodynamic variables to a better understanding of the Oporto micro-climates. Therefore, the results presented had shown the importance of diurnal and seasonal variation in understanding the behavior of the Oporto Urban Boundary Layer associated with the mesoscale sea-land thermal and humidity contrast, development of breeze circulation cells and Oporto Urban Heat Island at both diurnal and seasonal scales.

Acknowledgements

Thanks to Dr. Alfredo Rocha (UA-Portugal) and Dr. Edson P. Marques Filho (UFBA, Brazil) and for their comments that enriched the initial version of the manuscript. We also express thanks to the Institutode Geosciences (IGEOCCMN-UFRJ) and the support from CNPq. A.J.P.F is sponsored by Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq) under grant 302349/2017-6.

Conflicts of Interest

The authors declare no conflicts of interest regarding the publication of this paper.

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