QCM Advanced Calculator
Quartz Crystal Microbalance — Multi-Model Frequency Analysis
Researcher's Guide & Quick Reference
▼This calculator provides real-time analysis for Quartz Crystal Microbalance (QCM) experiments using three complementary physical models. All input fields update results instantly — no button click required. Hover over the ? icons for contextual explanations of each parameter and result.
Choose the appropriate model tab based on your experimental conditions: Sauerbrey for rigid thin films in air, Kanazawa–Gordon for Newtonian liquid loading, and Voigt–Voinova for viscoelastic films with or without liquid contact. All three models share the same AT-cut quartz constants (ρQ = 2.648 g/cm³, μQ = 2.947 × 10¹¹ g/(cm·s²), ZQ ≈ 8.828 × 10⁵ g/(cm²·s)), displayed at the bottom of each panel for reference.
Use this tab for rigid, acoustically thin films deposited in air (or vacuum). Enter the crystal's resonant frequency f₀, active electrode diameter, observed frequency shift Δf, and film density ρf.
The calculator returns:
- Mass sensitivity Cf — Sauerbrey constant [ng/(Hz·cm²)]
- Mass per Hz — total mass per 1 Hz shift over the active area
- Saturation mass — maximum mass at the 1% Δf/f₀ limit
- Film thickness — in nm, μm and Å
- Total mass change Δm and areal mass Δm/A
Validity criterion: |Δf/f₀| < 1/1000 for reliable results; theoretical Sauerbrey limit ≈ 1/100. Beyond this, the acoustic impedance mismatch between film and quartz causes nonlinear deviations.
Switch between QCM Characterization (sensor properties at a given f₀ and electrode geometry) and Film Measurement (thickness and mass from a measured Δf).
Select this tab when the crystal contacts a semi-infinite Newtonian liquid with no adsorbed film. Two operating modes are available:
- Forward: given liquid density ρL and viscosity ηL, predict Δf, ΔD, ΔΓ and the viscous penetration depth δ.
- Inverse: given a measured Δf, extract the ρL·ηL product. If ρL is known, extract ηL individually.
The Kanazawa signature is |Δf| = ΔΓ, equivalently ΔD·f₀/(2·|Δf|) = 1. Significant deviation from this ratio indicates non-Newtonian behaviour, viscoelastic film presence, or interfacial slip.
Penetration depth δ = √(ηL/(π·f₀·ρL)) defines the liquid layer thickness sensed by the shear wave. In water at 10 MHz, δ ≈ 178 nm.
Use this tab for viscoelastic films — hydrogels, polymer brushes, protein adlayers, lipid bilayers, cell monolayers. Provide the film's density ρf, thickness hf, storage modulus G′, and a loss parameter (either film viscosity ηf or loss modulus G″). Choose between Air and Liquid contact medium.
The calculator predicts:
- Δf — frequency shift (includes both mass and viscoelastic contributions)
- ΔD — dissipation change (energy lost per oscillation cycle)
- ΔD/|Δf| ratio — key diagnostic for regime classification
- |G*| — magnitude of the complex shear modulus
- tan δ — loss tangent (G″/G′), ratio of dissipated to stored energy
- ΔfS — Sauerbrey rigid-film prediction for comparison
A regime assessment automatically classifies the film behaviour:
Limiting cases: G′ → ∞ recovers the Sauerbrey equation; hf → 0 with liquid contact recovers Kanazawa. Use this to verify continuity across models.
- All calculations update automatically with a short debounce delay (280 ms) as you type.
- Negative Δf means mass was added to the crystal; positive Δf means mass was removed or liquid was displaced.
- For QCM-D users: ΔD = 2ΔΓ / f₀, reported in units of 10⁻⁶.
- The Voigt panel includes a Sauerbrey rigid-film comparison (ΔfS), so you can quantify how much viscoelasticity shifts the result.
- Use the loss parameter toggle (ηf ↔ G″) in the Voigt panel for convenience. The calculator auto-converts between the two using G″ = ω·ηf at the fundamental frequency.
- For multi-harmonic analysis, run the Voigt model at each overtone frequency (e.g. 5, 15, 25, 35 MHz for n = 1, 3, 5, 7) and compare Δf/n and ΔDn to diagnose frequency-dependent viscoelastic behaviour.
- Unit conventions: viscosity in mPa·s (= cP), density in g/cm³, frequency in Hz, moduli in Pa. The calculator uses CGS internally (standard for QCM literature) and converts for display.
- Sauerbrey: G. Sauerbrey, "Verwendung von Schwingquarzen zur Wägung dünner Schichten und zur Mikrowägung", Z. Phys. 155, 206–222 (1959).
- Kanazawa–Gordon: K.K. Kanazawa & J.G. Gordon II, "Frequency of a quartz microbalance in contact with liquid", Anal. Chem. 57, 1770–1771 (1985).
- Voigt–Voinova: M.V. Voinova, M. Rodahl, M. Jonson, B. Kasemo, "Viscoelastic acoustic response of layered polymer films at fluid-solid interfaces: Continuum mechanics approach", Phys. Scr. 59, 391–396 (1999).
- Comprehensive review: M. Rodahl, F. Höök, B. Kasemo et al., "Quartz crystal microbalance setup for frequency and Q-factor measurements in gaseous and liquid environments", Rev. Sci. Instrum. 66, 3924 (1995).
- QCM-D technique: M. Rodahl & B. Kasemo, "On the measurement of thin liquid overlayers with the quartz-crystal microbalance", Sens. Actuators A 54, 448–456 (1996).
Cf = √(ρQ·μQ) / (2·f₀²) [g/(Hz·cm²)]
t = −Δf · Cf / ρf
ΔΓ = |Δf| ⟹ ΔD = 2|Δf|/f₀
δ = √(ηL / (π·f₀·ρL))
Validity: Semi-infinite, homogeneous Newtonian liquid, no-slip at interface, no film present. Combined ρ·η characterisation of a liquid from a single Δf measurement.
Z̃load = Z̃f · (Z̃L + Z̃f·tanh ξ̃f) / (Z̃f + Z̃L·tanh ξ̃f)
Z̃f = √(ρf·G̃f) G̃f = G' + iG'' = G' + iωηf
Z̃L = √(iω·ρL·ηL) [0 in air]
ξ̃f = ω·hf·√(ρf/G̃f)
ΔD = 2ΔΓ/f₀
High ΔD/|Δf| ratio indicates strong viscoelastic losses. Typical threshold: ΔD/|Δf| > 0.2×10⁻⁶/Hz signals Sauerbrey breakdown.