Definition and Overview
Basic Concept
Hysteresis: lagging response of magnetization (M) in ferromagnetic materials to applied magnetic field (H). Magnetic flux density (B) does not retrace same path when H varies cyclically. Nonlinear, path-dependent behavior.
Historical Context
Term introduced by Sir James Alfred Ewing, 1881. Early studies on iron and steel magnetic properties. Foundation for magnetic materials science and electrical engineering.
Physical Origin
Arises from domain wall motion, magnetic domain rotation, and energy barriers. Intrinsic material defects and microstructure cause irreversible magnetization changes.
"Hysteresis is the memory effect of magnetic materials, crucial for permanent magnetism and transformer design." -- C.P. Bean
Magnetization Process
Initial Magnetization Curve
Starting from demagnetized state, magnetization increases with H, domains align, walls move. Curve nonlinear, saturates at high H (saturation magnetization, Ms).
Domain Wall Movement
Primary mechanism at low fields. Domain walls shift to increase aligned domains. Impeded by defects, inclusions, grain boundaries.
Rotation of Magnetic Moments
At higher fields, domain rotation dominates. Magnetic moments rotate towards field direction overcoming anisotropy energy barriers.
B-H Curve Characteristics
Definition
B-H curve: plot of magnetic flux density (B) versus magnetic field strength (H). Illustrates magnetization and hysteresis behavior.
Hysteresis Loop
Closed loop formed during cyclic magnetization. Area proportional to energy loss per cycle. Key parameters: coercivity (Hc), remanence (Br), saturation (Bs).
Saturation
Maximum B reached when all domains fully aligned. Further increase in H produces negligible B change.
| Parameter | Symbol | Description |
|---|---|---|
| Coercive Force | Hc | Field needed to reduce B to zero after saturation |
| Remanent Magnetization | Br | Residual magnetization at zero field |
| Saturation Magnetization | Bs | Maximum magnetization achievable |
Magnetic Domains and Microstructure
Domain Concept
Ferromagnetic materials subdivided into domains with uniform magnetization. Minimize total magnetic energy by reducing stray fields.
Domain Wall Types
Bloch walls: magnetization rotates perpendicular to wall. Néel walls: magnetization rotates within plane. Wall type affects hysteresis properties.
Influence of Microstructure
Grain size, impurities, dislocations affect domain wall mobility. Fine grains increase coercivity; annealing reduces defects, lowers hysteresis loss.
Coercivity and Retentivity
Coercivity (Hc)
Magnetic field intensity required to reduce net magnetization to zero after saturation. Indicator of material's resistance to demagnetization.
Retentivity or Remanence (Br)
Residual magnetization after external field removed. Determines permanent magnet strength.
Classification by Coercivity
Soft magnetic materials: low Hc, used in transformers. Hard magnetic materials: high Hc, used in permanent magnets.
Energy Loss and Hysteresis Loop Area
Energy Dissipation
Energy loss per magnetization cycle equals area enclosed by hysteresis loop. Manifests as heat.
Quantitative Expression
Energy loss density (W) per cycle:
W = ∮ H dBIntegral of H over B for closed loop path.
Impact on Devices
Core loss in transformers, inductors. Minimizing hysteresis loss improves efficiency and reduces heating.
| Material Type | Typical Coercivity (A/m) | Hysteresis Loss (J/m³ per cycle) |
|---|---|---|
| Soft Iron | 50 - 200 | Low |
| Silicon Steel | 100 - 400 | Moderate |
| Hard Ferrite | >1000 | High |
Types of Hysteresis
Magnetic Hysteresis
Classic lag of B behind H in ferromagnets. Exhibits irreversible domain processes.
Ferroelectric Hysteresis
Analogous behavior in ferroelectric materials with polarization versus electric field.
Other Forms
Mechanical hysteresis: stress-strain lag in ferromagnetic alloys. Thermal hysteresis: temperature-dependent magnetization lag.
Mathematical Models
Preisach Model
Phenomenological model representing hysteresis as superposition of elementary rectangular loops. Widely used for simulation.
Jiles-Atherton Model
Physical model based on domain wall motion and pinning. Parameters relate to material microstructure.
Mathematical Expression
dM/dH = (M_eq - M)/ (kδ) - c dM/dHwhere:M = magnetization,M_eq = equilibrium magnetization,k = pinning coefficient,c = reversibility coefficient,δ = direction of field change (+1 or -1) Applications of Hysteresis
Transformers and Inductors
Soft magnetic cores designed to minimize hysteresis loss, improve efficiency in power devices.
Permanent Magnets
Utilize high coercivity materials to retain magnetization for motors, sensors, data storage.
Magnetic Recording
Hysteresis enables data encoding via remanent magnetization states in recording media.
Magnetic Sensors
Exploitation of hysteresis properties in switches, memory elements, and spintronic devices.
Measurement Techniques
Vibrating Sample Magnetometer (VSM)
Measures magnetic moment by vibrating sample in uniform field. High sensitivity, dynamic measurement.
B-H Loop Tracer
Direct plotting of B-H curves using electronic circuits, useful in material characterization.
Magneto-Optical Kerr Effect (MOKE)
Optical technique detecting surface magnetization changes during hysteresis cycles.
Temperature Effects
Curie Temperature
Above critical temperature, ferromagnetism disappears; hysteresis vanishes.
Temperature Dependence of Coercivity
Hc decreases with rising temperature due to thermal agitation reducing anisotropy energy.
Thermal Activation of Domain Walls
Thermally assisted domain wall motion causes variation in hysteresis loop shape and area.
Recent Research and Developments
Nanostructured Magnetic Materials
Engineering domain sizes and boundaries at nanoscale to tailor hysteresis for improved performance.
Magnetocaloric Effect and Hysteresis
Studies on low hysteresis materials enhancing magnetic refrigeration efficiency.
Spintronics and Hysteresis Control
Manipulation of hysteresis loops via spin currents, enabling energy-efficient memory devices.
Advanced Modeling Techniques
Machine learning approaches to predict hysteresis behavior from microstructural data.
References
- Cullity, B.D., Graham, C.D., Introduction to Magnetic Materials, Wiley-IEEE Press, 2008, pp. 101-145.
- Jiles, D.C., Introduction to Magnetism and Magnetic Materials, 2nd ed., CRC Press, 1998, pp. 200-230.
- Preisach, F., Über die magnetische Nachwirkung, Zeitschrift für Physik, vol. 94, 1935, pp. 277-302.
- Chikazumi, S., Physics of Ferromagnetism, 2nd ed., Oxford University Press, 1997, pp. 320-370.
- Jiles, D.C., Atherton, D.L., Theory of ferromagnetic hysteresis, Journal of Magnetism and Magnetic Materials, vol. 61, 1986, pp. 48-60.