Calculate the Curie constant, paramagnetic susceptibility, and Weiss molecular field for ferromagnetic and paramagnetic materials.
The Curie constant is a fundamental quantity in magnetism that characterizes how strongly a material responds to an external magnetic field as a function of temperature. Named after Pierre Curie, who discovered the relationship between susceptibility and temperature in paramagnetic materials, the Curie constant appears in both the Curie law and the Curie–Weiss law.
For paramagnetic materials above the Curie temperature, the magnetic susceptibility follows the Curie–Weiss law: χ = C / (T − Tc), where C is the Curie constant and Tc is the Curie temperature. Below Tc, the material transitions to a ferromagnetic state with spontaneous magnetization. The Curie constant depends on the angular momentum quantum number, the number density of magnetic atoms, and fundamental constants.
This calculator determines the Curie constant for any magnetic material from its quantum mechanical properties, computes the paramagnetic susceptibility at any temperature, and provides reference data for common ferromagnetic elements like iron, nickel, cobalt, and gadolinium.
The Curie constant is useful whenever you need to estimate how strongly a magnetic material will respond to temperature and field changes. Students use it to connect the Curie law to the Curie–Weiss form, while researchers use it to compare measured susceptibility against a quantum model.
This calculator is most helpful when you want to move from the material parameters to a practical susceptibility estimate without doing the algebra by hand.
Curie constant: C = μ₀ × N × g² × μ_B² × J(J+1) / (3 × k_B) Curie–Weiss susceptibility: χ = C / (T − Tc) Effective moment: p_eff = g × √(J(J+1)) (in Bohr magnetons) Where μ₀ = vacuum permeability, N = atomic density, g = Landé g-factor, μ_B = Bohr magneton, k_B = Boltzmann constant.
Result: Curie constant ≈ 7.21, χ ≈ 0.1265
For iron (J = 2.22, Tc = 1043 K) at 1100 K, the Curie constant is approximately 7.21 and the Curie–Weiss susceptibility is about 0.1265, indicating the paramagnetic regime just above the Curie temperature.
The Curie constant sits at the center of the Curie and Curie–Weiss descriptions of magnetic susceptibility. It links the microscopic magnetic moment of the ions to the macroscopic response you measure in the lab.
For temperatures above the Curie point, a positive Curie constant and a positive susceptibility indicate paramagnetic behavior. Near the transition, the Curie–Weiss model becomes a quick way to compare the measured response with the expected trend.
This is most useful when fitting susceptibility data, comparing materials, or checking whether a measured response is consistent with a claimed magnetic phase.
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The Curie constant C characterizes the strength of paramagnetic response. It depends on the number of magnetic atoms, their angular momentum, and fundamental constants. Larger C means stronger magnetic response.
At the Curie temperature Tc, a ferromagnetic material transitions to a paramagnetic state. Below Tc, atomic moments are spontaneously aligned; above Tc, thermal energy disrupts alignment and susceptibility follows the Curie–Weiss law.
The Curie law (χ = C/T) applies to ideal paramagnets with no interactions. The Curie–Weiss law (χ = C/(T−Tc)) accounts for exchange interactions between magnetic moments through the Curie temperature Tc.
As T approaches Tc from above, the denominator (T − Tc) approaches zero, causing χ to diverge. This signals the onset of the ferromagnetic phase transition where long-range magnetic order emerges.
The effective moment p_eff = g√(J(J+1)) represents the observed magnetic moment per atom in units of Bohr magnetons. It can be measured experimentally from susceptibility data and compared with quantum predictions.
Antiferromagnets follow a modified Curie–Weiss law with a negative Tc (Néel temperature). You can enter a negative Curie temperature to model antiferromagnetic susceptibility above the ordering temperature.