Author Affiliations
1Department of Physics, Nantong University, Nantong 22609, China2School of Information Science and Technology, Nantong University, Nantong 6019, Chinashow less
Fig. 1. Nonregular cylindrical m × n resistor network, where m and n are the numbers of resistors along the cycle and horizontal directions respectively, with unit resistors r and r0 in the respective horizontal and loop directions except for two arbitrary boundary resistors of r1 and r2.
Fig. 2. Resistor sub-network with resistors and potential parameters.
Fig. 3. m × n cobweb network with arbitrary left boundary resistor of r1.
Fig. 4. Arbitrary m × n globe network, where m and n are the number of grids along the cycle direction and horizontal direction respectively, with the resistors r and r0 in horizontal direction and loop direction, respectively.
Fig. 5. 3D □ × n network with resistors r and r0 in respective horizontal and vertical directions except for r1 and r2 on the left and right edges.
Fig. 6. 3D Δ × n network with resistors r and r0 in the respective horizontal and vertical directions except for r1 and r2 on the left and right edges.
Fig. 7. 3D graph showing equivalent resistance R(A0, Ak) changing with h and x in Δ × n network, and resistance R(A0, Ax) increasing with augment of n and x, where R(A0, A0) = 0 when x = 0.
Fig. 8. 3D graph showing equivalent resistance R(A0, Bk) changing with h and x in Δ × n network, and the resistance R(A0, Bx) increasing with argument of n and x, where R(A0, B0) > 0 when x = 0.
Fig. 9. 3D graph showing equivalent resistance R(A0, B0) changing with h and n in Δ × n network, R(A0, B0) decreasing with the increase of n, and R(A0, B0) increasing with argument of h except for n = 0.
Fig. 10. 3D graph showing equivalent resistance R(A0, Ak) changing with h and x in □ × n network, and resistance R(A0, Ax) increasing with augment of n and x, where R(A0, A0) = 0 when x = 0.
Fig. 11. 3D graph showing equivalent resistance R(A0, Ck) changing with h and x in □ × n network, and resistance R(A0, Cx) incresing with augment of n and x, where R(A0, C0) > 0 when x = 0.
Fig. 12. Crystal lattice with resistors r and r0 in respective horizontal and vertical directions.