Three-dimensional coil set used for neuromodulation
US-2021154488-A1 · May 27, 2021 · US
US12478796B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-12478796-B2 |
| Application number | US-202217694812-A |
| Country | US |
| Kind code | B2 |
| Filing date | Mar 15, 2022 |
| Priority date | Oct 26, 2021 |
| Publication date | Nov 25, 2025 |
| Grant date | Nov 25, 2025 |
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The disclosure discloses a magnetic stimulation method with a controllable induced field direction, and belongs to the technical field of noninvasive neural regulation. The method includes the following steps: S 100 , determining currents i 1j , i 2j , i 3j , j=1, 2, . . . , n required to respectively generate unit vector electric fields at a target point P t , when the currents i 1j , i 2j , i 3j , are respectively applied through a coil j of a magnetic stimulation coil group, n≥3 and n being an integer; S 200 , decomposing an electric field E required at the target point P t to three electric field components E 1 , E 2 , E 3 ; S 300 , calculating currents I 1j , I 2j , I 3j that respectively generate the electric field components E 1 , E 2 , E 3 at the target point P t , I 1j =E 1 i 1j , I 2j =E 2 i 2j , I 3j =E 3 i 3j ; S 400 , generating the electric field E at the target point P t by applying a current I j =I 1j +I 2j +I 3j =E 1 i 1 +E 2 i 2 , I 3j +E 3 i 3 ; through the coil j, j=1, 2, . . . , n.
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What is claimed is: 1 . A method, comprising: S 100 , determining currents i 1j , i 2j , i 3j , j=1, 2, . . . n required to respectively generate unit vector electric fields at a target point P t , when the currents i 1j , i 2j , i 3j , are respectively applied through a coil j of a magnetic stimulation coil group, n≥3 and n being an integer; S 200 , decomposing an electric field E required at the target point P t to three electric field components E 1 , E 2 , E 3 ; S 300 , calculating currents I 1j , I 2j , I 3j that respectively generate the electric field components E 1 , E 2 , E 3 at the target point P t , I 1j =E 1 i 1j , I 2j =E 2 i 2j , I 3j =E 3 i 3j ; S 400 , generating the electric field E at the target point P t by applying a current I j =I 1j +I 2j +I 3j =E 1 i 1j +E 2 i 2j +E 3 i 3j through the coil j, j=1, 2, . . . , n. 2 . The method according to claim 1 , wherein the electric field components E 1 , E 2 , E 3 are mutually orthogonal.
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