Magnetic Susceptibility and Its Measurement
Gouy, Evans NMR and SQUID methods in principle
Lesson 3298 of 4,500 · Coordination Chemistry: CFT, LFT, Spectra, Magnetism
Learning objectives
- Define molar magnetic susceptibility and its sign
- Compare the physical signals measured by Gouy, Evans NMR and SQUID techniques
Introduction
Counting unpaired electrons predicts a possible moment, but experiment measures a response to a magnetic field. Magnetic susceptibility connects these ideas. It can be measured through mechanical force on a solid, a field-induced NMR frequency difference in solution, or extremely sensitive superconducting detection. Each technique has a different sample requirement and source of error, yet all ultimately probe the same magnetic response of the material.
Core explanation
Magnetisation M is magnetic moment per unit volume. In a simple linear regime, volume susceptibility χ v relates M to applied magnetic field H through M=χ vH. Chemists often use molar susceptibility χ M, which scales the response per mole of complex rather than per unit volume or gram. SI and older cgs conventions use different units and numerical conversion factors; formulas must be used with one declared system. A paramagnetic response has positive susceptibility under the standard sign convention, while diamagnetism contributes a small negative background.
The Gouy method places a sample tube with one end in a strong magnetic field and the other in a weaker region. A field gradient exerts a force proportional to susceptibility under controlled geometry. The apparent weight changes when the field is applied. Paramagnetic material is drawn toward the stronger field; diamagnetic material is pushed away. Careful calibration, sample packing, tube background, field setting and temperature are important. It is a convenient teaching-lab method for bulk solids, but a raw balance difference is not yet a molar moment.
The Evans NMR method is distinct from an Evans magnetic balance. In the NMR version, a paramagnetic solution changes the local magnetic field experienced by a reference nucleus. Comparing reference resonances in the sample environment and a separate reference environment gives a frequency difference from which solution susceptibility can be calculated, using solvent, geometry and concentration corrections. It is attractive when a high-field NMR instrument is available and a compound can be measured in solution. It also helps avoid interpreting a solid-state magnetic phase as if it were the same molecular species in solution.
A superconducting quantum interference device, SQUID, detects extraordinarily small changes in magnetic flux coupled to a superconducting loop. In practical magnetometers, a sample is moved through pickup coils in a controlled field, and the instrument relates the resulting signal to its magnetic moment. SQUID measurements can follow susceptibility over broad temperature and field ranges and are especially valuable for weak moments, spin crossover and magnetic exchange. The sensitivity also makes holder background, trace ferromagnetic contamination, sample mass and alignment consequential.
No method alone identifies the electronic structure. A positive χ can arise from local spins, excited-state thermal population, exchange-coupled ions or impurities. A measured χ M must be corrected for diamagnetic contributions from ligands, counterions and sample holder as appropriate. One must state temperature because paramagnetic susceptibility is temperature-dependent. For solutions, chemical speciation and concentration matter; for solids, crystal packing and intermolecular coupling may matter.
To compare with a spin-only value, one usually converts corrected χ MT into an effective moment using a unit-specific relation. In cgs units a familiar approximation is μ eff(μ B)=2.828√[χ M(cm³ mol⁻¹)T(K)] for an ideal Curie paramagnet after diamagnetic correction. This coefficient cannot be carried unchanged into SI susceptibility units. The next pages examine the temperature law and corrections behind that expression.
Step-by-step reasoning
Choose whether the chemical question concerns a solid or solution and whether temperature dependence is needed. Record mass or concentration, sample composition and measurement temperature. Measure the field response by force, NMR shift or SQUID flux signal; calibrate and subtract holder/solvent background. Convert to molar susceptibility with explicit units, apply chemical diamagnetic correction, and only then compare an effective moment with spin and orbital models.
Visual explanation
Draw three panels. Gouy: a long sample tube straddles strong and weak fields and a balance reads force. Evans NMR: two reference signals in different solution environments are separated by Δf. SQUID: a sample passes through pickup coils linked to a superconducting loop. Beneath all three, draw arrows pointing to χ M(T), the shared chemically useful quantity.
Real-world analogy
One can measure how strongly an object responds to wind by its sideways force, by how it changes a nearby sensor's reading, or by a highly sensitive instrument detecting tiny motion. Gouy, Evans NMR and SQUID likewise observe different physical consequences of the same underlying magnetic response.
Real-world example
A newly prepared Fe²⁺ coordination compound may be tested as a powder by Gouy or SQUID to decide whether its moment is consistent with high spin. If it dissolves without changing identity, Evans NMR can probe the solution state. Agreement across phases is informative; disagreement may reveal ligand exchange, spin-state change or intermolecular coupling in the solid.
Why?
Why is a field gradient needed for a Gouy force? A uniform field can orient magnetic moments but produces no net translational force on a uniformly magnetised sample. The gradient makes one end experience a different field strength, producing a measurable pull or push.
Common misconception
“Evans NMR and an Evans balance are the same instrument.” They share a name but measure different signals: the NMR method uses a reference resonance shift in solution; a balance technique uses mechanical or electromagnetic force compensation.
Worked example
A powder gives positive molar susceptibility after holder subtraction and ligand diamagnetic correction. Its χ MT remains nearly constant from 150 to 300 K. This supports approximately independent paramagnetic centres following a Curie-like law. If a SQUID trace instead shows χ MT falling sharply below 50 K, one should consider antiferromagnetic exchange or zero-field splitting before concluding that the metal's d count changes at low temperature. The measurement gives a response pattern, not a direct electron diagram.
Quick check
1. What primary observable does a Gouy balance use? Answer: The change in force or apparent weight on a sample spanning a magnetic-field gradient when the field is applied.
Exam focus
Define the reported susceptibility and units. Distinguish solid force, solution NMR and superconducting-flux measurements. Mention temperature, blank/holder correction and speciation before turning a positive χ into a number of unpaired electrons.
Advanced insight
All three methods measure a thermodynamic or electromagnetic response of an ensemble. The relation between χ and a single-ion moment is simplest for dilute, independent moments at temperatures high compared with magnetic exchange and zero-field splitting. In concentrated solids or spin-crossover systems, a temperature-resolved model is required.
Summary
Magnetic susceptibility quantifies the field response per volume, mass or mole. Gouy measures force in a gradient, Evans NMR measures a solution reference shift, and SQUID detects tiny flux changes. Correct units, background subtraction and temperature are essential before interpreting electronic structure.
Practice questions
1. Why can a positive measured powder response not be assigned immediately to the compound's unpaired electrons? Answer: The signal may include holder background, impurities or other species and must be converted to molar susceptibility at a known temperature with corrections. 2. What information does a temperature series provide beyond one room-temperature value? Answer: It can reveal Curie-like independent moments, spin crossover, exchange coupling or thermally populated states that one value cannot distinguish. 3. A sample changes ligands on dissolving. Which caution applies to Evans NMR versus powder SQUID results? Answer: They may measure different chemical species and spin states, so a discrepancy is not necessarily instrumental error; verify solution speciation before comparing moments. 4. Which technique is especially suited to highly sensitive temperature-dependent measurements on a small solid sample? Answer: A SQUID magnetometer, provided sample holder and contamination backgrounds are controlled.