The urban heat island (UHI) phenomenon and climate change have become the major concerns for city sustainability in the wake of global warming and rapid growth in urbanization. This has resulted in increased intensity of heat stress and worsened outdoor thermal environmental conditions in urban microclimates. Water bodies are among the most effective means to alleviate the UHI and improve the thermal environment of urban microclimates. The thermal comfort conditions are observed at the pedestrian's level in a horizontal direction and at different vertical levels by assessing the reduction in three variables: ambient air temperature, surface temperatures, and alteration of flow velocity. The water body model used in this simulation is first validated using the sub-configuration method by replicating a previous experimental study. Two different scenarios (one with a realistic setting and the other with a representative water body) were studied and the results show that, for isolated streets, the water bodies can effectively improve thermal comfort conditions by reducing ambient air temperature (i.e. a reduction of 0.9 °C) and surface temperature by 3.5 °C, thereby reducing energy consumption. Moreover, a significant increase in wind velocity was also observed reaching its maximum value at peak times of thermal stress.

  • Climate change adaptation through the blue landscape in real urban areas: evaluation through predicting its thermal performance under hot, humid climatic conditions, not only at the pedestrian's height but also at diverse vertical levels.

  • Water bodies can effectively improve thermal comfort conditions by reducing air temperature.

  • Urban water bodies cause a significant increase in wind velocity, thus improving ventilation.

Urban areas have grown rapidly since the last century and the urbanization phenomenon is going to accelerate further in the future (Angel et al. 2005). The urban areas develop microclimates that can be significantly affected by the urban heat island (UHI) effect which refers to the phenomenon of possessing a higher temperature in the urban area as compared to the non-urban surroundings (Sarrat et al. 2006; Kovats & Akhtar 2008; Moonen et al. 2012; Klemm et al. 2015). In addition, the growing intensity of climate change is adversely affecting the population and environment of urban areas across the world, including Pakistan, in the form of elevated outdoor temperatures (increased heat index), increased frequency of heatwaves, and urban flooding, among others (Oke 1982; Fischer et al. 2004; Stott et al. 2004; Haines et al. 2006; Mirzaei & Haghighat 2010). These high levels of rising outdoor temperature have a direct impact on the energy systems inside urban areas as these intensify the electricity demand (e.g. air conditioning and chilling), specifically at the time of high solar irradiance, up to 0.45–12.3% (Santamouris et al. 2015). Hence, there is a great interest and increased effort now to adapting the cities to the changing climate, UHI, and the resulting rising outdoor temperatures. This is usually done by changing the aerodynamic and bio-physical attributes of urban areas using some mitigation measures which alter the energy flux between the earth's surface and upper surfaces, resulting in the reduced intensity of the UHI (O'Malley et al. 2015; Shiflett et al. 2017). The common mitigation measures include water bodies (Syafii et al. 2017; Toparlar et al. 2018; Yang et al. 2020; Zeeshan et al. 2022b); vegetation (Toparlar et al. 2018; Zeeshan & Ali 2022a; Zeeshan et al. 2022b); urban geometry Jamei et al. (2016); surface materials Zeeshan & Ali (2022b); and reduction in heat emissions from the anthropogenic sources (Rizwan et al. 2008).

Water bodies, in the context of sustainable urban development, have shown significant potential for alleviating the UHI due to their high thermal and evaporative cooling capacity. Various types of techniques including field measurements and numerical simulations have been used to investigate the cooling effect of water bodies in real urban areas including rivers and ponds (Soultana & Gianniou 2007; Taleghani et al. 2014). Hathway & Sharples (2012) documented an average temperature decrease of 1 °C in Sheffield, UK due to the existence of the river during hot weather conditions. Chen et al. (2006) analyzed the mitigation effectiveness of a small lake in China using remote sensing techniques and observed an air temperature reduction of 1.3 °C. Theeuwes et al. (2013) studied the effectiveness of water bodies by implementing it into multiple small patches rather than one large landscape and witnessed its relatively high cooling effectiveness toward thermal regulation of the urban environment. Syafii et al. (2017) undertook an experimental study and found the same observations. Despite various experimental studies on water bodies in urban microclimates, this approach can be subjected to challenges owing to its inherited cons of providing data at only certain discrete locations and its poor hold on boundary conditions coupled with huge costs/endeavors. In contrast, the studies involving computational approaches such as computational fluid dynamics (CFD) are escalating owing to their ability to simulate the coupled effect of heat transfer, wind flow, and moisture transfer (Lun et al. 2009; Toparlar et al. 2015) with proper boundary conditions control and data gathering at any discrete point (Blocken 2014). However, the reliability of CFD results may be of concern which can be tackled with suitable validation studies such as the replication of the previous experimental study with CFD using the sub-configuration method (Tominaga et al. 2008; Franke et al. 2010; Blocken 2014). Yang et al. (2020) carried out a numerical study and found that the water bodies help modulate the thermal environment of urban areas causing a reduction of up to 2 °C, and promoting the wind flow. Sun & Chen (2012) conducted a numerical study on water bodies by focusing on their landscape parameters such as area, location, geometry, and percentage of built density; and documented their significance for regulating the thermal environment of urban microclimates. Tominaga et al. (2015) performed another numerical study and demonstrated a decrease of 2 °C with the use of water at pedestrian height in a real urban microclimate. In addition to temperature decrease, water bodies also cause the flow velocity to increase (Yang et al. 2020). On the flip side, it results in increased localized humidity, which makes achieving thermal comfort conditions very difficult in hot-humid urban areas as its mitigation potential/effectiveness weakens due to impaired transpiration.

The studies carried out so far have evaluated the performance of water bodies in regulating the thermal environment only at a horizontal scale, i.e. at pedestrian's height, and mostly in summer (Yang et al. 2020; Bartesaghi-Koc et al. 2021). However, their evaluations in a hot, humid climate such as the currently studied location have not been widely investigated which is necessary for carrying out a complete and meaningful analysis of water effectiveness toward promoting cooling in its surrounding environment (Haddad et al. 2020). Such climatic conditions impaired the transpiration process of water, thereby impacting its mitigation potential. Moreover, an assessment of the cooling potential of water bodies for regulating the outdoor thermal environment in isolated streets has not been completely executed. This is attributed to the availability of huge temporal variability and spatial heterogeneity in microclimatic/boundary conditions (Lai et al. 2019; Haddad et al. 2020), and the effect of urban geometry and the advection phenomenon at locations of isolated spaces (Berardi & Wang 2016; Jamei et al. 2016).

Therefore, this study aims to demonstrate that thermal comfort conditions of the urban environment, having hot, humid climatic conditions in isolated (open spaces) streets, can be improved with water bodies. In this regard, the unmitigated scenario without implementing water bodies is first simulated to model realistic climatic conditions of I. I. Chundrigarh road, a central area of Karachi, a city in Sindh province, Pakistan. Moreover, this case will serve as a reference for the subsequent assessment to identify and prioritize the hotspots for the incorporation of water bodies. To fulfill this study's aim, the finite volume method employing URANS equations was adopted to perform CFD simulations. The model used for the water body is first validated using the sub-configuration method based on its evaporation phenomenon. This study furnishes important information, in terms of scientific recommendation, and facilitates urban architects and policymakers regarding the implementation of the blue landscape for ameliorating the local environment of the studied microclimate and for enhancing the naturally enhanced ecosystem at the street, neighborhood, and city scales.

Study area

The mitigation potential of water bodies is accessed in the urban microclimate of Karachi, Pakistan which is the 12th most dense urban area in the world with respect to its population (Qureshi 2010; Sajjad et al. 2009, 2015). Another reason for studying this city is its vulnerability to severe heat index and frequent heatwaves resulting from the rapid increase in urbanization and climate change Kovats & Akhtar (2008). The sub-area of Karachi – ‘I. I. Chundrigarh Road’, as portrayed in Figure 1 – is selected for the current study as it is among the hottest regions in Karachi on summer days and has high humidity levels resulting from seawater evaporation. The selected study area is approximately 1.2 km and is modeled in CFD as a circular sub-domain having a radius of 500 m with the highest building height of 60 m. This location has longitude and latitude values of 25°86′ 07 ″ N and 67°00′ 11″ E with a time zone of +5 Greenwich Mean Time (Figure 1(a)–1(d)).
Figure 1

(a) Location of Karachi in Pakistan, (b) grid location of urban microclimate understudy in Karachi, Pakistan, (c) view of studied location and PMD observatory, and (d) aerial view of the area with surroundings, black circle encompassing the modeled zone.

Figure 1

(a) Location of Karachi in Pakistan, (b) grid location of urban microclimate understudy in Karachi, Pakistan, (c) view of studied location and PMD observatory, and (d) aerial view of the area with surroundings, black circle encompassing the modeled zone.

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Datasets description

To evaluate the thermal comfort conditions in the urban climate of I. I. Chundrigarh Road, Karachi Pakistan, the climatic parameters (Supplementary material, Dataset) used in the current study are obtained from the Kiamari station observatory managed by Pakistan Meteorology Department (PMD). The Kiamari station is positioned 10 m above ground level. This observatory is located 4 km away from the studied area. The hourly averaged meteorological data for air temperature (°C), relative humidity (%), wind speed (m/s), and wind direction were collected for the heatwave period (18–22 June 2015). The representative data for carrying out the study in this area are given in Table 1.

Table 1

Meteorological data

DateDuration (h)Sea pressure level (hpa)Average DBT (°C)Average relative humidity (%)Average wind speed (m/s)
18-6-15 0–5 am 999 32.5 69 1.4 
18-6-15 6–14 am 999 37.6 48.8 5.35 
18-6-15 15–23 am 999 33.2 62 3.43 
19-6-15 0–5am 997 34 58 1.54 
19-6-15 6–14 am 997 38.6 43.1 5.21 
19-6-15 15–23 am 997 32.8 71.1 2.75 
20-6-15 0–5am 994 34 61.3 2.16 
20-6-15 6–14 am 994 40.5 39 4.23 
20-6-15 15–23 am 994 35.2 58.7 
21-6-15 0–5am 995 35 53.1 1.33 
21-6-15 6–14 am 995 40.6 32.4 3.78 
21-6-15 15–23 am 995 37 44.7 3.1 
22-6-15 0–5am 995 35.3 54.3 3.1 
22-6-15 6–14 am 995 39.46 46.2 3.61 
22-6-15 15–23 am 995 34.9 58.3 2.73 
DateDuration (h)Sea pressure level (hpa)Average DBT (°C)Average relative humidity (%)Average wind speed (m/s)
18-6-15 0–5 am 999 32.5 69 1.4 
18-6-15 6–14 am 999 37.6 48.8 5.35 
18-6-15 15–23 am 999 33.2 62 3.43 
19-6-15 0–5am 997 34 58 1.54 
19-6-15 6–14 am 997 38.6 43.1 5.21 
19-6-15 15–23 am 997 32.8 71.1 2.75 
20-6-15 0–5am 994 34 61.3 2.16 
20-6-15 6–14 am 994 40.5 39 4.23 
20-6-15 15–23 am 994 35.2 58.7 
21-6-15 0–5am 995 35 53.1 1.33 
21-6-15 6–14 am 995 40.6 32.4 3.78 
21-6-15 15–23 am 995 37 44.7 3.1 
22-6-15 0–5am 995 35.3 54.3 3.1 
22-6-15 6–14 am 995 39.46 46.2 3.61 
22-6-15 15–23 am 995 34.9 58.3 2.73 

Numerical method

CFD numerical setting

The CFD simulations have been performed using a finite volume-based method (FVM) along with a realizable k–ε turbulence model in the commercially available tool ANSYS FLUENT 16.2 (Shih et al. 1995; ANSYS 2016). The governing flow equations for velocity and turbulence are solved through the URANS equations model. Moreover, the CFD simulations for modeling urban flow were performed using best practice guidelines of Tominaga et al. (2008); Franke et al. (2010). The SolidWorks computer-aided design (CAD) tool was adopted to model the buildings with their configurations for the studied microclimate. The standard wall function, as proposed by Launder & Spalding (1974) with modified sand grain-based roughness, was imposed on wall type boundaries to resolve the fluid–wall interaction. Zo, the aerodynamic roughness length of 0.03, is set for all buildings including ground inside the inner circular sub-domain while it ranges from 0.03 to 1 for ground surface outside of the circular sub-domain (Zeeshan et al. 2022a). Moreover, the equations of turbulence, energy, and mean flow are resolved with the use of a second-order discretization scheme to avoid numerical diffusion. The PISO algorithm, for its stability and application for transient flow, was used for pressure velocity coupling (Ansys 2016; Toparlar et al. 2018). The discrete ordinate (DO) radiation model was used to model the (transmissivity) transparency of water bodies (Yang et al. 2020). The solar irradiation and radiative transfer are handled with a solar-ray tracing model and converges set for study results at 10−5 for all variables except continuity 10−4 at the end of each time step.

Computational domain and grid discretization

The computational domain and discretization are compiled using the best practice guidelines of Blocken (2015). With the inner circular domain of 500 m with an average building height of 60 m as a reference in Figure 2(a), the domain computed has length, width, and height of 1,700, 1,100, and 360 m. The non-physical boundaries of the domain are kept at a distance of at least 5Hmax from the circular sub-domain except for the outflow which is at 15Hmax(Tominaga et al. 2008). The domain constructed with buildings for CFD simulations has a blockage ratio of less than 3% (Franke et al. 2010; Blocken 2015) in its streamwise direction. The discretization of the computational domain is done with Pointwise (2017). First, the surface mesh was generated on the ground, building surfaces, and computational domain boundaries, with at least 10 cells on each of the building elements with an expansion ratio of 1.25. High resolution of mesh on inner interested circular regions (Figure 2(b)) was used in order to resolve the flow field with sufficiently high resolution and for CFD coupling of temperature with velocity field. The resulting surface mesh contains both triangular elements with triangular cells of 21,617 and 732,365 quadrilateral elements. After completing the surface mesh, the volumetric mesh for the fluid domain is constructed using the surface-grid extrusion technique (T-Rex). The resulting volumetric mesh (basic) has around 23.1 million cells. To ensure the accuracy of the result with current discretization, grid sensitivity analysis was performed with tree mesh named course, basic and fine mesh with transformation factor of √(2) (Franke et al. 2010; Blocken 2015). The results of grid sensitivity analysis are reported in terms of air temperature, surface temperature, and velocity and are given in Supplementary material, Annexure A.
Figure 2

(a) Computational domain and (b) mesh for the circular sub-domain, buildings, grounds, and water bodies.

Figure 2

(a) Computational domain and (b) mesh for the circular sub-domain, buildings, grounds, and water bodies.

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Boundary conditions

The simulation is performed with the following inlet velocity and turbulence profiles, proposed by Richard (1997), selected based on their application with various turbulence models, and is mathematically described as:
(1)
(2)
(3)
where

where Z0, Κ, U*, Uref, and Cμ refer to the aerodynamic roughness length for building elements and ground, the von-Karman constant has a value of 0.42, the friction-velocity, velocity of the reference height (height of PMD Observatories).

The symmetry boundary conditions are applied at the lateral and top sides of the computational domain having zero gradients of all parameters. The pressure outlet condition is imposed at the outflow. The buildings inside the circular sub-domain and the ground of the computational domain correspond to the wall. The building is modeled implicitly with an equivalent thickness of 0.35 m with enabled conduction equations and is treated as air-conditioned at a temperature of 23 °C. The thermal and radiation conditions, imposed on walls, have a heat transfer coefficient of 0.5 W.m−2.K−1, free stream temperature, and radiation temperature of 23 °C, in the water zone with heat flux obtained from Equations (4)–(9). The water and ground are modeled with 1 and 10 m thicknesses. At this ground depth, zero heat flux is imposed. The detailed properties of the material for all surface elements are given in Table 2.

Table 2

Material specifications and components used in this study (Lin et al. 2019)

MaterialThermal conductivity (W·m·K−2)Specific heat (J·kg·K−1)Density (kg·m−3)EmissivityAbsorptivityThickness (m)
Earth 1.3 1,000 1,400 0.9 0.68 0.15/0.15/0.05 
Brick 0.8 900 2,000 0.9 0.8 0.35 
Earth with concrete 1.5 300 1,600 0.85 0.85 0.5/9.5 
Water 0.59 4,187 1,000 0.95 0.9 1.0 
Limestone 908 1.3 1,090  Not a surface material  
Insulation 1,200 0.03 50 – Not a surface material  
MaterialThermal conductivity (W·m·K−2)Specific heat (J·kg·K−1)Density (kg·m−3)EmissivityAbsorptivityThickness (m)
Earth 1.3 1,000 1,400 0.9 0.68 0.15/0.15/0.05 
Brick 0.8 900 2,000 0.9 0.8 0.35 
Earth with concrete 1.5 300 1,600 0.85 0.85 0.5/9.5 
Water 0.59 4,187 1,000 0.95 0.9 1.0 
Limestone 908 1.3 1,090  Not a surface material  
Insulation 1,200 0.03 50 – Not a surface material  

Modeling the effects of water bodies

The heat exchange in the water bodies is usually associated with convection, radiation, and evaporation to its surrounding medium. Mathematically, the net heat exchanged through these three phenomena is given as:
(4)
where , , , , and are the absorptions of shortwave radiation of the sun at the surface of the water, longwave radiation emitted by water top surface, heat dissipation due to evaporation, the heat took place due to convection, and incoming longwave radiations in W/m2, respectively. The mathematical equations for these variables are given as:
(5)
(6)
(7)
(8)
(9)
where , Wz refers to the velocity of wind at reference height above the water surface. and are water and air temperature at a height of 2 m above the water zone.

The mean radiation of the sun for the studied climate for a given heatwave period, as calculated from equations of radiation, was 164.6 W/m2 and is denoted with I. , , and represent the water reflectivity of water for solar shortwave radiation, longwave radiation, and the atmosphere; their average values are 0.1, 0.03, and 0.97. are the air saturated vapor pressure and evaporation pressure of air near water, expressed in mmHg. The resulting heat flux for the water zone, computed using Equations (4)–(9), is incorporated into the governing energy equation.

This section is comprised of two sub-sections which are: Validation studies given in Section 3.2 and thermal effects of water bodies, given in Section 3.3. Before simulating the water bodies’ effectiveness, a base case simulating the existing conditions was modeled which served as a reference case for predicting the water effectiveness and for identification of locations to propose representative water bodies. The cooling effect has been given in terms of hourly average data for 19 June 2015; and in terms of cooling intensity evaluated at the pedestrian height at selected horizontal and vertical planes for 1500 LST.

Base case and evaluation zone identification

To make a comparative assessment of the cooling effect of water bodies inside a hot-humid urban microclimate, the reference case was first modeled without incorporating the representative water zone inside the studied microclimate. The purpose of this modeling scenario was threefold: first, the identification of hotspots for water bodies’ intervention; second, modeling the in situ conditions of the heatwave period; and third, validation of surface temperature results obtained from satellite data with the current study. To model this case, the input parametrized conditions for velocity, temperature, and humidity were taken from the meteorological service and embedded into the inlet velocity and turbulent profiles. Based on the magnitude of these variables, 15 unsteady modeling scenarios were simulated (Table 1). The simulations were performed using a finite volume method using the URANS equation with numerical settings, described in Section 2.3, for a complete 5-day heatwave period (18–22 June 2015). The results were reported in terms of surface temperature contours for two different instances of days. It can be seen from Figure 3 that higher surface temperature was present in isolated spaces, i.e. street trees, and lower temperature at building facades and vertical envelopes. This pattern of surface temperature distribution was attributed to proliferated impervious surfaces at street trees and shorter solar access at vertical building envelopes. Based on the temperature distribution, the isolated streets were chosen for incorporation of artificial water bodies for appraising their mitigation effectiveness. The zones evaluated in such open spaces are depicted in Figure 3 with evaluation planes for ascertaining the cooling intensity. Three areas (first, second, and third zones) were selected in the urban microclimate to analyze the effectiveness of water bodies in modulating the studied urban area. Two layers of water bodies with center free space, each having approximately 10 m × 350 m water surface area in 1st zone and one layer of water bodies in each 2nd and 3rd zone with approximately 10 m × 400 m surface area, were modeled to predict their effect on pedestrian thermal comfort in narrower and wide-open spaces. Moreover, one representative plane was marked to evaluate the cooling intensity in both the horizontal and vertical direction and is given in Figure 4.
Figure 3

(a) Color ramp of surface temperature: (a) 11 am and (b) 3 pm.

Figure 3

(a) Color ramp of surface temperature: (a) 11 am and (b) 3 pm.

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Figure 4

(a) Representation of water zones highlighted in red color and (b) horizontal cross-sectional/wake planes highlighted in purple color, and the vertical plane in green color. Please refer to the online version of this paper to see this figure in colour: http://dx.doi.org/10.2166/wcc.2023.363.

Figure 4

(a) Representation of water zones highlighted in red color and (b) horizontal cross-sectional/wake planes highlighted in purple color, and the vertical plane in green color. Please refer to the online version of this paper to see this figure in colour: http://dx.doi.org/10.2166/wcc.2023.363.

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The validation of surface temperature obtained from current study results was made with MODIS (Moderate-resolution Imaging Spectroradiometer) satellite data and has also been described in detail in the study by Zeeshan et al. (2022a, 2022b). MODIS, with its bandwidth of 3.66–3.84 nm and resolution of 1 km, was used as it has been extensively applied to validate CFD results in urban microclimates (Montazeri et al. 2015; Toparlar et al. 2018; Antoniou et al. 2019; Zeeshan et al. 2022b).

Validation of the evaporation from a small-scale water surface

The validation study for modeling the thermal effect of water on the surrounding environment was also performed by employing heat flux at the water surface. The wind tunnel experiment data of Kato & Nakane (2009) was taken as a reference. They examined the basic mechanism of evaporation from the water surface in the wind tunnel by maintaining steady-state conditions. For this validation, steady-state simulations were performed and compared with the measured data. The computational domain was modeled as per the actual wind tunnel domain which had a dimension of 3 m × 1 m × 0.98 m along streamwise, lateral, and vertical sides, respectively. The water depth was taken as 20 cm. The domain discretization contained a structured mesh with 50, 20, and 60 cells along x, y, and z dimensions, and meshing was performed in the POINTWISE meshing tool. The wall adjacent cell height was kept at 0.005 m. The computational domain had one inlet, one outlet, and symmetry at the top and lateral sides. The bottom of the ground was assigned as a wall with water at a temperature of 16 °C. At the inlet, the profile of turbulent properties and velocity was assigned according to Equations (1)–(3) with Uref as 3 m/s and href 0.3 m. The air inlet temperature and humidity of 20 °C and 8 g/kg, respectively, were used. The results were compared in normalized form with these values as reference.

Figure 5(a) and 5(c) shows the comparison of CFD results with wind tunnel data in terms of air temperature and mass fraction while Figure 5(b) and 5(d) shows the regression analysis results for these two variables. The comparisons have been made for two different heights above the water surface. The results depicted a gradual decrease in temperature and a gradual increase in humidity along with the flow directions. Ansys and ENVI-met usually tend to overestimate the temperature and under-evaluate the humidity. Such behavior of CFD tools has also been highlighted by Yang et al. (2013) and Lee et al. (2016). This effect was profound near the water surface owing to relatively low velocity near the surface. The CFD-based temperature profile was quite consistent with the results of a wind tunnel without a significant difference between the two approaches at certain points. However, the CFD simulation showed only a moderate agreement for humidity. Since, the primary focus was on the temperature computation for which a reasonable/fair agreement between the measurement and simulated data was obtained, thus it was considered satisfactory for validation. It can be observed that a fairly good agreement is exhibited between the surface temperatures of the two approaches as R2 value is quite close to 1 (see Figure 5(b) and 5(d)).
Figure 5

(a and b) Comparison of air temperature between CFD and Tominaga study along with regression analysis. (c and d) Comparison of relative humidity along with regression analysis.

Figure 5

(a and b) Comparison of air temperature between CFD and Tominaga study along with regression analysis. (c and d) Comparison of relative humidity along with regression analysis.

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Results and discussion

24-hourly distribution: impact of water thermal effect

The 24-hourly distribution of air temperature, surface temperature, and flow velocity for the aforementioned two cases is given in Figure 6.
Figure 6

24-hourly distribution of (a) air temperature and (b) surface temperature.

Figure 6

24-hourly distribution of (a) air temperature and (b) surface temperature.

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It can be seen from Figure 6(a) that air temperature decreased with the incorporation of water bodies inside the urban microclimate at all time intervals of the day. The mitigation potential was more abundant/prominent at the time of high solar irradiance, owing to the availability of larger energy for evaporation generating more latent heat (Syafii et al. 2017). The maximum temperature reduction that occurred with water bodies was around 0.9 °C at 2 pm. This reduction was mainly attributed to its water thermal capacity, causing an increase in flow velocity, facilitating heat convection between air and its surroundings, thereby resulting in thermal evaporative dissipation and atmospheric turbulence. These phenomena then caused temperature gradients to develop between the water top zone and its surrounding air, discouraging positively sensible heat flux for generating more latent heat to cause cooling. The reduction of 0.9 °C in air temperature, with the use of water bodies, is in line with previous study results (Syafii et al. 2017; Jacobs et al. 2020; Yang et al. 2020). This lessening of temperature has a direct impact on the urban energy systems such as air conditioning applications since lesser temperature put forth lower electricity demand, particularly at times of high solar irradiance (Santamouris et al. 2015). The promoted cooling effect also contributes to energy savings inside urban microclimates (Akbari et al. 2016; Morakinyo et al. 2018). Similiar to air temperature, water bodies also contributed to lowering the surface temperature of urban surfaces by up to 3.5 °C (Figure 6(b)) as it absorbed more solar radiation due to their thermal capacity, causing a decrease in the surface temperature of surrounding elements/surfaces.

Temperature distribution (horizontal and vertical)

The intensity of the cooling effect of water bodies, both in the horizontal and vertical direction, has been reported in Figure 7 for 15 00 LST. The water bodies, owing to their larger thermal capacity, held a lower temperature over their area in comparison with their surrounding environment as is clearly portrayed in Figure 7(b). This cooling effect was attributed to the water thermal capacity with its representative area of 4,000 m2 in every four layers which promoted the absorption of the incoming solar radiation. This then increased the latent heat by reducing the sensible heat for the surroundings, developing the slight water surface to air temperature gradient, resulting in a negative sensible heat flux to grow. Moreover, advection and urban geometry had a strong effect on the mitigation potential in such isolated streets. This was attributed to hot air routing through these isolated street canyons from the surrounding geometric elements due to differences in pressure and temperature (Ahmadi et al. 2019; He et al. 2020). With water bodies, the intensity of cooling was about 0.9 °C (see Figure 7(c)). The results are quite comparable with those of Manteghi et al. (2015); Zhao & Fong (2017); Ampatzidis & Kershaw (2020); and Triyuly et al. (2021). However, this effect was insignificant in the crosswind spatial direction as is evident from Figure 7(d) and 7(e), owing to lower dispersion of cooling effect than advection in the crosswind direction because of having streamlined wind direction along the water length. This was also attributed to small areas of water bodies and their slim-line arrangement, enough to diffuse the cooled air far from their immediate surroundings.
Figure 7

(a) Representation of wake and vertical planes, (b) contours of air temperature at the wake plane for water bodies, 1500 LST, 19 June 2015, (c) contours of air temperature difference, water minus SAF at the wake plane, (d) contours of air temperature for water bodies at the vertical plane, and (e) contours of air temperature difference, water minus SAF at the vertical plane.

Figure 7

(a) Representation of wake and vertical planes, (b) contours of air temperature at the wake plane for water bodies, 1500 LST, 19 June 2015, (c) contours of air temperature difference, water minus SAF at the wake plane, (d) contours of air temperature for water bodies at the vertical plane, and (e) contours of air temperature difference, water minus SAF at the vertical plane.

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Flow velocity

Figure 8(b) shows the diurnal variation of the average flow velocities for the cases with water. It can be seen from Figures 8(c) and 8(e) that incorporating water bodies inside the urban microclimate had also contributed to promoting flow velocities both in streamwise and lateral directions. This increase in flow velocity with water bodies further promoted ventilation, resulting in a low heat accumulation phenomenon and a better livable environment. The velocity increase largely appeared in the region of water and its immediate vicinity (see Figure 8(b)–8(e)), and was attributed to a temperature difference between the water and waterless ground due to its high thermal capacity which promotes wind flow. The velocity increase was also due to the blockage of wind by the building surfaces owing to their larger roughness compared to water. This increase in velocity is consistent with the results of a previous study (Syafrina et al. 2020; Yang et al. 2020). However, the velocity increasing effect was somewhat less in crosswind directions as is clear from Figure 8(e) and 8(f).
Figure 8

24-hourly distribution of velocity. (a) Representation of wake and vertical planes, (b) contours of wale velocity with water bodies, 1500 LST, 19 June 2015, (c) contours of wake velocity difference, water minus SAF, (d) contours of velocity with water bodies at the vertical plane, and (e) contours of velocity difference, water minus SAF at the vertical plane.

Figure 8

24-hourly distribution of velocity. (a) Representation of wake and vertical planes, (b) contours of wale velocity with water bodies, 1500 LST, 19 June 2015, (c) contours of wake velocity difference, water minus SAF, (d) contours of velocity with water bodies at the vertical plane, and (e) contours of velocity difference, water minus SAF at the vertical plane.

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The present study aimed to perform the CFD simulations for evaluating the cooling potential of water bodies for the heatwave period 18–22 June 2015 in the hot-humid climate of I. I. Chundrigarh road, Karachi, Pakistan. The CFD simulations were performed using an FVM employing URANS equations. The water bodies model adopted in this study was evaluated and validated through the sub-configuration method. Surrounding temperatures and wind velocity were appraised to evaluate the thermal influence of water. Following are the major conclusions implied from this study's results:

  • (1)

    With respect to the water bodies simulation case, the thermal evaporative model with no inclusion of anthropogenic heat sources, as adapted in this study, had proven to have good accuracy, as validated through the sub-configuration method.

  • (2)

    Under heatwave and summer conditions, incorporating water bodies inside urban areas could effectively contribute to its thermal environment regulation, i.e. improving the ventilation and decreasing the thermal stress of pedestrians.

    • (a)

      For airflow velocity, it was significantly increased by 0.2 m/s in water areas compared to its surroundings which is attributed to temperature difference between water bodies and around hard ground situations.

    • (b)

      For air temperatures and surface temperatures, these were reduced by 0.9 and 3.5 °C as increased airflow velocity expedites the convected heat to/from air to surroundings causing evaporative thermal dissipation. This facilitates temperature gradients at the water surface to air to develop coupled with atmospheric turbulence, affecting negative sensible heat flux, resulting in lower ambient temperatures. It is thus inferred that water heat capacity could play a part in decreasing surrounding temperatures.

  • (3)

    The effect of temperature reduction and improved wind velocity could also influence its surroundings with greater effect in its immediate vicinity.

Nevertheless, water effectiveness in regulating the microclimate and assisting in air cooling varies with the availability of thermal energy, the intensity of climatic parameters (air temperature, relative humidity, velocity), water body properties (quality, depth, area), and surrounding area around water as they significantly influence the microclimate around it so additional simulations are required to gain knowledge of how these parameters affect cooling which would be helpful for designers/planners in designing natural ecosystem services. Moreover, the missing aspects, i.e. the relevant inlet profiles for different atmospheric conditions and anthropogenic heat sources, are proposed to be studied for future research work since their application would ensure and improve the result integrity.

The authors are highly thankful to PMD for providing environmental data for the heatwave period of 2015.

All relevant data are included in the paper or its Supplementary Information.

The authors declare there is no conflict.

Akbari
H.
,
Cartalis
C.
,
Kolokotsa
D.
,
Muscio
A.
,
Pisello
A.
,
Rossi
F.
,
Santamouris
M.
,
Synnefa
A.
,
Wong
N.
&
Zinzi
M.
2016
Local climate change and urban heat island mitigation techniques – The state of the art
.
Journal of Civil Engineering and Management
22
(
1
),
1
16
.
Ampatzidis
P.
&
Kershaw
T.
2020
A review of the impact of blue space on the urban microclimate
.
Science of the Total Environment
730
,
139068
.
Angel
S.
,
Sheppard
S.
,
Civco
D.
,
Buckley
R.
,
Chabaeva
A.
,
Gitlin
L.
&
Perlin
M.
2005
The Dynamics of Global Urban Expansion
.
World Bank, Transport and Urban Development Department
,
Washington, DC
, p.
205
.
ANSYS
2016
ANSYS Fluent
.
ANSYS, Inc
,
Canonsburg
.
Antoniou
N.
,
Montazeri
H.
,
Neophytou
M.
&
Blocken
B.
2019
CFD simulation of urban microclimate: validation using high-resolution field measurements
.
Science of the Total Environment
695
,
133743.
Bartesaghi-Koc
C.
,
Haddad
S.
,
Pignatta
G.
,
Paolini
R.
,
Prasad
D.
&
Santamouris
M.
2021
Can urban heat be mitigated in a single urban street? monitoring, strategies, and performance results from a real-scale redevelopment project
.
Solar Energy
216
,
564
588
.
Berardi
U.
&
Wang
Y.
2016
The effect of a denser city over the urban microclimate: the case of Toronto
.
Sustainability
8
,
822
.
doi:10.3390/su8080822
.
Blocken
B.
2014
50 years of computational wind engineering: past, present, and future
.
Journal of Wind Engineering and Industrial Aerodynamics
129
,
69
102
.
Chen
X. L.
,
Zhao
H. M.
,
Li
P. X.
&
Yin
Z. Y.
2006
Remote sensing image-based analysis of the relationship between urban heat island and land use/cover changes
.
Remote Sensing of Environment
104
(
2
),
133
146
.
Fischer
P. H.
,
Brunekreef
B.
&
Lebret
E.
2004
Air pollution related deaths during the 2003 heat wave in The Netherlands
.
Atmospheric Environment
38
(
8
),
1083
1085
.
Franke
J.
,
Hellsten
A.
,
Schlünzen
H.
&
Carissimo
B.
2010
The Best Practise Guideline for the CFD simulation of flows in the urban environment : an outcome of COST 732
. In:
The Fifth International Symposium on Computational Wind Engineering (CWE2010)
, pp.
1
10
.
Haddad
S.
,
Paolini
R.
,
Ulpiani
G.
,
Synnefa
A.
,
Hatvani-Kovacs
G.
,
Garshasbi
S.
,
Fox
J.
,
Vasilakopoulou
K.
,
Nield
L.
&
Santamouris
M.
2020
Holistic approach to assess co-benefits of local climate mitigation in a hot humid region of Australia
.
Scientific Reports
10
(
1
),
1
17
.
Haines
A.
,
Kovats
R. S.
,
Campbell-Lendrum
D.
&
Corvalan
C.
2006
Climate change and human health: impacts, vulnerability and public health
.
Public Health
120
(
7
),
585
596
.
Jacobs
C.
,
Klok
L.
,
Bruse
M.
,
Cortesão
J.
,
Lenzholzer
S.
&
Kluck
J.
2020
Are urban water bodies really cooling?
Urban Climate
32
,
100607
.
Jamei
E.
,
Rajagopalan
P.
,
Seyedmahmoudian
M.
&
Jamei
Y.
2016
Review on the impact of urban geometry and pedestrian level greening on outdoor thermal comfort
.
Renewable and Sustainable Energy Reviews
54
,
1002
1017
.
Kato
T.
&
Nakane
K.
2009
Fundamental experiment of evaporation mechanism on small scale water surface
.
Proceedings of Hydraulic Engineering, Japan Society of Civil Engineers
53
,
343
348
.
(in Japanese)
.
Klemm
W.
,
Heusinkveld
G.
,
Lenzholzer
S.
,
Jacobs
H.
&
Van Hove
B.
2015
Psychological and physical impact of urban green spaces on outdoor thermal comfort during summertime in The Netherlands
.
Building and Environment
83
,
120
128
.
Kovats
S.
&
Akhtar
R.
2008
Climate, climate change and human health in Asian cities
.
Environment and Urbanization
20
(
1
),
165
175
.
Launder
E.
&
Spalding
B.
1974
The numerical computation of turbulent flows
.
Computer Methods in Applied Mechanics and Engineering
3
(
2
),
269
289
.
Lin
H.
,
Xiao
Y.
,
Musso
F.
&
Lu
Y.
2019
Green façade effects on thermal environment in transitional space: field measurement studies and computational fluid dynamics simulations
.
Sustainability (Switzerland)
11
(
20
),
1
21
.
Lun
I.
,
Mochida
A.
&
Ooka
R.
2009
Progress in numerical modelling for urban thermal environment studies
.
Advances in Building Energy Research
3
(
1
),
147
188
.
Manteghi
G.
,
Bin Limit
H.
&
Remaz
D.
2015
Water bodies an urban microclimate: a review
.
Modern Applied Science
9
(
6
),
1
12
.
Mirzaei
A.
&
Haghighat
F.
2010
Approaches to study urban heat island – abilities and limitations
.
Building and Environment
45
(
10
),
2192
2201
.
Montazeri
H.
,
Blocken
B.
&
Hensen
J.
2015
CFD analysis of the impact of physical parameters on evaporative cooling by a mist spray system
.
Applied Thermal Engineering
75
,
608
622
.
Moonen
P.
,
Defraeye
T.
,
Dorer
V.
,
Blocken
B.
&
Carmeliet
J.
2012
Urban physics: effect of the micro-climate on comfort, health and energy demand
.
Frontiers of Architectural Research
1
(
3
),
197
228
.
Oke
T. R.
1982
The energetic basis of the urban heat island
.
Quarterly Journal of the Royal Meteorological Society
108
(
455
),
1
24
.
O'Malley
C.
,
Piroozfar
P.
,
Farr
E.
&
Pomponi
F.
2015
Urban Heat Island (UHI) mitigating strategies: a case-based comparative analysis
.
Sustainable Cities and Society
19
,
222
235
.
Pointwise
I.
2017
Available from: https://www.pointwise.com.
Qureshi
S.
2010
The fast growing megacity Karachi as a frontier of environmental challenges: urbanization and contemporary urbanism issues
.
Journal of Geography and Regional Planning
3
(
11
),
306
321
.
Richard
P. J.
1997
Appropriate boundary conditions for computational wind engineering models using k-e turbulence model
.
Journal of Wind Engineering and Industrial Aerodynamics
47 & 46
,
145
153
.
Rizwan
A. M.
,
Dennis
L. Y. C.
&
Liu
C.
2008
A review on the generation, determination and mitigation of Urban Heat Island
.
Journal of Environmental Sciences
20
(
1
),
120
128
.
Sajjad
S. H.
,
Hussain
B.
,
Khan
M. A.
,
Raza
A.
,
Zaman
B.
&
Ahmed
I.
2009
On rising temperature trends of Karachi in Pakistan
.
Climatic Change
96
(
4
),
539
547
.
Sajjad
S.
,
Blond
N.
,
Batool
R.
,
Shirazi
S.
,
Shakrullah
K.
&
Bhalli
M.
2015
Study of urban heat island of Karachi by using finite volume mesoscale model
.
Journal of Basic & Applied Sciences
11
,
101
105
.
Sarrat
C.
,
Lemonsu
A.
,
Masson
V.
&
Guedalia
D.
2006
Impact of urban heat island on regional atmospheric pollution
.
Atmospheric Environment
40
(
10
),
1743
1758
.
Shiflett
S. A.
,
Liang
L. L.
,
Crum
S. M.
,
Feyisa
G. L.
,
Wang
J.
&
Jenerette
G. D.
2017
Variation in the urban vegetation, surface temperature, air temperature nexus
.
Science of the Total Environment
579
,
495
505
.
Shih
W.
,
Liou
A. S.
&
Zhu
J.
1995
A new kt eddy viscosity model for high Reynolds number turbulent flows
.
Compurers Fluids
24
(
3
),
227
238
.
199
.
Soultana
K.
&
Gianniou
V. Z. A.
2007
Evaporation and energy budget in lake Vegoritis, Greec
.
Journal of Hydr
345
,
212
223
.
Stott
P. A.
,
Stone
D. A.
&
Allen
M. R.
2004
Human Contribution to the European Heatwave of 2003
.
Sun
R.
&
Chen
L.
2012
How can urban water bodies be designed for climate adaptation?
Landscape and Urban Planning
105
(
1–2
),
27
33
.
Syafii
N. I.
,
Ichinose
M.
,
Kumakura
E.
,
Chigusa
K.
,
Jusuf
S. K.
&
Wong
N. H.
2017
Enhancing the potential cooling benefits of urban water bodies
.
Nakhara: Journal of Environmental Design and Planning
13
,
29
40
.
Syafrina
A.
,
Koerniawan
M. D.
,
Novianto
D.
&
Fukuda
H.
2020
Influence of urban water body on thermal environment in Pontianak City
.
Journal of Asian Institute of Low Carbon Design
2020
,
163
166
.
Taleghani
M.
,
Sailor
J.
,
Tenpierik
M.
&
van den Dobbelsteen
A.
2014
Thermal assessment of heat mitigation strategies: the case of Portland state university, Oregon, USA
.
Building and Environment
73
,
138
150
.
Theeuwes
E.
,
Solcerová
A.
&
Steeneveld
J.
2013
Modeling the influence of open water surfaces on the summertime temperature and thermal comfort in the city
.
Journal of Geophysical Research Atmospheres
118
(
16
),
8881
8896
.
Tominaga
Y.
,
Mochida
A.
,
Yoshie
R.
,
Kataoka
H.
,
Nozu
T.
,
Yoshikawa
M.
&
Shirasawa
T.
2008
AIJ guidelines for practical applications of CFD to pedestrian wind environment around buildings
.
Journal of Wind Engineering and Industrial Aerodynamics
96
(
10–11
),
1749
1761
.
Toparlar
Y.
,
Blocken
B.
,
Vos
P.
,
Van Heijst
F.
,
Janssen
D.
,
Van Hooff
T.
,
Montazeri
H.
&
Timmermans
P.
2015
CFD simulation and validation of urban microclimate: a case study for Bergpolder Zuid, Rotterdam
.
Building and Environment
83
,
79
90
.
Toparlar
Y.
,
Blocken
B.
,
Maiheu
B. V.
&
van Heijst
F.
2018
The effect of an urban park on the microclimate in its vicinity: a case study for Antwerp, Belgium
.
International Journal of Climatology
38
,
e303
e322
.
Triyuly
W.
,
Triyadi
S.
&
Wonorahardjo
S.
2021
Synergising the thermal behaviour of water bodies within thermal environment of wetland settlements
.
International Journal of Energy and Environmental Engineering
12
(
1
),
55
68
.
Yang
L.
,
Liu
X.
&
Qian
F.
2020
Research on water thermal effect on surrounding environment in summer
.
Energy and Buildings
207
,
109613
.
Zeeshan
M.
&
Ali
Z.
2022a
Heat Stress Mitigation in urban streets having Hot-Humid climatic conditions: strategies and performance results from a real scale retrofitting project
.
Science and Technology for the Built Environment
0
(
0
),
1
23
.
Zeeshan
M.
&
Ali
Z.
2022b
The potential of cool materials towards improving thermal comfort conditions inside microclimate
13
(
1
),
56
72
.
Zeeshan
M.
,
Ali
Z.
,
Sajid
M.
,
Ali
M.
&
Usman
M.
2022a
Modelling the cooling effectiveness of street trees with actual canopy drag and real transpiration rate under representative climatic conditions
.
Journal of Building Performance Simulation
doi:10.1080/19401493.2022.2080865
.
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