15Cellular function depends on heterogeneous dynamic intra-, inter-, and supramolecular structure-16 function relationships. However, the specific mechanisms by which cellular function is 17 transduced from molecular systems, and by which cellular dysfunction arises from molecular 18 dysfunction are poorly understood. We proposed previously that cellular function manifests as a 19 molecular form of analog computing, in which specific time-dependent state transition fluxes 20 within sets of molecular species ("molecular differential equations" (MDEs)) are sped and 21 slowed in response to specific perturbations (inputs). In this work, we offer a theoretical 22 treatment of the molecular mechanisms underlying cellular analog computing (which we refer to 23 as "biodynamics"), focusing primarily on non-equilibrium (dynamic) intermolecular state 24 transitions that serve as the principal means by which MDE systems are solved (the molecular 25 equivalent of mathematical "integration"). Under these conditions, bound state occupancy is 26 governed by and , together with the rates of binding partner buildup and decay.
27Achieving constant fractional occupancy over time depends on: 1) equivalence between k on and 28 the rate of binding site buildup); 2) equivalence between and the rate of binding site decay; 29 and 3) free ligand concentration relative to / (n K d , where n is the fold increase in 30 binding partner concentration needed to achieve a given fractional occupancy). Failure to satisfy 31 these conditions results in fractional occupancy well below that corresponding to n K d . The
32implications of biodynamics for cellular function/dysfunction and drug discovery are discussed. 33 34 35 45 46 Enzyme-substrate: -( ) 47 48 where represents the rates of non-equilibrium occupancy buildup and decay of state k ( )/ 49 from one or more predecessor to one or more successor states. State transition rates are governed 50 by adjustable barriers originating from intra-or intermolecular interactions (which we referred to 51 as "intrinsic rates") and time-dependent changes in the concentrations or number densities of the 52 participating species (which we referred to as "extrinsic rates") [1]. Molecular populations "flow" 53 over time in a transient (Markovian) fashion from one specific structural state to another (Fig 1) 54 in response to production/degradation or translocation-driven changes in the levels of the 55 participating species. 56 Fig 1. (A) Markovian state transition behavior exemplified for the human cardiac ether-a-57 go-go related gene (hERG) potassium channel between closed (C1, C2, and C3), open (O) 58 and inactivated states (I) underlying the state probability curves in (B) [4]. The rate 59 constants are labeled with Greek letters. (B) Molecular populations of hERG "flow" from 60 one specific state to another based on intrinsic voltage-dependent rates of entry and exit. 61 Multiple fluxes occur in parallel between specific states, speeding and slowing in response 62 to dynamic perturbations. For ex...