• Chinese Physics B
  • Vol. 29, Issue 8, (2020)
Zhi-Zhong Tan1、† and Zhen Tan2
Author Affiliations
  • 1Department of Physics, Nantong University, Nantong 22609, China
  • 2School of Information Science and Technology, Nantong University, Nantong 6019, China
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    DOI: 10.1088/1674-1056/ab96a7 Cite this Article
    Zhi-Zhong Tan, Zhen Tan. Electrical properties of m × n cylindrical network[J]. Chinese Physics B, 2020, 29(8): Copy Citation Text show less
    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. 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.
    Resistor sub-network with resistors and potential parameters.
    Fig. 2. Resistor sub-network with resistors and potential parameters.
    m × n cobweb network with arbitrary left boundary resistor of r1.
    Fig. 3. m × n cobweb network with arbitrary left boundary resistor of r1.
    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. 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.
    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. 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.
    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. 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.
    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. 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.
    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. 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.
    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. 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.
    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. 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.
    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. 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.
    Crystal lattice with resistors r and r0 in respective horizontal and vertical directions.
    Fig. 12. Crystal lattice with resistors r and r0 in respective horizontal and vertical directions.
    Zhi-Zhong Tan, Zhen Tan. Electrical properties of m × n cylindrical network[J]. Chinese Physics B, 2020, 29(8):
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