The Biot-Savart law enables the calculation of the magnetic field created by electric currents. It's a universal law applicable to various current configurations. Essentially, it says that a very small segment of a current-carrying wire generates a magnetic flux density at a certain distance away. This concept is fundamental in understanding how electric currents produce magnetic fields.
The law states that an infinitesimally small current-carrying path produces magnetic flux density at a distance r:
Where is the vacuum permeability and is the unit vector in the direction of the distance. In symmetric problems, it is possible to simplify the analysis and obtain a closed form solution. The field on the axis of a current carrying loop can be easily computed using the Biot-Savart law, due to the fact that only axis component of the vector contributes to the resultant field intensity (Fig. 1):
The total flux density at a point on the centerline at a distance z is found by integrating the expression for over the circumference of the loop:
For a current and loop radius , the axial magnetic field is .
In a simulation using EMS, a thin toroid with a 5mm cross-sectional radius and a 100mm loop radius is modeled in a Magnetostatic study. Copper is used as the material for the toroid, while the remainder of the assembly is air. For precise magnetic field measurements, it's crucial to create a sufficiently large air domain.
For guidance on assigning materials in EMS, refer to the example “Computing capacitance of a multi-material capacitor.” Additionally, the “Electric field inside the cavity of a charged sphere” example provides insights into defining the air domain in EMS.
To apply the EMS Coil feature to the Toroid, access to its cross-sectional surface is needed. Therefore, the procedure involves splitting the Toroid into two separate bodies. This step is essential for the proper application of the feature in the simulation process. For detailed instructions on how to split the Toroid part, you can refer to the source for more comprehensive guidance.
In the EMS feature tree, Right-click on the Coilsfolder, select Solid Coil .
Click inside the Components or Bodies for Coils box .
Click on the (+) sign in the upper left corner of the graphics area to open the components tree.
Click on the Toroid icon. It will appear in the Components and Solid Bodies list.
Click inside the Faces for Entry Port box then select the entry port face.
In the Exit Port Tab, Check “Same as Entry Port“. (Figure 3)
General Properties:
To be able to display the variation of the magnetic field along the axis of the Toroid, before running the simulation:
Once the simulation is complete:
The comparison of the theoretical and EMS calculated magnetic flux density along the toroid's axis is shown in Figure 4, where both results display a high level of agreement. This illustrates the accuracy and reliability of the EMS simulation in replicating theoretical predictions for magnetic flux density in this context. For a detailed view and further analysis, you can refer to the original source.
Figure 4 - Comparison of EMS and theoretical results for magnetic flux density along the axis of a toroid
Figure 5 - Section plot of the magnetic flux density
Conclusion
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