Curie's Law Calculator

Enter a material's Curie constant, temperature, and applied magnetic field to find its magnetic susceptibility (χ = C / T), field intensity, magnetization, and relative permeability.

Quick Facts

Curie's law
χ = C / T
Magnetic susceptibility falls as absolute temperature rises.
Relative permeability
μr = 1 + χ
Stays very close to 1 for paramagnets, since χ is tiny.
Where it applies
Dilute paramagnets, weak fields
Breaks down near saturation or a magnetic ordering transition — see the Curie-Weiss law.

Your Results

Calculated
Magnetic Susceptibility (χ)
-
χ = C / T, dimensionless
Field Intensity (H)
-
H = B / μ₀, in A/m
Magnetization (M)
-
M = χ × H, in A/m
Relative Permeability (μr)
-
μr = 1 + χ

Ready

Enter the Curie constant, temperature, and applied field, then press Calculate.

About Curie's Law

Curie's law, discovered by French physicist Pierre Curie in 1895, describes how the magnetic response of a paramagnetic material weakens as temperature rises. It states that the volume magnetic susceptibility χ is directly proportional to a material-specific Curie constant C and inversely proportional to the absolute temperature T: χ = C / T. This calculator uses that relationship to find χ, then combines it with an applied field B to find the field intensity H = B / μ₀, the magnetization M = χ × H, and the relative permeability μr = 1 + χ (μ₀ = 4π × 10⁻⁷ T·m/A is the permeability of free space).

Where the formula comes from

In a paramagnetic material, each atom or ion carries a small permanent magnetic moment that points in a random direction because of thermal agitation. Applying an external field B creates a torque that favors alignment with the field, while thermal energy (proportional to kBT) keeps randomizing the orientations. When the magnetic energy per moment is much smaller than the thermal energy — the normal situation for weak-to-moderate lab fields at room temperature — statistical mechanics shows the average magnetization grows linearly with B and falls off as 1/T. Bundling the moment density, the Landé g-factor, the total angular momentum quantum number J, the Bohr magneton, and Boltzmann's constant into one material constant C reproduces χ = C / T.

When Curie's law applies — and when it doesn't

Curie's law is a good approximation for dilute paramagnets (moments far enough apart that they barely interact) at temperatures well above any magnetic ordering transition, and in fields too weak to noticeably align the moments. It breaks down at very low temperature or very high field, where the moments approach full alignment and the magnetization saturates instead of continuing to grow linearly. It also breaks down in materials where neighboring moments interact strongly: those instead follow the Curie-Weiss law, χ = C / (T − θ), where the constant θ shifts the temperature axis to reflect the interactions (θ = 0 recovers pure Curie behavior).

Frequently Asked Questions

What is the Curie constant?
The Curie constant C is a material-specific value (in kelvin) that sets how strongly a paramagnetic substance responds to a magnetic field. Microscopically, C = μ₀ N g² J(J+1) μB² / (3 kB), where N is the number density of magnetic moments, g is the Landé g-factor, J is the total angular momentum quantum number, μB is the Bohr magneton, and kB is Boltzmann's constant. A larger C means a stronger susceptibility at a given temperature.
What is the difference between Curie's law and the Curie-Weiss law?
Curie's law, χ = C / T, assumes the magnetic moments do not interact with each other. The Curie-Weiss law, χ = C / (T − θ), adds a correction temperature θ that accounts for interactions between neighboring moments; θ = 0 reduces it back to pure Curie's law, θ > 0 signals ferromagnetic-like coupling, and θ < 0 signals antiferromagnetic-like coupling.
Does Curie's law apply to ferromagnetic materials?
Not directly. Below its Curie temperature, a ferromagnet has spontaneous magnetization that does not follow χ = C / T. Above the Curie temperature, ferromagnets become paramagnetic and their susceptibility follows the Curie-Weiss law, χ = C / (T − Tc), where Tc is the Curie temperature.
Why is magnetic susceptibility dimensionless in SI units?
Volume magnetic susceptibility is defined as χ = M / H, the ratio of magnetization to applied field intensity. Both M and H are measured in amperes per meter (A/m) in SI, so their ratio has no units — which is why the Curie constant C carries units of kelvin, to cancel the kelvin in T so χ comes out dimensionless.