Rail transit vehicle axle counter magnetic field EMC semi-physical simulation method
A rail transit vehicle, semi-physical simulation technology, applied in the direction of instruments, simulators, general control systems, etc., can solve problems such as the inability to fully simulate the working environment of the axle counter, test and actual use effects, and result errors, etc. Good and stable timeliness, reduced deviation, and accurate data
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Embodiment 1
[0050] A rail transit vehicle axle counter magnetic field EMC semi-physical simulation method, comprising the following steps:
[0051] S1. Digital simulation: establish a mathematical model in the Simulink environment, and the Maxwell's equations obeyed by the magnetic field around the axle counter are as follows:
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[0053]
[0054]
[0055]
[0056] Among them: Γ is the field quantity surface, ι is the boundary of Γ, S is the field boundary surface, H is the magnetic field strength, J is the dielectric current density, J s is the density of the external field source current, D is the potential vector, E is the electric field strength, B is the magnetic induction, and ρ is the charge density.
[0057] When the field quantity is continuous, the differential form to obtain its Maxwell equations is as follows:
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[0062] S2. Boundary derivation of magnetic field quantity: According to the above formula, we can ge...
Embodiment 2
[0079] A rail transit vehicle axle counter magnetic field EMC semi-physical simulation method, comprising the following steps:
[0080] S1. Digital simulation: establish a mathematical model in the Simulink environment, and the Maxwell's equations obeyed by the magnetic field around the axle counter are as follows:
[0081]
[0082]
[0083]
[0084]
[0085] Among them: Γ is the field quantity surface, ι is the boundary of Γ, S is the field boundary surface, H is the magnetic field strength, J is the dielectric current density, J s is the density of the external field source current, D is the potential vector, E is the electric field strength, B is the magnetic induction, and ρ is the charge density.
[0086] When the field quantity is continuous, the differential form to obtain its Maxwell equations is as follows:
[0087]
[0088]
[0089]
[0090]
[0091] S2. Boundary derivation of magnetic field quantity: According to the above formula, we can ge...
Embodiment 3
[0108] A rail transit vehicle axle counter magnetic field EMC semi-physical simulation method, comprising the following steps:
[0109] S1. Digital simulation: establish a mathematical model in the Simulink environment, and the Maxwell's equations obeyed by the magnetic field around the axle counter are as follows:
[0110]
[0111]
[0112]
[0113]
[0114] Among them: Γ is the field quantity surface, ι is the boundary of Γ, S is the field boundary surface, H is the magnetic field strength, J is the dielectric current density, J s is the density of the external field source current, D is the potential vector, E is the electric field strength, B is the magnetic induction, and ρ is the charge density.
[0115] When the field quantity is continuous, the differential form to obtain its Maxwell equations is as follows:
[0116]
[0117]
[0118]
[0119]
[0120] S2. Boundary derivation of magnetic field quantity: According to the above formula, we can ge...
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