Maxwell 15.01之缺陷【轉(zhuǎn)發(fā)】

2017-06-27  by:CAE仿真在線  來源:互聯(lián)網(wǎng)

DE28651 In 2D magnetostatic when using a demagnetization link, the mesh
in the source design and target designs must be identical. However, if you
have added mesh operations or additional adaptive passes in the target design
the software will enforce them causing the meshes to be different. There is
currently no error message, but postprocessing solutions in the target design
will fail (calculations may fail to evaluate and plots will show no fields).

使用退磁計算時(2D靜態(tài)場),網(wǎng)格導入必須要完全相同。因此,在target design中設(shè)置要注意。

DE32794 - In 2D transient using dynamic demagnetization should not be used
in a design that is also using the advanced setting consider core loss
effect on field. Results are unreasonable if you attempt to combine these
2 functions.

動態(tài)退磁(2D瞬態(tài)場)功能與考慮鐵耗影響功能不能聯(lián)合使用。期待版本升級

DE33012 - In 2D transient models that do not have any windings defined,
current density output to the postprocessor is incorrect. You can add a
dummy winding to work around.

沒有繞組定義的2D瞬態(tài)場模型,進入后處理器中的電流密度是錯誤的。因此,
要添加一個虛擬繞組。

DE32768 - In 2D transient RZ models force calculations are incorrect in
passive conducting objects with eddy effects activated.

2D瞬態(tài)場RZ模型中,則渦流引起的力計算錯誤。

DE34048 - In 3D transient when using the advanced feature "Dynamic
demagnetization distribution", if a magnet is fully demagnetized and operating
in the 4th quadrant with very high field levels, the B and H field values
passed to the post-processor are not quite correct and would show points
on the extension of the BH curve instead of the expected location on a straight
line with Hc=0. This is a post-processing issue only, the solver is using the
correct values and field solutions are otherwise correct.
3D瞬態(tài)場中,使用動態(tài)退磁分布時,在第4象限中,后處理有誤。

DE29212 and DE34138 In 2D transient RZ designs, solid losses are incorrect
in some cases due to an error in eddy current calculations.
2D瞬態(tài)場RZ模型中,solid losses在一些渦流計算中不正確。


DE33891 and DE34082 In 3D transient with rotational motion, when using a
magnet in the rotating part of the geometry that was defined using a
cylindrical coordinate system, vector plots of the fields will not show
correctly as the magnet rotates position. This is a post processing issue
only, the field solutions are correct in the solver and other quantities
(such as torque) are correct. You can avoid this issue by defining the
magnet using a Cartesian coordinate system.
3D瞬態(tài)場旋轉(zhuǎn)運動時,使用直角坐標系定義永磁體方向較好。

In Maxwell 2D transient when working with demagnetization and temperature
dependence, the temperature dependence only takes effect if the radio button
in the BH entry dialog for the material is set to Intrinsic before leaving
the dialog. If you have Normal selected then the thermal modifier will be
ignored. Conversely, if you are not interested in temperature dependence you
should convert to the Normal curve before you leave the BH entry dialog.
In either case, you can enter the data in whichever form you like, but you
must convert to Intrinsic for temperature dependence, or Normal for all other
cases.
2D瞬態(tài)計算退磁和溫度依賴時,注意選擇相關(guān)的選項。

In 2D transient, dynamic demagnetization of nonlinear magnets with conductivity
and eddy effect turned on in the magnets, cannot be combined with coreloss
calculation with the advanced consider coreloss effect on field setting turned
on and with eddy effects enabled in the winding. This combination produces
incorrect results. The same combination will work if consider coreloss effect on
field is turned off.
2D瞬態(tài)場中,非線性永磁體的動態(tài)退磁計算時(渦流開),不能與考慮鐵耗計算、繞組中的渦流效果
聯(lián)合使用。

轉(zhuǎn)自:http://blog.sina.com.cn/s/blog_4f850b690100ziwe.html

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