Supporting Information 1 2 3 High spatial resolution of distribution and interconnections 4 between Fe- and N-redox processes in profundal lake sediments 5 Melton E.D.1, Stief P.2, Behrens, S.1, Kappler A.1 & Schmidt C.1* 6 7 8 1. 9 2. Geomicrobiology, Center for Applied Geosciences, University of Tübingen, Tübingen, Germany Microsensor Research Group, Max Planck Institute for Marine Microbiology, Bremen, Germany 10 (2.Department of Biology, University of Southern Denmark, Odense, Denmark) 11 *corresponding author: 12 13 14 Caroline Schmidt, Geomicrobiology, Center for Applied Geosciences 15 University of Tübingen, Sigwartstraße 10, D-72076 Tübingen, Germany 16 Phone: +49-7071-2974790, Fax: +49-7071-295059 17 Email: caroline.schmidt@uni-tuebingen.de 18 19 Running Title: Microbial Fe and N redox cycling in lake sediments 20 1 21 Supporting Information 22 23 Figure S1: Geochemical gradients in profundal Lake Constance sediments. 24 The grey filled black squares represent the fit of the measured concentration profiles obtained by 25 diffusion-reaction modelling with Profile 1.0 (Berg et al., 1998). The measured concentration profiles 26 are shown as open black squares. A) Oxygen (O2). B) Nitrate (NO3-). C) Ammonium (NH4+). 27 28 Material & Methods 29 Diffusion-reaction modelling of microsensor concentration profiles 30 The average concentration profiles of O2, NO3-, and NH4+ were used to derive the vertical sequence 31 of production and consumption zones of these solutes in the sediment (Fig. S1). Diffusion-reaction 32 modelling was carried out using the program Profile 1.0 (Berg et al. 1998). The calculation domain 33 was set to reach from the sediment surface to the maximum depth at which microsensor profiling 34 resulted in reliable readings (O2: 20 mm, NO3-: 17.5 mm, and NH4+: 16.5 mm). A few obvious outliers 35 were manually removed from the concentration profiles (NO3-: 4 out of 39 measuring points, NH4+: 1 36 out of 60 measuring points). Boundary conditions were selected according to the availability of data 37 (O2 and NO3-: concentration at the top and flux at the bottom of the calculation domain, NH4+: 38 concentrations at the top and bottom of the calculation domain). The diffusivities of O2, NO3-, and 39 NH4+ in water (D0) at 15°C were taken as 1.80 · 10-5 cm2 · s-1, 1.47 · 10-5 cm2 · s-1, and 1.54 · 10-5 cm2 · 40 s-1, respectively (Stief et al. 2002). The effective diffusivities in sediment (Ds) were calculated by the 41 program as Ds = D0 · Ο2, where Ο is the sediment porosity of 0.806. Model runs were repeated with 42 different numbers of equally spaced conversion zones allowed until the modelled concentration 2 43 profiles fitted satisfactorily the measured concentration profiles. The vertical sequence of 44 production and consumption zones of O2, NO3-, and NH4+ obtained in the best model run is 45 presented. 46 47 Thermodynamic calculations 48 The Gibbs free energy was determined based on the geochemical concentrations measured at each 49 depth in the profile and the sediment pore water DOC. Dissolved ferrous iron concentration were 50 taken from preliminary voltammetric microsensor measurements in the profundal sediments of Lake 51 Constance (data not shown). Solid compounds, gases and water were considered to be 1 in the 52 calculations. The H+ concentration was based on the pH microelectrode measurements. 53 theoretical energetic budget βG at 25°C was determined by: 54 βπΊ = βπΊ0 − π π πππ 55 where βG0 is the standard Gibbs free energy at 25°C and pH 0 for the respective reaction equation, R 56 is the ideal gas constant, T is the temperature (in K) and Q expresses the equilibrium conditions for 57 the respective reaction equation: 58 π= 59 for the general reaction equation: 60 ππ΄ + ππ΅ ↔ ππΆ + ππ· 61 The considered reactions for the energy computation and the respective βG0 values are as follows: 62 πΉπ 2+ + π» + + π2 →→ πΉπ 3+ + π»2 π 63 πΉπ 2+ + 4 π2 + 64 πΉπ 2+ + 5 ππ3− + 5 π» + → πΉπ 3+ + 10 π2 + 5 π»2 π 65 πΉπ 2+ + 5 ππ3− + 66 8πΉπ(ππ»)3 + πΆπ»3 πΆππ− + 17π» + → 8πΉπ 2+ + 2πΆπ2 + 22π»2 π The {πΆ}π {π·}π {π΄}π {π΅}π 1 4 1 10 π» π 4 2 1 2 βG0 = -44 kJ.mol-1 → πΉπ(ππ»)3 + 2π» + βG0 = -36 kJ.mol-1 1 6 1 12 π» π 5 2 1 → πΉπ(ππ»)3 + 3 1 π 10 2 βG0 = -46 kJ.mol-1 9 + 5 π»+ βG0 = -38 kJ.mol-1 βG0 = -72 kJ.mol-1 67 3