4.2. Characterization of Indoor Air Flow for Different Configurations
Airflow pattern
As referred in section 3.2, six different situations were simulated to replicate summer, winter, and mid-season conditions, as listed in
Table 2. Numerical simulations show that the flow pattern inside the broiler building is quite complex and very much dependent on the thermal and dynamic initial conditions. This can be observed in
Figure 5, that shows the streamlines for S1 and MS2 configurations, with representation at half domain. For the S1 configuration, the flow pattern along the longitudinal direction (x-axis) is characterized by the formation of strong vortices immediately after the air enters in the domain, as clearly shown in
Figure 5(a). This pattern is also observed in MS1 configuration, and is even more intense for the winter configuration. The consequence is a significant variation of the local properties inside the domain for different initial conditions.
A different flow pattern is observed in the MS2 configuration (
Figure 5(b)). For this configuration, although in the initial zone of the air inlet the flow pattern is similar to that verified in S1, the longitudinal vortices of configuration S1 are not verified but, instead, the streamlines become linear and parallel to each other. This different behavior is due to the higher exhaust air flow rates imposed in the initial conditions. Thus, in this configuration, the inertial forces are larger than the viscous forces and turbulence almost disappears. In these cases, and at least for zones far away from the inlet, the flow is clearly characterized as a displacement flow, with higher predictability of local flow properties. This airflow pattern also promotes a better and effective removal of pollutants presented in the compartment. However, as a disadvantage, the higher flow velocity may cause discomfort. This will be confirmed in further figures showing NH
3 concentration and velocity profiles.
Figure 6 shows the velocity vectors in a vertical plane located at x=15 m, for configurations S1 and MS2. This Figure clearly confirms the flow complexity and the differences between these two configurations, with configuration MS2 showing two large vortices rotating in opposite directions. In configuration S1, the lower air temperature at the inlet forces the flow down, creating a single large vortex that proceeds downstream as seem in
Figure 5(a). In configuration MS2, the higher values of temperature and inlet air velocity originate a different flow pattern. In this case, two opposite recirculation cells are observed. This behavior is obviously strongly dependent of inlet and initial conditions, which, once again, originate the great local variability of the properties. So, special attention must be dedicated in the selection of the location of sample collection points in field measurements.
Ammonia distribution
Figure 7 shows the NH
3 volume fraction distribution in a horizontal plane located at z = 0.5 m from ground, for the 6 simulated configurations. As expected, concentration values increase from the inlet zone to the exhaust zone, as the fresh air entering the domain through the evaporative pad is contaminated by NH
3 released from the ground (i.e., litter material).
Mid-Season configurations are characterized by a significant exhaust ventilation rate, so the NH
3 is more effectively removed as can be observed in
Figure 7(d). This configuration is characterized by the tunnel (displacement) ventilation, with parallel streamlines along the tunnel. In the MS2 configuration, the NH
3 emission is similar to the S2 configuration; however, in MS2 the ventilation rate is 50% larger than in S2 configuration.
In Winter situations the outside air temperature, as well as, the exhaust ventilation rate is significant lower.
Figure 7(e) and (f) shows the contours of NH
3 concentration for these situations. Although in Winter situation the flow velocities are much lower, we can confirm that, just as in configurations S1 and S2, also in configurations W1 and W2 the NH
3 concentration increases in a considerable amount near the exhaust zones, at the tunnel exit. This also indicates that the exhaust flow rate imposed by the fans is not sufficient to efficiently remove the NH
3.
To better understand the NH
3 distribution, this property was averaged in the transversal y direction using 15 sampling points and plotted in
Figure 8 as function of the longitudinal x direction at height z=0.5 m and z=1.8 m. Although the vertical scale of the graph is limited to 30 mg/m
3 for better depicting the evolution of NH
3 concentration in the first half of the tunnel, NH
3 concentration reaches values larger than 40 mg/m
3 for configurations S1, S2, and W1.
From the
Figure 7 it may be concluded that NH
3 is efficiently removed from the building in configurations MS1, MS2 and W2. On the opposite, in configuration S1, S2, and W1 the NH
3 concentration substantially increases after the mid-length of the tunnel. It may be also noticed in
Figure 8 (a) and (b) that the NH
3 concentration distribution is rather similar at heights of z=0.5 m and z=1.8 m. Previous studies [
3,
4,
6] recommend a limit of 7.6 mg/m
3 (10 ppm) of NH
3 to maintain a good indoor air quality on broiler buildings, but the threshold values of 15.2 mg/m
3 (20 ppm) are recommended as limit for a short period exposure. Note that long-term NH
3 toxicity in the broiler building may increase the susceptibility of birds to the adverse effects of NH
3 even at 15.2 mg/m
3 [
4,
6].
Figure 9 represents the NH
3 concentration along the longitudinal x direction at y = 7.5 m, at constants heights from the ground z=0.5 m and z=1.8 m. Comparing these local concentration values obtained at a specific y transversal location with the concentration values averages over the transversal direction depicted in
Figure 8, it may be noted that, at least up to x=60 m, the local concentration values (
Figure 9(a)) are always higher. Thus, despite of the same trend observed, it may be concluded that the experimental point measurement methodology are, in this case, overestimating the values of gas concentration.
We can also underline that, taking into account the numerical results, it is verified that the NH
3 concentration at the outlets is much higher than the average values obtained in the longitudinal line, the average in the horizontal plane (cf.
Figures 8), and also the values measured experimentally at the 4 sample collection points (cf.
Figure 3). Thus, it is predicted that the methods that consist in collecting the gases at the outlet may overestimate the average concentration inside the building.
Velocity distribution
Figure 10 shows the velocity distribution colored with the local air velocity values, for all the configurations. Are also printed the average velocity values at z=0.5 m. Not surprisingly, the highest values of indoor air velocity are verified in configurations MS2 and S2, because these were also the configurations where the highest exhaust ventilation rates imposed in the numerical calculation. Particularly in MS2 configuration, there is a large central extension where velocity exceeds 2 m/s. The same occurs in configuration S2, but only in the area in front of the air inlets. The highest velocity values are observed at the outlet surface (exhaust fans). These high velocity areas are prone to cause more stress to the broilers. However, we must underline that these situations refer to the final stage of the growing period (day 30), characterize by low mortality rate, due to the greater broilers’ resistance. The opposite is verified for the winter configurations, and also for S1, with zones where the velocity doesn’t reach 1 m/s, representing difficulties for the removal of gaseous pollutants, in particular NH
3, as verified in
Figure 7 and
Figure 8.
For configurations W1 and W2, as the exhaust air flow rate are lower, the inner air velocities are also lower, with average velocity values 0.35 m/s and 0.49 m/s in plane z=0.5 m, for W1 and W2 configurations, respectively. In these configurations, as the inner air velocities are lower, it is verified that buoyancy forces are significant, overlapping the inertial forces of the longitudinal flow, which causes an increase in NH
3 concentration along the tunnel (cf.
Figure 9).
It can also be identified, in all situations, the existence of a recirculation and almost stagnation zone, near the lateral wall and immediately after the air intake, approximately between x=20 m and x=30 m.
Cited by [
15], [
31] reported that the optimum air velocity in individual boiler building should be in the range between 1.5 m/s and 2 m/s. In the present, numerical results identify several zones where air velocity is lower than 1 m/s, observed particularly in the Winter configurations, and higher than 2 m/s observed in MS2 configuration (cf.
Figure 10).