WHAT IS THE MAXIMAL POSSIBLE SOIL METHANE UPTAKE?

M. Glagolev, G. Suvorov, D. V. Il’yasov, A. Sabrekov, I. Terentieva
{"title":"WHAT IS THE MAXIMAL POSSIBLE SOIL METHANE UPTAKE?","authors":"M. Glagolev, G. Suvorov, D. V. Il’yasov, A. Sabrekov, I. Terentieva","doi":"10.18822/edgcc133609","DOIUrl":null,"url":null,"abstract":"The spread of published values of the rate of methane uptake by soils makes up several orders of magnitude from 0.0001 to 1 mgm-2h-1, which is comparable in magnitude to the spread of estimates of the release of CH4 out of waterlogged soils. The high values of CH4 emissions out of waterlogged soils are well explained, since with high methane production, it can be removed from the soil at almost any speed through a convective (most often bubble) transport mechanism. But when being absorbed by the soil, methane can penetrate in it only due to an apparently slow diffusion mechanism. Thus, the question arises of the maximum theoretically justified assessment of methane consumption by the soil. The aim of our work was to try to quantify the maximum possible amount of CH4 consumption by the soil relying on a strict basis of soil biokinetics and physics. \nTo estimate the maximum specific absorption flux of CH4 by the soil, we used the \"mass conservation equation\" [Walter et al., 1996; Zhuang et al., 2004; Глаголев, 2006, p. 316; 2010, p. 35-36]: \n \nC/t = -F/z + Qebull + Qplant + Rprod + Roxid, \n \nwhere C (mg/m3) is the concentration of methane at time t at depth z; F (mgm-2h-1) is the specific flux of methane due to diffusion; Qebull and Qplant (mgm3h-1) are the rates of change in methane concentration at time t at depth z due to the formation of bubbles and drainage through the roots of plants, respectively; Rprod and Roxid (mgm-3 h-1) are the rates of formation and consumption of methane, respectively. \nSince we going to estimate the flux of CH4 only at its maximum possible consumption, the equation is simplified, as far as its terms accounted for the formation and transport of methane (Rprod, Qebull, Qplant) will be equal to 0. Finally, we will consider the system in a steady state, i.e. C/t=0. Thus:F(t,z)/z = Roxid(t,z). \nUsing Fick's first law to calculate the diffusion flux (used with a modified sign compared to its traditional form): \n \nF(t,z) = D(z)C/z, \n \nwhere D(z) is the diffusion coefficient [Zhuangetal.,2004]; and the modified Michaelis-Menten equation for calculating methane oxidation is:Roxid(t,z) = -Vmax(C-CTh)/(KM + C-CTh), where CTh (mgm-3) is the threshold concentration [Panikov, 1995, p. 151]; Vmax (mgm-3h-1) is the maximum specific consumption rate; KM (mgm-3) is the halfsaturation constant, and also under assumptions, (i) the concentration of CH4 is approximately equal to atmospheric (CA=1.29mg/m3) at the upper boundary (soil/atmosphere); (ii) the flux of CH4 can be assumed to be zero at an infinitely great depth [Born et al., 1990]; (iii) D, Vmax and KM (C- CTh) do not change with depth. Therefore, the absolute value of the specific flux from the atmosphere to the soil is: \n \n|F(0)|= (CA-CTh)(VmaxD/KM). \n \nThe maximum value of the diffusion coefficient can be estimated by the Penman equation: D=D oPa0.66, where Do is the diffusion coefficient in air; Pa is the porosity of aeration [Смагин,2005,p.165]. Since we are going to estimate the maximum value of diffusion, we will take the limit value of porosity, which is 1, but as far as the proportion of pores of stable aeration accounts for half of the total pore volume [Растворова,1983,p.52], then for further calculations we will take Pa = 0.5, hence D = D o0.33. According to [Arah andStephen, 1998], for CH4 \n \nDo = 1.910-5∙(T/273)1.82 m2/s = 6.810-2∙(T/273)1.82 m2/h, \n \nwhere T is temperature (K). When solving our diffusion problem, we assumed that the temperature is the same throughout the soil profile, and is 293 K. then D=6.810-2∙(293/273)1.820.33 = 2.5510-2m2/h. \nThe maximum rate of CH4 oxidation by soil was experimentally estimated in [Bender and Conrad, 1992] and was 57.3 mg/(hm3), which is in good agreement with the value of Vmax=47mg/(hm3) obtained at T=32 C according to the temperature dependence for automorphic soils of boreal forests Vmax=1.5(T ‑5.4)/10mmol/(hL), given in the work of Zhuang et al. [2004]. \nThe halfsaturation constant is the concentration of the substrate, at which the specific growth rate of microorganisms takes a value equal to a half of the maximum. Summaries of the values KM have been repeatedly published (see, for example, [King,1992,Tab.II; Segers,1998,Tab.4; Глаголев,2006,pp.324-325]). For our purposes, we should take the KM obtained directly in the experiments with substrate concentrations (CH4) closest to those found in natural conditions. The minimum value (310-8mol/L) is given in [Bender and Conrad, 1992]. This value corresponds to the methane concentration in the air of about 20 ppm (14.3 mg/m3). This КМ value will be taken for further calculations. \nThe threshold concentration of CH4 for methanotrophs in the upper soil layer, given in the scientific literature, varies from 0.1 to 3.5 ppm [Crill, 1991; Bender and Conrad, 1992; Kravchenko et al., 2010]. Since we are interested in the minimum value of this indicator, we will bring it to the minimum temperature (273 K or 0 C): CTh=0.0714 mg/m3. \nNow, having all the necessary numerical values, we can estimate the maximum intensity of methane consumption by natural soils: \n|F(0)|= 1.2186(57.32.5510-2/14.3)0.39mg/(m2h). \n \nThus, for a certain \"ideal\" soil (evenly warmed throughout the profile, perfectly aerated, and at the same time containing enough moisture to create optimal living conditions for methanotrophs, which, by the way, are extremely numerous in the soil, and their methane halfsaturation constant is very low, etc.) we obtained an absorption intensity of CH4 of about 0.39 mg/(m2h). Since the combination of optimal values of all factors affecting methane consumption is very unlikely (or, rather, even improbable) in real soils, the resulting value can be considered extremely possible. And in view of this, the empirical generalization made in [Crill, 1991] becomes clear: \"From the Amazon floodplain to the Arctic, the most rapid rates rarely exceed 6 mgCH4m-2d-1\" i.e. 0.25 mg/(m2h). \nConclusion. So, we considered the absorption of methane as a biochemical process (following the Michaelis-Menten law with certain kinetic parameters), limited by diffusion in porous medium (soil). Based on this theoretical analysis, we came to the conclusion that the extremely large values of the specific absorption flux of CH4 (about 0.4 mgm-2h-1 and more), which are sometimes found in the literature, are unrealistic, if we are talking about the soils, which are always under methane concentrations no greater than atmospheric 1.8 ppmv. This applies to the vast majority of soils almost all, except for wetlands and soils covering landfills, underground gas storage facilities or other powerful sources of methane.","PeriodicalId":336975,"journal":{"name":"Environmental Dynamics and Global Climate Change","volume":"4173 2 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2023-01-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"2","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Environmental Dynamics and Global Climate Change","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.18822/edgcc133609","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 2

Abstract

The spread of published values of the rate of methane uptake by soils makes up several orders of magnitude from 0.0001 to 1 mgm-2h-1, which is comparable in magnitude to the spread of estimates of the release of CH4 out of waterlogged soils. The high values of CH4 emissions out of waterlogged soils are well explained, since with high methane production, it can be removed from the soil at almost any speed through a convective (most often bubble) transport mechanism. But when being absorbed by the soil, methane can penetrate in it only due to an apparently slow diffusion mechanism. Thus, the question arises of the maximum theoretically justified assessment of methane consumption by the soil. The aim of our work was to try to quantify the maximum possible amount of CH4 consumption by the soil relying on a strict basis of soil biokinetics and physics. To estimate the maximum specific absorption flux of CH4 by the soil, we used the "mass conservation equation" [Walter et al., 1996; Zhuang et al., 2004; Глаголев, 2006, p. 316; 2010, p. 35-36]: C/t = -F/z + Qebull + Qplant + Rprod + Roxid, where C (mg/m3) is the concentration of methane at time t at depth z; F (mgm-2h-1) is the specific flux of methane due to diffusion; Qebull and Qplant (mgm3h-1) are the rates of change in methane concentration at time t at depth z due to the formation of bubbles and drainage through the roots of plants, respectively; Rprod and Roxid (mgm-3 h-1) are the rates of formation and consumption of methane, respectively. Since we going to estimate the flux of CH4 only at its maximum possible consumption, the equation is simplified, as far as its terms accounted for the formation and transport of methane (Rprod, Qebull, Qplant) will be equal to 0. Finally, we will consider the system in a steady state, i.e. C/t=0. Thus:F(t,z)/z = Roxid(t,z). Using Fick's first law to calculate the diffusion flux (used with a modified sign compared to its traditional form): F(t,z) = D(z)C/z, where D(z) is the diffusion coefficient [Zhuangetal.,2004]; and the modified Michaelis-Menten equation for calculating methane oxidation is:Roxid(t,z) = -Vmax(C-CTh)/(KM + C-CTh), where CTh (mgm-3) is the threshold concentration [Panikov, 1995, p. 151]; Vmax (mgm-3h-1) is the maximum specific consumption rate; KM (mgm-3) is the halfsaturation constant, and also under assumptions, (i) the concentration of CH4 is approximately equal to atmospheric (CA=1.29mg/m3) at the upper boundary (soil/atmosphere); (ii) the flux of CH4 can be assumed to be zero at an infinitely great depth [Born et al., 1990]; (iii) D, Vmax and KM (C- CTh) do not change with depth. Therefore, the absolute value of the specific flux from the atmosphere to the soil is: |F(0)|= (CA-CTh)(VmaxD/KM). The maximum value of the diffusion coefficient can be estimated by the Penman equation: D=D oPa0.66, where Do is the diffusion coefficient in air; Pa is the porosity of aeration [Смагин,2005,p.165]. Since we are going to estimate the maximum value of diffusion, we will take the limit value of porosity, which is 1, but as far as the proportion of pores of stable aeration accounts for half of the total pore volume [Растворова,1983,p.52], then for further calculations we will take Pa = 0.5, hence D = D o0.33. According to [Arah andStephen, 1998], for CH4 Do = 1.910-5∙(T/273)1.82 m2/s = 6.810-2∙(T/273)1.82 m2/h, where T is temperature (K). When solving our diffusion problem, we assumed that the temperature is the same throughout the soil profile, and is 293 K. then D=6.810-2∙(293/273)1.820.33 = 2.5510-2m2/h. The maximum rate of CH4 oxidation by soil was experimentally estimated in [Bender and Conrad, 1992] and was 57.3 mg/(hm3), which is in good agreement with the value of Vmax=47mg/(hm3) obtained at T=32 C according to the temperature dependence for automorphic soils of boreal forests Vmax=1.5(T ‑5.4)/10mmol/(hL), given in the work of Zhuang et al. [2004]. The halfsaturation constant is the concentration of the substrate, at which the specific growth rate of microorganisms takes a value equal to a half of the maximum. Summaries of the values KM have been repeatedly published (see, for example, [King,1992,Tab.II; Segers,1998,Tab.4; Глаголев,2006,pp.324-325]). For our purposes, we should take the KM obtained directly in the experiments with substrate concentrations (CH4) closest to those found in natural conditions. The minimum value (310-8mol/L) is given in [Bender and Conrad, 1992]. This value corresponds to the methane concentration in the air of about 20 ppm (14.3 mg/m3). This КМ value will be taken for further calculations. The threshold concentration of CH4 for methanotrophs in the upper soil layer, given in the scientific literature, varies from 0.1 to 3.5 ppm [Crill, 1991; Bender and Conrad, 1992; Kravchenko et al., 2010]. Since we are interested in the minimum value of this indicator, we will bring it to the minimum temperature (273 K or 0 C): CTh=0.0714 mg/m3. Now, having all the necessary numerical values, we can estimate the maximum intensity of methane consumption by natural soils: |F(0)|= 1.2186(57.32.5510-2/14.3)0.39mg/(m2h). Thus, for a certain "ideal" soil (evenly warmed throughout the profile, perfectly aerated, and at the same time containing enough moisture to create optimal living conditions for methanotrophs, which, by the way, are extremely numerous in the soil, and their methane halfsaturation constant is very low, etc.) we obtained an absorption intensity of CH4 of about 0.39 mg/(m2h). Since the combination of optimal values of all factors affecting methane consumption is very unlikely (or, rather, even improbable) in real soils, the resulting value can be considered extremely possible. And in view of this, the empirical generalization made in [Crill, 1991] becomes clear: "From the Amazon floodplain to the Arctic, the most rapid rates rarely exceed 6 mgCH4m-2d-1" i.e. 0.25 mg/(m2h). Conclusion. So, we considered the absorption of methane as a biochemical process (following the Michaelis-Menten law with certain kinetic parameters), limited by diffusion in porous medium (soil). Based on this theoretical analysis, we came to the conclusion that the extremely large values of the specific absorption flux of CH4 (about 0.4 mgm-2h-1 and more), which are sometimes found in the literature, are unrealistic, if we are talking about the soils, which are always under methane concentrations no greater than atmospheric 1.8 ppmv. This applies to the vast majority of soils almost all, except for wetlands and soils covering landfills, underground gas storage facilities or other powerful sources of methane.
最大可能的土壤甲烷吸收量是多少?
已公布的土壤甲烷吸收速率值的传播范围从0.0001到1 mg -2h-1不等,这与浸水土壤释放CH4的估计值的传播范围相当。浸水土壤中CH4的高排放值可以很好地解释,因为由于甲烷产量高,它可以通过对流(通常是气泡)运输机制以几乎任何速度从土壤中移除。但是当甲烷被土壤吸收时,由于明显缓慢的扩散机制,甲烷只能渗透到土壤中。因此,产生了一个问题,即对土壤甲烷消耗的最大理论合理评估。我们的工作目的是在严格的土壤生物动力学和物理学基础上,试图量化土壤消耗CH4的最大可能量。为了估算土壤对CH4的最大比吸收通量,我们使用了“质量守恒方程”[Walter et al., 1996;庄等,2004;Глаголев, 2006,第316页;[j]: C/t = -F/z + Qebull + Qplant + Rprod + Roxid,其中C (mg/m3)为深度z时刻的甲烷浓度;F (mg -2h-1)为甲烷扩散比通量;Qebull和Qplant (mgm3h-1)分别为深度z处t时刻由于气泡形成和植物根部排水引起的甲烷浓度变化率;Rprod和Roxid (mg -3 h-1)分别是甲烷的生成速率和消耗速率。由于我们只估计最大可能消耗时的CH4通量,因此简化了方程,因为方程中用于甲烷形成和输送的项(Rprod, Qebull, Qplant)等于0。最后,我们考虑系统处于稳态,即C/t=0。因此:F(t,z)/z = Roxid(t,z)。利用菲克第一定律计算扩散通量(与传统形式相比,符号有所修改):F(t,z) = D(z)C/z,其中D(z)为扩散系数[Zhuangetal.,2004];计算甲烷氧化的修正Michaelis-Menten方程为:Roxid(t,z) = -Vmax(C-CTh)/(KM + C-CTh),其中CTh (mg -3)为阈值浓度[Panikov, 1995, p. 151];Vmax (mg -3h-1)为最大比消耗率;KM (mg -3)为半饱和常数,同样在假设下,(i) CH4的浓度在上界(土壤/大气)近似等于大气(CA=1.29mg/m3);(ii)可以假设CH4的通量在无限深处为零[Born et al., 1990];(iii) D、Vmax和KM (C- CTh)不随深度变化。因此,大气到土壤的比通量绝对值为:|F(0)|= (CA-CTh)(VmaxD/KM)。扩散系数的最大值可由Penman方程估计:D=D oPa0.66,其中Do为空气中的扩散系数;Pa为曝气孔隙率[Смагин,2005,p.165]。由于我们要估计扩散的最大值,所以我们取孔隙率的极限值为1,但就稳定通气的孔隙占总孔隙体积的一半而言[Растворова,1983,p. 1]。[52],那么为了进一步的计算,我们将取Pa = 0.5,因此D = d0.33。根据[Arah and stephen, 1998],对于CH4 Do = 1.910-5∙(T/273)1.82 m2/s =6.810-2∙(T/273)1.82 m2/h,其中T为温度(K)。在求解扩散问题时,我们假设整个土壤剖面的温度相同,为293 K,则D=6.810-2∙(293/273)1.820.33 = 2.5510-2m2/h。[Bender and Conrad, 1992]实验估计土壤CH4氧化的最大速率为57.3 mg/(hm3),这与Zhuang等[2004]根据北方森林自同态土壤的温度依赖,在T=32℃时得到的Vmax=47mg/(hm3)的值吻合得很好。半饱和常数是底物的浓度,在此浓度下,微生物的特定生长速率等于最大值的一半。关于KM值的总结已被反复发表(例如,参见[King,1992, table ii;塞格尔,1998年,Tab.4;Глаголев,2006,打印- 325])。就我们的目的而言,我们应该采用在底物浓度(CH4)最接近自然条件下的实验中直接获得的KM。最小值(310-8mol/L)在[Bender and Conrad, 1992]中给出。这一数值相当于空气中甲烷浓度约为20 ppm (14.3 mg/m3)。此КМ值将用于进一步计算。科学文献中给出的上层土壤中甲烷氧化菌CH4的阈值浓度在0.1至3.5 ppm之间变化[Crill, 1991;Bender and Conrad, 1992;Kravchenko et al., 2010]。由于我们对该指标的最小值感兴趣,我们将其调至最低温度(273 K或0℃):CTh=0.0714 mg/m3。 现在,有了所有必要的数值,我们可以估计出天然土壤甲烷消耗的最大强度:|F(0)|= 1.2186(57.32.5510-2/14.3)0.39mg/(m2h)。因此,对于某种“理想”土壤(整个剖面均匀升温,完全通气,同时含有足够的水分,为甲烷氧化菌创造最佳的生存条件,顺便说一句,甲烷氧化菌在土壤中数量非常多,它们的甲烷半饱和常数非常低,等等),我们获得了约0.39 mg/(m2h)的CH4吸收强度。由于影响甲烷消耗的所有因素的最佳值的组合在实际土壤中是非常不可能的(或者更确切地说,甚至是不可能的),因此所得值可以认为是极有可能的。鉴于此,在[Crill, 1991]中所做的经验概括变得清晰起来:“从亚马逊河漫滩到北极,最快的速率很少超过6毫克/立方米/小时”,即0.25毫克/立方米/小时。结论。因此,我们认为甲烷的吸收是一个生化过程(遵循Michaelis-Menten定律,具有一定的动力学参数),受多孔介质(土壤)扩散的限制。基于这一理论分析,我们得出结论,文献中有时发现的CH4的比吸收通量的极大值(约0.4 mg -2h-1及以上)是不现实的,如果我们谈论的是土壤,甲烷浓度总是不大于大气1.8 ppmv。这适用于绝大多数土壤,除了湿地和覆盖垃圾填埋场、地下储气设施或其他强大的甲烷来源的土壤。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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