1. Introduction
Composting is well known as a complex aerobic process governed by microorganisms with its inherent temperature dynamics divided into three main phases: psychrophilic, mesophilic and thermophilic. The environment with the highest temperatures is created in the thermophilic phase that occurs immediately after initial heat-up provided that suitable compost mixture [
1], its physical and chemical parameters, composting principles [
2] as well as proper composting facility construction [
3] and management [
4] were respected. Compost Heat Recovery Systems (CHRSs) [
5] are being reviewed [
6], investigated and modeled [
7] as well as developed in order to utilize the heat produced by bacterial metabolism. This biologically produced heat can be considered as low-temperature heat source [
8] with the potential of becoming another method for sustainable energy [
9] production from biomass [
10] and a novel waste management strategy [
11]. This heat would be otherwise treated as waste heat and dissipated into the environment without productive use. Applications of this heat source are in green and hoop houses, preparation of hot water [
12] and heating of buildings [
13].
At the pilot-scale or practical level, experiments with the Jean Pain-style composting systems [
12] are being conducted and modified (under names such as Biomeiler [
14], thermocompost, bioreactor or composting reactor). However, the evidence and measured data of their life cycle, performance and final compost quality are scarce in scientific literature. For the purpose of filling this gap, experiments have been performed [
15,
16,
17,
18] with medium-sized compost piles (volume 15–20 m
) where the whole process was observed, physical/chemical parameters were measured and potential of this renewable heat source and biomass utilization strategy was estimated.
In this research, we focus on heat capture and its transport mechanisms within the passively aerated static pile with the aim of maximum heat recovery without adversely affecting the composting process. The heat exchange system, especially the type of the heat exchanger, determines the way the heat is recovered. Careful design needs to be applied in order to tap into the most abundant heat source which naturally occurs during composting, i.e., the water vapour [
5].
Heat exchangers used in Jean Pain style bioreactors are usually formed from plastic pipes that are gradually laid in layers and in a certain pattern as the compost mound is built [
19]. This approach allows heat removal from the whole volume of the pile by conduction as a prevailing heat transport mechanism. Limitations of this system are the susceptibility to leakage and potential damage by heavy weight or manipulation [
12]. Moreover, the system of installation/dismantling of the heat exchanger is dependent on the pile construction/deconstruction and it can be labour intensive and impractical on larger scales (when machinery is used). Importantly, excess heat removal from internal parts of the pile can affect heat generation [
19] and potentially the microbial activity itself [
20].
The goals of this study are therefore the introduction of a new type of heat exchanger based on condensation of water vapour, providing evidence, operational data and analysis of the performance of the heat exchanger prototype under real conditions (in a medium-sized compost pile) as well as sharing and discussing observations and drawing conclusions for the further development of compost heat recovery technique.
Impact of Heat Removal on Its Source
Since temperature determines which bacteria (from thermophilic, mesophilic or psychrophilic families) predominates in aerobic degradation processes, direct heat removal from internal parts of the compost mound via heat exchanger can therefore affect their activity. Potentially, too much heat removed from the mound can harness the whole composting process as some bacteria become inactive or dormant.
Experiments with continuous temperature measurements inside the compost mound provided an observation of the impact of heat removal on heat sources, [
17].
Figure 1 shows temperature profiles inside the mound (left) and the position of measuring poles with sensors and schematic drawing of spiral heat exchanger (right) buried inside the compost mound. Inlet and outlet from the hydronic heat exchanger and ambient temperature sensors are depicted as well as direction of water circulation.
The graph in
Figure 1 recorded three time lapses when the circulation pump was on and heat had been actively removed from the mound. Power output for each 15, 30 and 45-min run was estimated as
and 1379 W, respectively. Even if the heat recovery system was on only for a short period of time, a slight drop in the internal temperature field is noticeable. Moreover, previous steady state (balance between heat production and losses) had not been fully recovered in this experiment and the internal temperatures continued to decrease.
Note that the standalone cylidrical pile, 3 m in diameter, 2 m high, without any insulation, has significant heat losses due to its high surface area/volume ratio
m
/m
. Larger piles seem to be less prone to adverse effects of heat removal, although cold inlet water is circulated in the heat exchanger [
12,
19].
3. Results
The bioreactor with proposed condenser-type heat exhanger was built during November 2018 (South Moravian region—Czech Republic) with already cold or freezing temperatures over night. In spite of these weather conditions, the initial heat-up phase with exponential temperature growth finished by the end of day 4. Once the temperature started to rise, the natural convection began to push the moist air through the aeration system. Although the biofilter was used, the moisture was transported into the hoop house, condensed and created icicles. For this reason, we closed the outflow orifice (see
Figure 7) to keep the moisture inside the pile and let the aeration be driven only by diffusion.
The temperature dynamics during days 4 and 45 are depicted in
Figure 15.
For the sake of lucidity, all data in
Figure 15 are averaged over each hour. Measurement of the core temp. started by the end of day 3, the ambient temp. was launched later during day 7 (Bus A), whereas the rest of the sensors (Bus B) associated with the heating circuit and hoop house started during day 9 when the core temperature stabilized around
. The dark red line shows the temp. of the heating circuit, which is calculated as an average of Compost—In and Out temp. readings.
Three modes of circulation in the heating circuit were chosen: firstly, the circulation pump was on for 30 min in each hour, which resulted in fluctuating behaviour of readings from sensors Compost—In/Out. Detailed readings over days 9–10 are depicted in
Figure 16.
The graph in
Figure 16 also shows the initial/transient phase when the average temperature of the heat-carrying fluid is continuously rising with each cycle as the whole heating system becomes warmer. The green line (Ambient-Top) appears in the following figures as the indication of heat losses to the surroundings from the upper surface of the pile. The average temperature difference of around
between sensors Ambient and Ambient-top still indicates considerable heat loss, even if the biofilter cover layer is applied.
The most stabilized performance of the bioreactor over a 5-day period is shown in
Figure 17.
For each half-day (0–12 h and 12–24 h), temperature differences were calculated and shown in the box plot in
Figure 18.
Average volumetric flow rate measured using water meter for this period reads
l/min. The power output then follows from:
where
[kg/s] is the mass flow rate,
[J/kgK] the specific heat capacity of water at constant pressure and
[K] the temperature difference.
Bar plot in
Figure 19 shows the thermal power output and the cumulative heat recovery [kWh] of the bioreactor over the selected 5-day period:
During day 19, a sudden drop in the heating circuit appeared and the temperature stayed between 20 and
for several days, even though the core temp. was above
(see
Figure 15).
In the second mode, the circulation pump was on for three hours, 2-times within the first 12 h in a day and the rest still as in the previous mode, i.e., the overall running time of the pump remains 12 h per day (see days 27–33 in
Figure 15). However, the cooling period was found to be too long and, since day 34, the pump had run continuously (3rd mode) in order to stay above the freezing point. The temperature difference between Compost—In and Out stayed around
, which limited the heat recovery.
4. Discussion
The design ideas for a condenser-type heat exchanger for utilization of compost heat have been presented, cf.
Figure 2. A prototype was built from LDPE pipe (see
Figure 4) and installed as a key part of CHRS for the pilot-scale passively aerated standalone composting pile (modified Jean Pain mound). Its properties have been studied in a practical composting experiment over the winter period and its thermal performance has been evaluated.
This heat exchanger should overcome potential effects on microbial activity and heat production due to its position on the top of the pile in a “heat exchange area” as shown in
Figure 8. Direct contact with actively composting biomass is avoided as the pipes lay on a platform that forms a cavity for hot gas accumulation (see
Figure 3). As the moist air condenses on the heat-exchange surface, the heat is then transferred via conduction through the wall of the pipe to heat-carrying medium. Therefore, the exchanger utilizes the majority of ”waste” heat available in the latent form.
However, if the heat exchanger surface is covered with other layers (woodchips, biochar and matured compost) for thermal insulation from the top, approximately 50% of the surface is therefore excluded from direct condensation. Better design of the holding platform with more spacious cavity should be adopted for maximal thermal performance of the heat exchanger itself.
Condensed water solutions are re-used directly inside the pile (thus local water cycle is achieved)—less moisture is diverted from the pile, thus keeping moisture content at a similar level. This is true if the outflow orifice of the aeration system is closed (see
Figure 7). The spiral shape of the heat exchanger with horizontal gaps between each pipe allows gases to penetrate through this layer. Therefore, the natural convection should not be affected by the presence of the spiral.
From a practical point of view, the installation and dismantling of the heat exchanger is not dependent on the construction of the pile itself, thus allowing the extension of this technology for larger scales composting operations. It was found that the heat exchanger from LDPE used in this experiment is sturdy enough to withstand the pressure from the compaction of the medium-size pile in time and manual handling.
A limitation of this experiment is the radiating coil as heat appliance, which could not transfer enough heat to the hoop house air. This severely limited the measured power output, since the temperature difference between sensors Compost—In and Compost—Out stayed only around
on average (see
Figure 18).
Thermal Performace of the CHRS
Figure 15 shows the period of 36 days (days 9–45) when the temperature measurements could be used for the estimation of the heat recovery directly from the operational data. It was found the average power output of 655 W with overall 574 kWh or 510 kJ/kg DM of heat recovered over this period. Note that this time period is just a part of the compost lifetime, when heat could be captured.
The readings for a 5-day period (days 14–18) were presented in
Figure 17. Analysis of temperature differences (
Figure 18) and the heat recovered in each day were coupled with cumulative heat recovery (
Figure 19). It was found the average power output of 622 W and total 75 kWh or
kJ/kg DM of heat (over 5-day period) is recovered. Note that the core temperature measured inside the central aeration channel was not affected by the heat removal.
Power for the circulation pump: input 15 W or kWh/day of electricity was the only input in order to run the CHRS (since the pump was on only 12 h/day). Average net energy recovery of the CHRS can therefore be calculated as kWh/day in the form of heat. Extrapolating the average heat production from the beginning of the thermophilic phase (day 3) to day 45, we can estimate the average net heat recovery of kWh per 42 days.
To evaluate the overall performance of presented CHRS, the heat source (bioreactor) provided considerable amount of energy that could be captured. Unfortunately, the utilization system (the radiating coil as heat appliance) was able to transfer only 1 kW in average. Therefore, heat recovery was limited especially during the first weeks of thermophilic phase, when the potential power output peaked around kW. Thus, the presented results are severely limited by the underestimated power output of the appliance and not the heat source.
Comparing the results with review articles on various CHRS’s [
5], the lab-scale reactors reached a heat recovery rate 1895 kJ/h
kW and pilot-scale reactors reached 20,035 kJ/h
kW. Our composting system with a condenser-type heat exchanger had peak power output of 13,940 kJ/h
W and longterm average power output of 2358 kJ/h
W. With proper heat appliance, we estimate that the measured power output would increase four times. Future work will be therefore focusing on improvements of the heat appliance as well as the heat exchanger design and manufacturing for higher recovery rates.
The plastic foil stretched over the southern side of the bioreactor (see
Figure 13) protected not only the heat utilization system, but it also created a hoop house structure. The bioreactor itself provided thermal mass and insulation from the northern side. Heat could be therefore dissipated through the uninsulated north wall and contributed to the elevated temperature inside the hoop house. Temperature readings shown in
Figure 15 indicate only two days (day
) over the winter months (December and January) with below-zero temperatures.
It is important to note that the position of the probe inside the hoop house is approximately 50 cm from the ground and close to the reactor. More experimental research is needed for verification, if this kind of structure is able to keep the air (and soil) in the hoop house warm throughout the whole winter. Applications of compost-generated heat in greenhouses and hoop houses are promising, especially due to its synergistic relationship: compost produces heat, nutrients and CO2 and the enhanced growth of plants then provides feedstock for composting.With the results obtained from this study, we plan to explore concepts for heating of green and hoop houses using compost heat.
Lastly, the performance of composting reactors depends on various factors including size and shape of the pile, initial compost mixture, moisture, porosity of the material, etc. Regarding only the volume of the pile, cylindrical piles with larger diameter and height perform better due to their lower area-to-volume ratio. Heat losses are therefore reduced and more heat can be used for recovery. Larger piles are also able to produce heat for longer periods (piles 6 m in diameter,
m high should provide usable heat for more than 12 months, [
19]).
5. Conclusions
This paper introduces a new design of condenser-type heat exchanger for compost heat recovery systems. The main advantage compared to the buried-types hydronic heat exchangers is the extraction of a more abundant latent part from the overall enthalpy contained in compost vapours, thus enhancing the heat recovery rate. The exchanger uses natural convection (chimney effect) inside the compost pile. Hot and moist gases rise through vertical aeration channels to the cavity created on top of the mound and condense on the heat exchanger surface. Due to this heat removal method, a potential adverse effect on heat generation (driven by microbial activity) is reduced, since no direct heat removal in active composting zone is applied.
Moreover, moisture retention is achieved since the condensed water stays in the pile. From the practical point of view, the major advantage of this exchanger is that it can be installed after the compost mound is finished. This design simplifies the construction and allows machinery manipulation without damaging the exchanger.
The exchanger was tested with a passively aerated static pile (modified Jean Pain mound) and hydronic heat utilization system inside the ad hoc constructed hoop house. Temperature dynamics and performance were measured and evaluated in order to compare with other CHRS’s [
5]. Unfortunately, power output of the final appliance was chosen below the possible power output of the heat source (bioreactor). The heat recovery was therefore severely limited by the transfer and utilization parts of the CHRS, not by the heat source itself. As a recommendation for the following experiments, these parts of the system need to be adjusted in order to gain maximal heat recovery rate from the bioreactor.