There was a change in colouration of the biomass, from green to brown, for both heaps during the course of the experiment. Also, there was extensive growth of Agrocybe rivulosa (wrinkled field cap) on the Rothamsted heap but not on the East Midlands heap.
During the course of the experiment, a total of 334 and 164 mm of rainfall were recorded in the East Midlands and Rothamsted sites, respectively. Ambient temperature records and rainfall are shown in Figs. 2 and 3 along with the average (taken over the netted bag samples) internal temperature of the piles. Mean ambient temperatures were 18 and 16 °C, respectively.
Nine temperature recorders were retrieved from the East Midlands site. The records showed a rapid increase in temperature from 13 °C to a maximum of 66 °C after 12 days. Across Log Tags®, temperatures were recorded to be above 60 °C between day 3 and day 30. At day 27, the average temperature of the heap began to decline (Fig. 2). After day 56, there was a more rapid drop, after which heap temperature fluctuated between 20 and 35 °C.
All 20 recorders were retrieved from the Rothamsted pile. The maximum recorded temperature within the heap was 64 °C on day 6. Readings from the Log Tags® showed a consistent rapid increase in temperature from 24 °C to just over 60 °C over a period of 5 days (Fig. 3). A temperature of 60 °C was maintained for a period of 19–29 days, after which the temperature declined. Between day 31 and the end of the experiment, the temperature ranged between 30 and 40 °C. Comparing the two heaps, the Rothamsted one heated up more rapidly, reaching peak average temperature (61 °C) after 6 days of establishment compared to 27 days for the East Midlands heap (60 °C). Overall, the Rothamsted heap had 32 days over 40 °C compared to 46 days for the East Midlands heap. Temperature patterns fluctuated between 20 and 40 °C after day 65 at East Midlands and after day 45 at Rothamsted. It therefore appears that the temperature increase occurred faster at Rothamsted, where ambient temperature was less variable, and where there was a long period of dry weather for 12 days following 5 mm of rain on day 4.
Heap Breakdown Observations
After bisecting the heaps, various layers were identified (Table 1). At the East Midlands site, four layers were identified: the outmost layer was approximately 10 cm deep and much drier on the southern (S)-facing side. Below this on the S-facing side there was a distinct white mould layer which ranged between 15 and 30 cm deep, under which the drier core region was found. On the northern (N) side, the layers were more heterogeneous with varying depths of mould, though sometimes it was absent, being replaced with a darker wet layer absent on the S-facing side. The central regions of the heap were generally dry. The Rothamsted heap was similar, except there was no darker layer present. The wood chips forming the apex of both heaps were extremely wet.
As the East Midlands heap had been positioned on grass, it was necessary to leave a layer of chip on the soil to eliminate contamination. Taking 21 samples along a transect bisecting the remaining bed found that this was on average 15 mm deep (95 % confidence interval (CI) 14–19), but ranged between 5 and 30 mm. Four samples taken from the bed averaged 63 kg fresh material (95 % CI 60–66) per m2, with a moisture content of 65 %, (95 % CI 63–66) resulting in a dry matter loss of 22 kg/m2, or approximately 6 tonnes for the whole heap. Measuring the additional loss from the use of wood chips to drive over the ground during heap construction was difficult, as compression from the vehicles meant that lower layers of the chips were fully embedded into the ground. However, the driving bed had an estimated footprint of 86 m2. Four random quadrat samples taken from the area weighed 22 kg/m2 (95 % CI 20–25) at 69 % moisture content (95 % CI 65–72) suggesting a loss of up to 1 t dry matter for this area in addition to losses under the heap. Analysis of this material showed the ash content to be 3.7 times higher than that of the original wood chip, which is most likely due to soil contamination. At the Rothamsted site, losses to the ground and surrounding area were negligible.
Dry Matter Losses and Compositional Changes
At the East Midlands site, samples of the initial fresh chip had average moisture content 54 %, 95 % CI 52–54 %. Samples of the mixed heap showed that biomass had dried to 39 % (95 % CI 30–48 %) after 6 months (Table 1). Unfortunately, only 13 of the 20 bagged samples were found in the East Midland pile. Of these, two had been damaged and opened, therefore could not be used for dry matter (DM) loss assessment. The mean moisture content of the net bag samples from the core region of the heap was 31 % (95 % CI 21–42 %), although this was skewed somewhat by the two particularly wet and mouldy bags (62 and 78 % moisture content); without these, the average was 23 %, which was the same as the core. This indicates a successful rate of drying within the heap; however, after mixing the heap with the wetter outside layer, the average moisture content increased. The average dry matter loss of the netted bags was 18 % (95 % CI 13–23 %), with the highest loss (46 %) occurring in the 62 % moisture content bag. Without the two particularly wet bags, the average dry matter loss was 14 %.
At the Rothamsted site, 84,060 kg of freshly cut biomass was stored (Table 2). Samples showed the chips had an initial moisture content of 50 % (95 % CI 47–53 %) and had dried to 43 % after 4 months (95 % CI 32–54 %). Only 1 of the 20 bags was lost through damage. The average moisture content of the remaining net bags was 29 % (95 % CI 27–31 %), which is slightly drier than the sample for the core. Out of the 19 bags examined, 9 dried down to between 22 and 25 % moisture content, and the overall range was 22 to 34 %. The average dry matter loss of the netted bags was 19 % (95 % CI 17–20 %). The measured mass of the wood chip heap at the end of the experiment was 58,030 kg, corresponding to an estimated dry matter loss of 9062 kg or 21 % of the dry matter of the stored biomass.
Table 2 Summary of dry matter losses in the Rothamsted heap
There was high variability in the changes in nitrogen and ash composition between the bags at the East Midlands site, with no statistical difference (p > 0.05, t test) between before and after storage (Table 1). At the Rothamsted site, the original wood chip had a significantly lower N content than the East Midlands heap (t = −4.34, d.f = 4, SED = 0.00054, p < 0.001). At the Rothamsted site, there was a significant increase in the percentage N content between the bagged samples and original chip (t = −1.99, d.f = 20, SED = 0.0017, p < 0.05), but a zero change in relative C, resulting in an decrease in the C/N ratio after storage. Compared to the bagged samples found within the heap, there were significant (p < 0.05, t tests) increases in C and N proportions in the outer layers, particularly the mouldy zone. There were no clear differences in ash contents of the Rothamsted wood chips before and after storage.
Using the information on moisture content and composition, the Milne equation and data in the Phyllis Database were used to predict the lower heating value (LHV) of the wood chips [22], using the average figure for willow (untreated wood, willow). The LHV was estimated at 7.2 and 9.9 GJ/t before and after storage at the East Midlands pile. When accounting for the dry matter losses, there was an average net energy loss of 1.1 GJ/t stored, as estimated from all the net bags. The highest losses (2.1 and 3.5 GJ/t stored) were recorded in the wettest bags (78 and 62 % moisture content bags, respectively). At the Rothamsted pile, the LHV of the mixed heap was estimated at 7.8 and 9.1 GJ/t before and after storage. Factoring in dry matter losses leaves a net energy loss of 129 GJ for the whole heap, or 1.5 GJ per t stored. The estimated energy losses from the average of all of net bag samples within the heap were small (0.1 GJ/tonne stored). This was due to the acceptable level of drying in the bags as they were situated in the core. After the heap was moved, re-tipped and mixed however, the outer layers and chimney zone meant that the average moisture content of a random mixed heap samples was 10–16 % higher than in the core and hence a net energy loss was calculated.
GHG Concentrations in the Wood Chip Heap
East Midlands Heap
There was a rapid increase in CO2 concentrations in the first 30 days of the experiment, with the peak (35,000 ppm) occurring on day 27 on the darker, north side of the heap (Fig. 4a). On a number of occasions, the CO2 levels observed were off scale (FID attenuation settings selected were a compromise in order to detect peaks across a broad range of both CH4 and CO2 concentrations), with the truncated CO2 peaks thus providing an under-estimate of the actual concentration. After 60 days of sampling, the concentration levelled out at around 1500 ppm and remained roughly constant until sampling ceased. After the peak in CO2, a steady increase in CH4 concentrations was recorded (Fig. 4b), again on the darker side, with the maximum average concentration (275 ppm) occurring on day 48. The highest single probe measurement for methane was 1633 ppm, on day 55. By day 69, CH4 concentration had declined to an average of 13 ppm and remained roughly constant until the end of the experiment. Nitrous oxide concentrations were highest early in the experiment, with the greatest variation occurring at days 6 and 8. The peak average N2O concentration was 0.56 ppm, occurring on the south-east or ‘sunny’ side. There was a downward trend in the N2O concentrations from the probes at 3 m after the first sampling (Fig. 4c). Correlation of the average 3-m probe GHG concentrations against the average temperature of the heap showed a significant positive relationship for CO2 (R
2 = 0.6, n = 18, p < 0.001) and N2O (R
2 = 0.4, n = 18, p < 0.005) with temperature. There was no significant correlation between CH4 concentration and heap temperature (p = 0.800).
The linear mixed model fitted for log(CH4) and log(N2O) was:
$$ y= vHeight+\left( AirvsHeap/\left( Depth* Side\right)\right)* vDay+Spl\left( vDay+ vDay. Depth\right)+\left( Probe/ Day\right), $$
where y represents log(CH4) or log(N2O), the slash (/) indicates a nesting of model terms, a star (*) indicates the main effects and interactions between terms, and Spl(vDay + vDay.Depth) indicates the variance component of the curvature with respect to days modified with respect to depth. Here, vHeight and vDay are variables, and all the other terms are factors: AirvsHeap accounting for the control samples, Depth and Side accounting for these sample zone effects nested within the heap, and Probe/Day extracting variance due to the time points nested within probes. The model for log(CO2) was the same but with Spl(vDay + vDay.Depth) being replaced by Spl(vDay + vDay.Side), as curvature was different with respect to the two sides rather than between the two depths of the probes (Supplementary data).
Given the repeated measures from probes, concentrations of all three GHGs showed correlation over time that was heterogeneous, i.e. significantly different (p < 0.05, χ
2 tests), over the time points (Supplementary data). Following this, the F-tests for the fixed effects indicated a significant interaction (F = 5.44 on 1 and 29 df, p = 0.027) between AirvsHeap, Depth, Side and vDay, for CO2 (Fig. 5a), and between AirvsHeap, Depth and vDay for CH4 (F = 20.15 on 1 and 55 df, p < 0.001) (Fig. 5c) and N2O (F = 14.86 on 1 and 44 df, p < 0.001) (Fig. 5e). There was therefore an effect of side for CO2 that was not seen in the other gases.
Figure 5 shows the trends for each GHG that are recognised by the spline term along with the significant (p < 0.05, F-test) main effect (or interaction) terms for depth and/or side. For all gases, the concentrations were noticeably higher from the deeper probes (Fig. 5b, d, f). For CO2, there was an opposite effect of depth and side: where the highest concentrations were from the 3-m probes of the sunny side of the pile but in the 1-m probes of the dark side. Hence, there was evidence of a different trend over time for the five sample zones (air, Dark 1 and 3 m, Sunny 1 and 3 m) albeit with the shape of the trend (in the spline term) being modified with respect to side. There was also an overall negative relationship of CO2 with height (F = 6.19 on 1 and 18 df; p = 0.017; coefficient −0.0083, SE 0.0027). This effect was not observed in the CH4 or N2O results.
Rothamsted Heap
The statistical analysis did not directly compare the two heaps because there was no replication of the heaps at the sites; these also being confounded with method of construction (on concrete or soil). A general inspection of the results shows that the CO2 concentrations in the Rothamsted heap were far higher in the first few days than those detected in the East Midlands heap; however, CO2 concentration fell more rapidly, following a peak at day 4, to a similar level as in the East Midlands heap, within a period of 34 days (Fig. 6a). The concentrations then dropped to a lower level (2500 ppm) that was near constant until the end of the experiment. Correlation of the average 3-m probe GHG concentrations with the average temperature of the heap gave a significant positive relationship (R
2 = 0.26, n = 18, p < 0.05) for CO2. There were no such correlations for N2O or CH4 (p = 0.180 and 0.870, respectively); however, over the first 2 weeks only, across all probes, there was a significant negative relationship between N2O concentration and the heap temperature (R
2 = 0.14, n = 60, p < 0.005). For CH4, the greatest variance occurred at days 20, 28 and 34, when there was an obvious, yet brief peak of CH4 detected for the 3-m probes on day 20 (Fig. 6b). After the peak, the CH4 concentrations did not stabilise in the same way as the CO2 concentrations did, but continued to fluctuate. As for CO2, the peak in CH4 concentration was earlier than seen in the East Midlands heap. Similar to the CO2, there was a very early peak in N2O concentrations in the Rothamsted heap (Fig. 6c), with the greatest variance at day 4. The peak was higher than that observed in the East Midlands heap (0.95 vs. 0.55 ppm).
The linear mixed model fitted for log(CO2) was:
$$ y= vHeight+\left( AirvsHeap/\left( Depth* Side\right)\right)* vDay+Spl\left( vDay+ vDay. Depth\right)+\left( Probe/ Day\right), $$
with terms as described previously; the model for N2O had Spl(vDay + vDay.Depth + vDay.Side) as the spline term, and the model for CH4 only had Spl(vDay), in this case there being no difference in the curvature over time with respect to depth or side (Supplementary data). In the CO2 concentrations, there was a significant interaction between AirvsHeap, Depth and vDay (F = 26.55 on 1 and 60 df, p < 0.001), showing an effect of depth and time (Fig. 7a); the AirvsHeap by vDay interaction was also significant (F = 22.81 on 1 and 62 df, p < 0.001) but the AirvsHeap by Depth interaction was not (F = 1.94 on 1 and 19 df, p = 0.180), suggesting that the effect of time was stronger than that of depth. Figure 7b shows the trend recognised by the spline term along with the AirvsHeap by Depth by vDay interaction in Fig. 7a.
The peak in CH4 was not as well-defined as in the East Midlands heap; however, there was a significant interaction between AirvsHeap, Depth and vDay (F = 8.23 on 1 and 94 df, p = 0.005) (Fig. 7c); again, the AirvsHeap by vDay interaction (F = 6.32 on 1 and 94 df, p = 0.014) was significant but the AirvsHeap by Depth interaction was not (F = 2.14 on 1 and 17 df, p = 0.161). Greater concentrations of N2O were detected from the deeper probes, with a significant interaction between AirvsHeap, Depth, Side and vDay (F = 10.72 on 1 and 46 df, p = 0.002) (Fig. 7e) indicating evidence of a different trend over time for the five sample zones, and with the shape of trend being modified with respect to both depth and side. Figure 7f shows the effect of depth and side given the spline terms, with the dark side having greater levels of N2O than the sunny side. In both instances, the deeper probes detected higher levels of the gas, and there was an overall marginally significant positive relationship of N2O with height (F = 4.59 on 1 and 25 df; p = 0.042; coefficient 0.070, SE 0.040). No effect of height was observed for CO2 or CH4.