Theoretische Physik II, Physikalisches Institut, Universität Bayreuth, D-95440 Bayreuth, Germany.
J Chem Phys. 2019 Feb 21;150(7):074112. doi: 10.1063/1.5061764.
We generalize power functional theory [Schmidt and Brader, J. Chem. Phys. 138, 214101 (2013)] to Brownian many-body systems with orientational degrees of freedom. The framework allows the study of active particles in general inhomogeneous and time-dependent nonequilibrium. We prove for steady states that the free power equals half the negative dissipated external work per time, and is hence trivially related to the average forward swim speed of the particles. The variational theory expresses the free power as a functional of the microscopic one-body density and current distribution. Both fields are time-, position- and orientation-dependent, and the total current consists of translational and rotational parts. Minimization of the free power functional with respect to the current(s) yields the physical dynamics of the system. We give a simple approximation for the superadiabatic (above adiabatic) contribution which describes excess dissipation in homogeneous bulk fluids due to drag. In steady states, we evaluate the free power using Brownian dynamics simulations for short-ranged soft repulsive spheres. We describe the necessary sampling strategies and show that the theory provides a good account of the simulation data.
我们将幂次泛函理论[Schmidt 和 Brader, J. Chem. Phys. 138, 214101 (2013)]推广到具有取向自由度的布朗多体系统。该框架允许对一般的非平衡、不均匀和时变的活性粒子进行研究。我们证明了在稳态下,自由能等于单位时间内负耗散外部功的一半,因此与粒子的平均前向游动速度有直接关系。变分理论将自由能表示为微观单粒子密度和电流分布的泛函。这两个场都是与时间、位置和取向相关的,总电流由平移和旋转两部分组成。通过最小化自由能泛函对电流的偏导数,可以得到系统的物理动力学。我们给出了超绝热(超过绝热)贡献的一个简单近似,它描述了由于拖曳导致均匀体相流体中过度耗散的情况。在稳态下,我们使用短程软排斥球的布朗动力学模拟来计算自由能。我们描述了必要的采样策略,并表明该理论很好地解释了模拟数据。