1. Introduction
Until the first quarter of the 20th century, the main roofing material for buildings involved wooden boards and shingles [
1] in many parts of the world. On the basis of archeological findings, it can be proven that, in Hallstatt, Upper Austria, already in the Bronze Age (13/12th century before Christ (BC)), wood shingles with a length of 20 to 30 cm and a width of 10 to 15 cm were used [
2]. The tradition of wooden roof claddings has never completely stopped and, in recent years, along with a renaissance of ecological building materials, wooden shingles are increasingly applied again.
Shingles should be preferably made from slowly grown wood, meaning that there have to be a minimum of four growth rings per cm, because of the higher durability of this wood [
3]. The spiral grain of the wood is beneficial because rain-wetted shingles twist in the sun and the bottom side dries off more quickly. This results in a low average wood moisture content and adverse conditions for wood-decaying microorganisms [
4]. Damage in the roof construction is often the precursor for severe damage in the structure of traditional buildings [
5]; consequently, the durability of wooden shingles is a crucial factor in the preservation of building artifacts. It was shown in a study in Norway that the majority of defects in pitched wooden roofs are moisture-related [
6]. Wood rots if its equilibrium moisture content is lastingly higher than 20% because of fungal infection [
7]. Wooden roofing only maintains its function sustainably if the wooden shingles dry out regularly below this level [
8].
Building elements, such as roofing constructions, are ventilated as this is a simple and effective technical solution to remove undesirable moisture [
6]. Already shortly before Christ, the Roman architect Vitruv discussed a ventilated wall construction using the principle of gravity ventilation [
9]. Until the 19th century, ventilated roofing constructions were realized using moisture-absorptive, moisture-storing, and at the same time diffusion-open materials like wooden shingles. Moisture accruing in the ventilation layer could be absorbed, stored, transferred, and finally removed without harming the building construction [
10]. Partly, the implementation of new materials and constructions such as insulation at the rafter level and roofing underlays in buildings led to moisture problems which were nonexistent before [
11].
Due to the efficient ventilation of attics and moisture-buffering effects of hygroscopic materials in historic buildings, the adverse effects of slightly leaking roof claddings are reduced [
12]. Traditional roofs are ventilated with cold roof-spaces. The attic room functions as a climatic buffer between the outside heat and cold and the living climate in the parlor areas [
12]. Moisture diffusing and streaming (through leakages) from the conditioned spaces into unvented attics in cold climates can cause harmful condensation under cold roof surfaces [
13]. Sufficient ventilation of the attic space or thermal insulation of the roof surface can help to prevent the problem, although this depends on the moisture conditions of the introduced air. Insulating roofs at rafter level in these constructions can result in lower temperatures of the roofing and, worse, drying-out [
14].
In cold climate regions, roof ventilation can prevent the formation of ice dams due to heat energy which is transported from the conditioned parts of a building to the lower side of the roof via both convection and conduction [
15]. This warm air melts the snow on the roof and the melting water freezes at the colder eave of the roof, resulting in ice dams. Ventilated roofs are also applied in hot climates to avoid overheating of the living space, although its effect is minimal in this respect [
16]. Moreover, ventilated roof constructions can help to reduce the damage potential of moisture accruing in insulation layers underneath the ventilation layer in cold climates [
17].
On the one hand, condensation water can occur inside construction components; on the other hand, it can be formed on the surfaces of construction components when their surface temperature is lower than the dew-point temperature of the surrounding air [
18]. Roof surface temperatures can fall below the ambient air temperature due to radiative effects. This leads to condensation of air moisture on cold surfaces. Water and vapour are absorbed by wood, which causes swelling and shrinking when the moisture dries off.
Surface temperatures inside ventilated roofs were shown to be below ambient temperatures for approximately half of the time during spring and autumn in Trondheim, Norway [
19]. During the warm season, the moisture input into a construction from the outside air can be significantly larger than that from the inside. Especially problematic is when the air in the ventilation system on the southern roof side is warm and wet and is transferred to the northern roof side, which is cold during spring and autumn. Under these circumstances, intense ventilation was shown to be disadvantageous due to condensation and increasing the moisture content of wooden construction elements [
20]. It was shown that, in cold attics, ventilation adds moisture when its relative humidity is higher than 70% [
21]. In north-facing cold attic spaces under the eaves, infiltration of moisture from conditioned spaces, as well as ventilation, can lead to increased moisture levels in the construction; hence, existing construction rules have to be evaluated [
22]. Moisture is only removed from the inside air or building component by ventilation air when the absolute moisture content of the introduced air is lower than that of the inside air [
23].
In this respect, it was shown that the risk of mold growth can be higher in ventilated attics when the climate gets milder and wet due to climate change. Under these circumstances, mechanically ventilated attics are recommended [
24]. In ventilated walls, the introduced air can also wet the construction during moist weather conditions [
25].
It was shown that transient hygrothermal models are suitable to predict the temperature and moisture conditions in cold roofs [
26]. The authors stated that the definition of reliable in- and outdoor climate boundary conditions are especially crucial when creating hygrothermal models, which is also the most important reason for a model’s potential deviation from real values.
The reason for this investigation is the assumption that the durability of wooden shingles on ventilated roof (cold roofs) constructions could be shorter than that on constructions with a cold attic space [
27]. It is assumed that deficient flow in the ventilation gap and condensation of humid air might be the reason. The research question for this investigation is whether it is recommended to apply wooden shingles on a ventilated roof construction or if their application should be limited to buildings with uninhabited cold attics without ventilation of the roof cladding. The effect of cardinal orientation is also evaluated in this respect. Moreover, it is discussed whether the partial closing of the ventilation gaps results in a lower wood moisture content. This is a relevant question, because historic buildings, which originally had cold attics, are increasingly equipped with roof ventilation in the course of roof refurbishment.
The research question is addressed using the example of a historic building, which originally had no ventilation layer under its wooden shingle roof and which was refurbished applying a ventilation layer under a new wooden shingle roof cladding. Air temperature, humidity, and air speed in- and outside the ventilation layer were measured throughout a year. A hygrothermal model of the construction was set up and the measured data were used to validate the model. Finally, the model was used to simulate the effects of varying cardinal orientation of the roof, varying airflow in the ventilation layer, and partial closing of the ventilation layer on the dry-out of the shingles. The results were compared with the performance of the roof without ventilation layer and a cold attic.
2. Materials and Methods
The building analysed is located in Weinbach, Salzburg, Austria. Weinbach is situated between Strobl and Bad Ischl at the bottom of a west–east-oriented u-shaped valley at a sea level of approximately 520 m above sea level. The house was built around 1630 and was used as a mill. The building consists of pure stone masonry with a thickness of 65 and 50 cm at both levels. The roof is a double-pitch roof with a slope of approximately 38° (ridge direction north-south) and a small one-sided hip. There is a loggia under the roof on the south façade. The building was bought by a private citizen who plans to use it as a permanent residential building. In a first work phase, the old and damaged roof was refurbished, but renovated using larch wood (
Larix decidua Mill.) shingles. The only modification was the implementation of a ventilated roof construction with a ventilation gap on the eave and ridge (eave–ridge distance 470 cm). The whole building was neither inhabited nor heated and the roof was not insulated in between rafters during the time of measurement (
Figure 1).
Various sensors were positioned in the construction on the western roof side according to
Figure 2 and a multi-input data logger was used to store the sensor data. Sensor 1 (bidirectional digital thermoanemometer; air speed 0.08–2 m/s, resolution 0.001 m/s; air temperature −20 to 70 °C, resolution 0.1 °C) was positioned in the centre of a ventilation gap between two counter battens (width 80 cm) in the midst of the building. It was oriented to detect air movement in the ventilation direction. Sensor 2 (another identical thermoanemometer) was positioned at the border of the ventilation gap, next to the counter batten. Sensor 3 (digital sensor for air moisture and temperature; air moisture 5–98% r.m., precision ±2.0% r.m.; air temperature −20 to 80 °C, precision ±0.1 °C) was positioned in the centre of the ventilation field next to sensor 1. Identical sensors were used at positions 5 and 6. Sensor 4 (temperature sensor Pt 100; temperature −10 to 90 °C, resolution 0.01 °C) was applied on the outside wall to control the wall surface temperature. An identical temperature sensor (Sensor 7) was applied on the underside of the shingles at the same position as sensor 1 to control the surface temperature of the shingles. All measurements were stored every 5 min on an SD-card via the data logger. Measurements were recorded for 365 days, from 24 November 2017 until 24 November 2018, resulting in 35,305 measurements. Sensor 5 was installed on 2 February 2018, resulting in 28,359 measurements.
In order to evaluate the effectiveness of the eave–ridge ventilation, the air inlet on the eave was partially closed by a wooden board (as indicated in
Figure 2): period 1 (P1) 24 November until 7 December 2017—ventilation layer open at both eaves, period 2 (P2) 7 December until 20 December 2017—ventilation layer closed at the western eave, period 3 (P3) 20 December until 25 January—ventilation open at both eaves, period 4 (P4) 25 January until 1 April—both opposite eaves closed, period 5 (P5) 1 April until 24 November—eaves open.
The measurement variables detected were ambient air temperature (AAT), ambient air moisture (AAM), air temperature in the centre of the ventilation layer (VAT), air moisture in the centre of the ventilation layer (VAM), air temperature and air moisture in the attic (AtAT, AtAM), surface temperature of the outside wall (WST), air speed in the ventilation layer in the centre and at the border (VASc and VASb), dew-point temperature of the air in the ventilation layer (VDT), and shingle surface temperature (SST). The partial water vapour pressure of the ambient air (AVP), ventilation air (VVP), and air in the attic (AtVP) was determined using physical relationships.
The resulting measurements were pairwise correlated using Pearson coefficients of correlation. Specific timelines were analysed using linear regression analysis. The graphs covering the time span of a whole year were smoothed using moving averages to the power of 288. This corresponds to an average of measurements over 24 h.
The dew-point temperature of the air in the ventilation layer was determined according to Equations (1) and (2), and the partial water vapour pressure was determined using well-known relationships. The equilibrium moisture content of wood (EMC), on the basis of the relative moisture content of the surrounding air, was estimated according to Equation (3) [
28].
The roof construction was evaluated for 365 days starting 24 November 2017 using the simulation program Delphin 5.8.1 (Bauklimatik Dresden Software GmbH) for coupled heat, air, and moisture transport in a two-dimensional consideration. A section with a length of 30 cm, including three roof battens, was considered in the model (
Figure 2). The materials larch wood for the shingles with a density of 550 kg/m
3 (absolutely dry) and spruce wood for the battens and the sheathing with a density of 425 kg/m
3 (absolutely dry), and a horizontal air layer with an inclination of 38° for the ventilation layer were considered. The physical material parameters were used as documented by Bauklimatik Dresden Software GmbH [
29] and Sontag et al. [
30].
The two shingle layers were simplified by considering two layers of wood with a thickness of 15 mm. The simplification consists of neglecting thin air gaps between shingle layers (a result of wood warping and shrinking) which would ease water input to and moisture dry-out from the lower shingle layer. The moisture ab- and desorption of the sheathing was limited by applying a high water conduction resistance value (5 × 10
15 m/s) on the surface corresponding to the roofing underlay. The temperature of the exterior air (AAT), its relative humidity (AAM), the attic air temperature (AtAT), and its humidity (AtAM) were imposed on the simulation model as boundary conditions using the measured values. A roof pitch of 38° and western orientation was considered. Hourly values of precipitation, global radiation, and wind velocity were integrated in the model using meteorological data from St. Wolfgang/Austria (measuring point 9 km from the building site) [
31]. In the measuring period, precipitation of 1160 L/m
2 and 1956 h of sunshine were recorded.
The air stream in the ventilation layer was integrated as a laminar flow. A linear relationship between a pressure gradient between the ventilation layer openings and the air flow was assumed. Pressure differences of 5 Pa (0.12 m/s), 3 Pa (0.06 m/s), and 10 Pa (0.25 m/s) between the air in- and outlet of the modeled domain were considered. Longwave radiation across the cavity between the alternate surfaces was considered using an emissivity of 0.9 for both surfaces (shingles and sheathing).
The model domain was discretized using variable discretization (smaller elements at material boundaries) with a minimum element width of 1 mm, which resulted in 1054 elements considered in the model (
Figure 2). All results derived from the model are marked with an “m” below to avoid confusion with measured values.
The temporal course of VAT_m, VAM_m at the specified position according to
Figure 2 (equivalent to the sensor position), was modeled as an averaged value of 20 finite elements (30 × 30 mm). The model values of SST were determined at the position of the sensor, averaging eight finite elements (length between to roof battens, 75 mm). Moreover, the moisture flux (liquid water, vapour diffusion, and convection) was integrated over time at the lower shingle layer’s lower surface (Dry-out_w_m). An average of 34 finite elements, corresponding to a length of 30 cm of the shingle’s lower surface, were considered. The dry-out rate (Dry-out rate_w_m) was determined as the derivation of Dry-out_w_m with respect to time.
Finally, the total moisture mass (liquid, vapour, ice) was determined for the lower and upper shingle halves and referred to the dry mass of the wood (EMC_w_m and EMC_w_u_m). Both values were an average of 136 finite elements (15 × 300 mm) each.
First of all, the model values were determined with the air stream in the ventilation layer as measured for all four cardinal orientations of the roof surface. Then, the air speed was set to 0.06 m/s (corresponding to the value determined with closed eaves) during the course of the whole year to evaluate the characteristics of a construction with permanently closed eaves (ventilation out of operation and thermal effects on the air speed neglected). Finally, the spruce sheathing in the model was removed, and AtAT and AtAM were considered as boundary conditions at the shingles’ lower surface, which represents a shingle roof on a cold attic.
All model values were determined as hourly values, and the measurements were averaged on an hourly basis for comparison with the model. This resulted in 8760 values for each measurement.
The model was validated by comparing real and modeled VAT, SST, VAM, and VVP using a linear regression analysis between real and modeled values in the course of a year (24 November 2017 until 24 November 2018).
where
is the saturation vapour pressure for air temperature
in Pa,
is the dew-point temperature in °C,
is the relative air moisture content,
is a constant (610.5),
is a constant (21.875 for
°C and 17.269 for
°C), and
is a constant (265.5 for
°C and 237.3 for
°C.
where
is the equilibrium moisture content as a percentage,
is the relative humidity expressed in decimal form, and
is the air temperature in °C.
3. Results and Discussion
The ambient air temperature (AAT) was measured throughout the year with a minimum of −15.9 °C on 28 February 2018 and a maximum of 34.5 °C on 4 August 2018 (
Figure 3). The average temperature during the measuring period accounted for 10.6 °C (standard deviation (SD) 9.4 °C). AAT was well correlated with the air temperature in the ventilation layer (VAT) (
R = 0.99), the bottom face layer of the wooden shingles (SST) (
R = 1.00), and the air temperature in the attic (AtAT) (
R = 0.95) (
Table 1 and
Table 2).
The relative humidity of the ambient air (AAM) was characterized by a minimum of 22% on 9 April 2018 and a maximum of 100% several times during the winter of 2017/2018. The average relative air moisture content during the measuring time was 76% (SD = 17%). AAM was correlated with that of the ventilation layer (VAMc) (
R = 0.84) and that in the attic (AtAM) (
R = 0.62). Nevertheless, AAM and VAMc were not perfectly correlated as only 71% of the variation in the VAMc could be explained by AAM (shown by the coefficient of variation =
R2). On average, VAMc was 2% lower than AAM (
Figure 4). Whilst the SD of AAM was 17%, the SD of AtAM was only 13% and, in this respect, more languid.
Focusing on specific time intervals, like that in mid-April 2018 (chosen because of great moisture uptake on the shingles’ underside) (
Figure 5), the air temperature rose from the morning until the afternoon, which caused the relative humidity to drop and the water vapour pressure to rise (
Figure 4). After reaching the top temperature around 4:00 p.m., the relative humidity of the air rose, the vapour pressure dropped, and the shingle lower surface was wetted during the night. This could be observed throughout the year (the dry-out rate was negative 45% of the year). The 24 h balance of Dry-out rate_w_m was predominantly positive (i.e., drying) from the end of November 2017 until mid-April 2018 and varied the rest of the year. Whenever the slope of the cumulated dry-out curve in
Figure 6 is low, the shingles’ lower surface was partly wetted by the inflowing air. Periods with a low slope of the dry-out timeline indicate a low balance of the dry-out. The vapour pressure (AVP) was positively correlated (
R = 0.91) with the air temperature (AAT).
The surface temperature on the shingles’ bottom surface fell below the dew-point temperature of the inflowing air 6.3% of the measuring time, which was also mentioned to an even larger extent by Gullbrekken et al. [
19]. This corresponds to 180 h of potential condensation. The time when the shingles’ lower side temperature was lower than the dew-point temperature was concentrated 99% in one half of the year (1 November to 1 May). During this time, 12% of the time condensation conditions were detected. How much the dew point temperature was undercut (SST-VDT) was strongly indirectly correlated (
R = −0.91) with the VAM. In the beginning of April 2018 in the morning hours, SST fell strongest below VDT throughout the whole measuring time (
Figure 7). The shingles did not take up a lot of moisture in this time (shown by predominantly positive values of Dry-out rate_w_m), because the vapour pressure (AVP, VVP) was low during that time, meaning that the air carried a low amount of water (
Figure 3). Consequently, it was not the condensation of moisture that caused the most moisture uptake on the shingles’ lower surface, but moist inflowing air in the warm season (shown in
Figure 6 during time intervals with a low slope of the cumulated dry-out curve).
The surface temperature of the shingles on the side of the ventilation space (SST) was well correlated with the air temperature in the ventilation layer (VAT) (
R = 0.99) and was on average 0.7 °C lower than VAT. This was probably caused by long-wave radiation of the shingles to the sky [
18], heat flow from the inside to the ventilation air (AtAT was on average 0.8 °C higher than VAT), and snow, partly lying on the shingles in the beginning of 2018. Snowfall was recorded on 40 days from the start of the measurements until the end of March 2018 and was a reason for the stronger deviations of SST from VAT during the winter months (
Figure 3).
The air speed in the ventilation layer in the centre (VASc) showed a minimum value of 0 m/s and a maximum of 1.03 m/s and was well correlated (
R = 0.99) with the air speed at the border (VASb). The average air speed in the ventilation centre was 0.19 m/s. The variability was high with a SD of 0.14 m/s. During the first measuring period P1 (ventilation open), the average of the air speed accounted for 0.12 m/s; during P2 (western eave closed), the average of the air speed accounted for 0.06 m/s; during P3 (ventilation open), the average of the air speed accounted for 0.12 m/s; during P4 (both opposite eaves closed), the average of the air speed accounted for 0.06 m/s; during P5 (ventilation open), the average of the air speed accounted for 0.25 m/s (
Figure 8). The air speed at the border of the ventilation field was on average insignificantly lower (on average 0.003 m/s) than in the center. It could be shown that, by closing one eave (P2), the average air speed in the ventilation layer could be reduced by 50%. VASc was positively correlated with AAT (
R = 0.76) and AtAT (0.82) meaning that higher air temperatures resulted in a higher air flow in the ventilation layer. In the summer half-year, the average air speed in the ventilation layer was twice as high as in the winter when the eaves were open, which supports this conclusion.
Comparing P2 with the western eave open and P4 with both opposite eaves closed, the air speed was the same, but the average of AAT was 12.2 °C higher in P4 than in P2, while the wind conditions were comparable (average wind speed P2 1.2 m/s, P4 0.9 m/s; average wind direction P2 205°, P4 190°) and there was a positive correlation of AAT and VASc. This suggests that there was additional air-flow hindrance when both eaves were closed. Considering a ventilation gap between two battens (0.8 × 0.03 m2), the air flow ranged between 5.2 m3/s and 21.6 m3/s.
The quality of the hygrothermal model was assessed by comparing the values of the in situ measurements of VAT, VAM, VVP, and SST with the modelled correspondent by calculating linear regression functions between measured and modelled values of the same quantity (
Table 3). The coefficient of correlation (
R2) between VAT and VAT_model was 0.99, and VAT was on average 0.4 °C underestimated by the model.
R2 between SST and SST_model accounted for 0.99 and overestimated the real value on average by 0.1 °C (
Figure 7). The interdependence of VAM and VAM_model was characterized by an
R2 of 0.90, whereby the model overestimated VAM by 3% (
Figure 4). The coefficients of determination of the VAT and SST models are high. The fit of the VAM model was, considering the high variability of the air moisture [
26], adequate. The vapour pressure, which is a characteristic for the water in the air, was modelled, and VVP_m deviated on average 10 Pa or 0.9% from VVP (
R2 = 0.96). This suggests that the general trend in VVP was correctly traced by VVP_m.
The modelled moisture content of the shingles’ upper layer (EMC_w_u_m) was on average 34% (SD = 22%), while that of the lower layer (EMC_w_m) was on average 23% (SD = 13%). The EMC of this study was not measured directly, but derived from the model [
30]. A lower bound for the modelled data was EMC, determined according to Mitchel [
28], representing the EMC without rain influence, which was in good agreement with the modelled values whenever the level of precipitation was low during summer 2018 (
Figure 9). Literature values report an average moisture content of unsheltered weathered wood in Sweden, mounted with an angle of 45°, of 46% for pine sapwood and 25% for pine heartwood [
32]. EMC_w_u_m in this study varied between the two values. The source cited supports the modelled results of the current study, but uncertainty is present; therefore, the results for EMC should be rather interpreted as basic trends, and they were primarily used to evaluate differences in the operation mode of the ventilation in this study.
The MC of the upper shingle layer was predominantly affected by precipitation, causing the peaks in
Figure 9. EMC_w_m was higher than EMC with an average of 16% (SD = 4%) (the moisture content of the shingles if there was no precipitation). Hence, the lower shingle layer was also significantly influenced by precipitation throughout the year, being stronger at the beginning (the peaks of precipitation are delayed in the EMC of the shingles in
Figure 9).
The EMC of the lower shingle layer was on average around 37% (SD = 14%) from the end of November 2017 until mid-April 2018 and then dropped to an average of 14% (SD = 2%) for the rest of the year. The risk for decay is high if the EMC is lastingly higher than 25% and the temperature stays above 5 °C [
33]. From the end of November until mid-April, the model showed an EMC of more than 25% for both shingle layers, and the temperature was above 5 °C 20% of the time. For the rest of the year, the upper shingle layer’s EMC bounced between 10% and 70%. The lower shingles’ EMC varied between 10% and 20%. The analysis shows that, during the warm season, the upper shingles’ EMC was repeatedly in a rot danger region. Consequently, strategies to lower the EMC (by improved dry-out) are advantageous, even if the improvement is low (
Figure 9). According to the model applied, the lower shingles were not at risk of decay from midst of April until end of November. This temporal course of wood moisture is in good agreement with findings of Isaksson and Thelandersson [
33], albeit with lower precipitation; hence, a lower average moisture level was measured in this study.
The lower shingle layer took up moisture from the streaming air in the ventilation layer 45% of the time (
Figure 6). Whilst the mechanism of wetting and drying the lower shingle surface varied during the day (
Figure 7), there were times, especially during the warm season, where the shingles were more severely wetted by the inflowing air. Focusing on the balance of moisture take-up and dry-out in
Figure 6 throughout a year, more moisture was removed by ventilation than carried in. This is a strong argument for the ventilation of shingle layers and contradicts the findings of Künzel [
20] stating that ventilation is not desirable a significant part of the year. If the eaves were permanently closed and the VASc was 0.06 m/s (thermal effects on the air speed neglected), the average MC of the lower shingle layer would be 24% (SD = 15%), 1% higher than with the open ventilation layer (
Figure 9). EMC_w_u_m was not significantly affected by closing the ventilation gaps (
Table 3).
The roof construction was also evaluated without roof ventilation applying the attic climate (AtAT, AtAM) as a boundary condition below the shingles. The EMC of the lower shingle layer would be on average 26% (S = 18%), 3% higher than with the vented one and 2% higher than that with reduced ventilation. The moisture dry-out would be 17 kg/m² throughout the measuring period, 6 kg/m² less than with ventilation layer. The disadvantageous effects of reduced ventilation or an unvented construction were more pronounced during the winter months.
Considering that ventilation of the shingle roofing is desirable when the lower shingle surface does not take up moisture from the ventilation air and that the air speed in the ventilation layer can be influenced by coverage on the eaves, technical solutions for steered ventilation are worthy of consideration [
21]. This would require flaps at the eaves which are steered depending on the evaluation of air moisture, shingle temperature, amount of solar irradiation, and general weather conditions (e.g., snow on the roof). An estimation for the effects of this approach was conducted by closing the eaves in the model whenever it showed a negative moving average of 6 h dry-out rate (i.e., the air speed was set to 0.06 or 0.25 m/s, and the thermal effects were neglected). On average, the EMC of the lower shingle layer (EMC_w_opt_m) was 0.3% lower compared with EMC_w_m. In the current situation, this effect is minimal because it is superimposed by the effects of wetting due to rain. Nevertheless, this could be an interesting optimization of ventilated constructions which are not subjected to direct rain, such as ventilated facades. In this context, bio-actuators to steer the ventilation gaps, as proposed by Rüggeberg and Burgert [
34] or Holstov et al. [
35], could find a meaningful future application.
If the attic is inhabited and heated, moisture diffusion and convection might interfere with the mechanisms studied in this project. The construction would be equipped with a vapour retarder under the insulation, but the moisture flow through leakages may be significant [
36]. Presumably, the moisture transport from the inside to the outside would be minimal because of vapour barriers applied on the inner side of the roof construction. The heat flow from the inside might slightly raise surface temperatures in the ventilation layer, which would diminish the condensation problems. This effect may also be minimal, because constructions tend to be very well insulated. Nevertheless, these multifactorial processes should be studied in further research.
In the current study, a roof of western orientation was studied. The unmodified roof construction was evaluated for the other cardinal directions as well, changing the boundary conditions in the software. In
Figure 9 and
Table 3, one can see that the modelled EMC of the lower shingle layer was highest on a north-facing roof with an average of 26% (SD = 15%) and lowest on a south-facing roof with an average of 20% (SD = 10%). The differences were most significant during the cold time of the year (end of November until mid-April). This findings are in good agreement with a study focusing on the fungal decay of wood in different microclimates showing that all studied wood species have a higher risk of decay in shaded areas [
37]. Focusing on the dry-out rate, it was highest with a north-facing orientation (26 kg/m²) and lowest with a south-facing orientation (20 kg/m²). As both roof orientations were flown through with the same air in the model, it follows that the south-facing roof’s lower shingle layer was dried up to the top more efficiently, because there was a higher drying potential of the sun. Evaluating the surface temperature on the shingles’ exterior surface, the average temperature accounted for 13.3 °C (SD = 11.9) east, 14.1 °C (SD = 12.5) south, 12.6 °C (SD = 12.0) west, and 11.6 °C (SD = 10.8) north. Hence, it can be concluded that efficient ventilation is more important on roofs with less sun exposition. In
Figure 6, one can see that the dry-out of the shingles’ lower surface increased from the south, followed by east, west, and north, and this was indirectly proportional to the radiation of sunlight, confirming this finding. This was also seen when comparing the average moisture content of a ventilated roof and one with closed eaves (
Table 3). Whilst the average EMC was unchanged for the south-facing roof, the EMC of a roof with reduced ventilation on the northern side was on average 1% higher. The modelled effects of cardinal orientation on the wood moisture of shingles need to be verified in further in situ measurements in subsequent investigations. Furthermore, it will be necessary to evaluate other effects such as cracks as a result of wood shrinkage on the shingle surface, which could cause significant local changes of moisture conditions after several years of exposure [
38], and such as ascending forces when air is heated up in sun-exposed ventilation layers.