Author Affiliations
1Science Education Department, Beijing Institute of Graphic Communication, Beijing 02600, China2Institute of Systems Science and College of Information Science and Engineering, Huaqiao University, Xiamen 36101, China3School of Science, Tianjin University, Tianjin 00072, China4School of Science, Hebei University of Technology, Tianjin 30001, China5School of Printing and Packaging Engineering, Beijing Institute of Graphic Communication, Beijing 102600, China6College of Science, Hebei Institute of Architecture and Civil Engineering, Zhangjiakou 075000, Chinashow less
Fig. 1. Schematic diagram of coupled Brownian motors in the two-dimensional traveling-wave potential V(x,y).
Fig. 2. The current υ versus the angular frequency ω for different values of (a) the coupling strength k at D = 5.0 and (b) the noise intensity D at k = 3.0, with other parameters being γ = 1.0, a = 5.0, V0 = 3.0, λ = 3.0, and ε = 0.2.
Fig. 3. The current υ versus the wavelength λ for different values of the angular frequency ω, with other parameters being γ = 1.0, a = 5.0, V0 = 3.0, k = 3.0, D = 5.0, and ε = 0.2.
Fig. 4. The current υ versus (a) the coupling strength k for different values of the angular frequency ω, and (b) the coupling strength k and the angular frequency ω with other parameters being γ = 1.0, a = 5.0, V0 = 3.0, λ = 3.0, D = 5.0, and ε = 0.2.
Fig. 5. The current υ versus (a) the free length of the spring a for different values of the angular frequency ω, and (b) the free length of the spring a and the angular frequency ω, with other parameters being γ = 1.0, k = 3.0, V0 = 3.0, γ = 3.0, D = 5.0, and ε = 0.2.
Fig. 6. The current υ versus (a) the noise intensity D for different values of the angular frequency ω, and (b) the noise intensity D and the angular frequency ω, with other parameters being γ = 1.0, k = 3.0, a = 5.0, V0 = 3.0, λ = 3.0, and ε = 0.2.