THEORY OF THE STRUCTURE OF FERROMAGNETIC DOMAINS

THEORY OF THE STRUCTURE OF FERROMAGNETIC DOMAINS

December, 1946 | CHARLES KITTEL
The paper by Charles Kittel discusses the theory of ferromagnetic domain structures in thin films, small particles, and long needles. The author develops a theory to explain how the domain structure of ferromagnetic materials changes as their dimensions are reduced to sizes comparable to the thickness of Weiss domains found in larger crystals. The key findings include: 1. **Energy Components**: The free energy of a ferromagnetic body is composed of surface energy ($F_w$), magnetic field energy ($F_m$), and anisotropy energy ($F_a$). 2. **Surface Energy ($F_w$)**: This energy is significant for small dimensions and depends on the surface energy density $\sigma_w$. 3. **Magnetic Field Energy ($F_m$)**: This energy is related to the magnetic field arising from the magnetization and is given by $F_m = -\frac{1}{2} J(\mathbf{H} \cdot \mathbf{M}) d V$. 4. **Anisotropy Energy ($F_a$)**: This energy arises from the preferred axes of easy magnetization and is given by $F_a = \rho_a V_a$, where $\rho_a$ is the anisotropy energy density. 5. **Domain Configurations**: - **Films**: The optimal configuration for thin films is a single domain magnetized to saturation in one direction. - **Needles and Wires**: The critical dimension for transition to a saturated configuration is estimated to be around $3 \times 10^{-4}$ cm for films and $2 \times 10^{-4}$ cm for particles or grains. - **Particles**: The critical diameter for small particles is around $1.5 \times 10^{-6}$ cm. 6. **Experimental Results**: The theory predicts that small particles and thin films should exhibit permanent saturation magnetization, high coercive force, and low initial permeability. Experimental results support these predictions, including studies on colloidal suspensions of iron oxides and thin films deposited under weak magnetic fields. 7. **Conclusion**: The study of magnetic behavior in thin films and small particles offers insights into domain theory and can help in selecting materials for permanent magnets. Techniques such as magnetometer measurements, electron diffraction, and magneto-optic studies are recommended to further explore these phenomena. The paper also includes an appendix that derives the magnetic field energy for coplanar strips of alternate sign, supporting the theoretical framework.The paper by Charles Kittel discusses the theory of ferromagnetic domain structures in thin films, small particles, and long needles. The author develops a theory to explain how the domain structure of ferromagnetic materials changes as their dimensions are reduced to sizes comparable to the thickness of Weiss domains found in larger crystals. The key findings include: 1. **Energy Components**: The free energy of a ferromagnetic body is composed of surface energy ($F_w$), magnetic field energy ($F_m$), and anisotropy energy ($F_a$). 2. **Surface Energy ($F_w$)**: This energy is significant for small dimensions and depends on the surface energy density $\sigma_w$. 3. **Magnetic Field Energy ($F_m$)**: This energy is related to the magnetic field arising from the magnetization and is given by $F_m = -\frac{1}{2} J(\mathbf{H} \cdot \mathbf{M}) d V$. 4. **Anisotropy Energy ($F_a$)**: This energy arises from the preferred axes of easy magnetization and is given by $F_a = \rho_a V_a$, where $\rho_a$ is the anisotropy energy density. 5. **Domain Configurations**: - **Films**: The optimal configuration for thin films is a single domain magnetized to saturation in one direction. - **Needles and Wires**: The critical dimension for transition to a saturated configuration is estimated to be around $3 \times 10^{-4}$ cm for films and $2 \times 10^{-4}$ cm for particles or grains. - **Particles**: The critical diameter for small particles is around $1.5 \times 10^{-6}$ cm. 6. **Experimental Results**: The theory predicts that small particles and thin films should exhibit permanent saturation magnetization, high coercive force, and low initial permeability. Experimental results support these predictions, including studies on colloidal suspensions of iron oxides and thin films deposited under weak magnetic fields. 7. **Conclusion**: The study of magnetic behavior in thin films and small particles offers insights into domain theory and can help in selecting materials for permanent magnets. Techniques such as magnetometer measurements, electron diffraction, and magneto-optic studies are recommended to further explore these phenomena. The paper also includes an appendix that derives the magnetic field energy for coplanar strips of alternate sign, supporting the theoretical framework.
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