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- Finite element meshes and grain distribution of hex_Ia1
- Cut planes of the easy axes, remanent, and coercive state plots of
hex_I
- Easy axes of hex_Ia1
- Easy axes of hex_Ia2
- Easy axes of hex_Ia3
- Finite element meshes and grain distribution of hex_H
- Cut planes of the easy axes, remanent, and coercive state plots of
hex_H
- Easy axes of hex_H
- FE mesh and cut planes of hex_T
- Easy axes of hex_T
- Demagnetization curves
- Comparison of hex_Ia1m2, hex_Ia2, and hex_Ia3
- Comparison of hex_Hm2, hex_Ia2, and hex_Ia3
- Comparison of hex_Ia1m2, hex_Hm2, and hex_T
- Color code for magnetization direction
- Magnetization distribution of hex_Ia1m1 in remanent state
- Magnetization distribution of hex_Ia1m2 in remanent state
- Magnetization distribution of hex_Ia2 in remanent state
- Magnetization distribution of hex_Ia3 in remanent state
- Magnetization distribution of hex_Hm1 in remanent state
- Magnetization distribution of hex_Hm2 in remanent state
- Magnetization distribution of hex_T in remanent state
- Color code for magnetization direction
- Magnetization distribution of hex_Ia1m1 in demagnetized state
- Magnetization distribution of hex_Ia1m2 in demagnetized state
- Magnetization distribution of hex_Ia2 in demagnetized state
- Magnetization distribution of hex_Ia3 in demagnetized state
- Magnetization distribution of hex_Hm1 in demagnetized state
- Magnetization distribution of hex_Hm2 in demagnetized state
- Magnetization distribution of hex_T in demagnetized state
- Simulation data of hex_Ia1m1
- Simulation data of hex_Ia1m2
- Simulation data of hex_Ia2
- Simulation data of hex_Ia3
- Simulation data of hex_Hm1
- Simulation data of hex_Hm2
- Simulation data of hex_T
The names of the simulations have the following structure: All names start with hex_. The next letter indicates the configuration of the particles. I stands for a single particle, whose long axis is parallel to the external field (cf. fig. 1). H stands for two parallel particles, whose long axes are parallel to the external field (cf. fig. 6). T stands for two particles, whose long axes are perpendicular to each other (cf. fig. 9). The next letter can be an a, which is followed by a number. It indicates the distribution of easy axes. Configurations with different anisotropy have been calculated only for a single particle. Finally, the letter m and a succeding number characterize the finite element mesh, which has been used in the calculations.
The following tables give an overview of all simulations and the figure in this report.
Table 1:
Figures of the simulated particles
Sim. |
Simulation |
FE mesh, |
Easy axes |
Remanent |
Demagnetized |
# |
name |
grains |
|
state |
state |
1 |
hex_Ia1m1 |
1 |
3 |
16 |
24 |
2 |
hex_Ia1m2 |
1 |
3 |
17 |
25 |
3 |
hex_Ia2 |
1 |
4 |
18 |
26 |
4 |
hex_Ia3 |
1 |
5 |
19 |
27 |
5 |
hex_Hm1 |
6 |
8 |
20 |
28 |
6 |
hex_Hm2 |
6 |
8 |
21 |
29 |
7 |
hex_T |
9 |
10 |
22 |
30 |
Table 2:
Graphs and data of the simulation results
Sim. |
Simulation |
Simulation |
Hysteresis |
# |
name |
data |
|
1 |
hex_Ia1m1 |
31 |
11 |
2 |
hex_Ia1m2 |
32 |
11 |
3 |
hex_Ia2 |
33 |
11 |
4 |
hex_Ia3 |
34 |
11 |
5 |
hex_Hm1 |
35 |
11 |
6 |
hex_Hm2 |
36 |
11 |
7 |
hex_T |
37 |
11 |
Next: List of Tables
Up: Micromagnetic Simulation of Bonded
Previous: Contents
Werner Scholz
1/30/1999