Wall Sound Insulation Calculator: Mass Law, Double Walls & Leaks

Estimate wall transmission loss, mass–air–mass resonance, coincidence dips and the effect of openings. Compare single and separated double leaves with approximate STC/Rw ratings.

#air leaks #double walls #mass law #Rw #STC

This wall sound insulation calculator helps home-studio builders, acoustic consultants, engineers and students explore why a partition stops some frequencies better than others. It combines mass law sound insulation, a separated double-wall approximation, coincidence losses and a simple opening model. Use it to compare design ideas and identify weak frequency ranges before selecting a tested assembly.

Choose a single leaf or a separated double leaf with an absorbent cavity. Enter each leaf's effective density and total material thickness. Their product gives surface mass, the total kilograms per square metre of that side. For a known surface mass, divide it by thickness to obtain the effective density. The inputs convert with the metric/US switch. Several sheets fastened together on one side form one leaf. Enter the effective critical frequency and loss factor from material measurements when available. A generic gypsum-board assumption is provided to make the physics easy to explore; it does not identify a particular board product.

For a double wall, enter the full distance between the inner leaf faces. This includes the depths of both independent stud frames and any space between them. Fibrous absorption occupies part of that cavity; its thickness is not subtracted. The model assumes that absorption is present and that the two leaves have no rigid bridges. Its air-spring loss factor is a sensitivity assumption near resonance, not a specification for a mineral-wool or glass-fibre product.

Enter the gross wall area and the total equivalent open area. A gap's area is its width multiplied by its length. The calculator treats an opening as an unobstructed bypass through the whole assembly. It adds transmitted powers, rather than averaging decibels. Even a small opening can set the high-frequency ceiling, so compare the sealed curve with the curve including the opening.

The transmission-loss chart shows the mass–air–mass dip, the improvement above resonance and the coincidence region of each leaf. A separate opening-area sweep shows the benefit of closing leaks at the inspection frequency. The third-octave table supplies approximate band values used by the wall STC calculator and Rw estimator. STC covers 125–4000 Hz; Rw covers 100–3150 Hz. Neither number describes deep bass adequately: inspect the low-frequency curve for music, drums and machinery.

The fixed NRC comparison uses published laboratory measurements, independently of your inputs. It reveals the limits of the simplified model instead of implying a universal prediction accuracy. Real walls also depend on supports, workmanship, absorption distribution and surrounding rooms. Shared studs, resilient-channel systems, flanking transmission, empty cavities, doors, ducts, triple leaves and thick masonry need a different model or measured data.

These results are estimates, not laboratory ratings, compliance evidence or a prediction of the sound level in the next room. Use tested assembly reports for specification and check against the standard in force. Installation work belongs to a qualified person, including the treatment of penetrations and required fire protection.

How it is calculated

Surface mass is calculated as m=ρleaftm=\rho_{leaf}t, using the effective density and summed material thickness of each leaf. Density and thickness convert with the metric/US switch; frequency is unchanged. The schematic and sensitivity chart explicitly retain SI labels.

Single leaf

Use SI numerical values in Sharp's field-incidence mass law, RM=20log⁡10(πfm/Z0)−5R_M=20\log_{10}(\pi fm/Z_0)-5, with Z0=411.6Z_0=411.6 Pa·s/m. Below fc/2f_c/2, this is the leaf estimate. At and above coincidence use Rc=20log⁡10(πfm/Z0)+10log⁡10(2ηf/(πfc))R_c=20\log_{10}(\pi fm/Z_0)+10\log_{10}(2\eta f/(\pi f_c)). Interpolate in dB against log frequency between the two endpoints at fc/2f_c/2 and fcf_c. Clip TL to zero to preserve passivity. See the attached AAS 2015 paper, PDF p.3, Eqs.4 and 6. The printed sign in Ballagh's Eq.2 is inconsistent with damping physics; this calculator uses the positive damping contribution in the AAS equation: more damping raises coincidence TL.

Separated double leaf

Air stiffness per area is Ka=ρ0c02/dK_a=\rho_0c_0^2/d, and f0=Ka(1/m1+1/m2)/(2π)f_0=\sqrt{K_a(1/m_1+1/m_2)}/(2\pi). Sharp's absorbent-cavity asymptotes are R1+R2+20log⁡10(fd)−29R_1+R_2+20\log_{10}(fd)-29 below the cavity transition and R1+R2+6R_1+R_2+6 above it; the transition is approximately 55/d55/d Hz. These are the equations reproduced and experimentally assessed by Ballagh (2004), PDF p.2. Critical-frequency effects are included in both leaf terms.

Sharp's asymptotes do not resolve the resonance dip. Here a derived extension, not Sharp's original model, supplies it. For each frequency form zj=iωmjz_j=i\omega m_j and Y=iωd/[ρ0c02(1+iηa)]Y=i\omega d/[\rho_0c_0^2(1+i\eta_a)]. Multiplication of the series-mass, shunt-compliance and series-mass transfer matrices gives the loaded pressure denominator

D=2+Y(z1+z2)+(z1+z2+z1Yz2)/Z0+YZ0.D=2+Y(z_1+z_2)+(z_1+z_2+z_1Yz_2)/Z_0+YZ_0.

Use max⁡(0,20log⁡10∣D/2∣−5)\max(0,20\log_{10}|D/2|-5) below f0f_0. The subtraction of 5 dB is an approximate field correction. Between f0f_0 and 2f02f_0, blend its transmitted power into the Sharp estimate using u=log⁡2(f/f0)u=\log_2(f/f_0) and w=u2(3−2u)w=u^2(3-2u); use Sharp alone above 2f02f_0. This numerical transition and the default cavity damping are screening assumptions. Inputs that overlap the resonance, cavity-transition or coincidence regimes are rejected.

Openings, bands and ratings

For open fraction a=Aopen/Aa=A_{open}/A, R=−10log⁡10[(1−a)10−Rwall/10+a]R=-10\log_{10}[(1-a)10^{-R_{wall}/10}+a]. This follows conservation of transmitted power; ASHRAE 2025 Fundamentals, Ch.8 Eq.41. The opening-only ceiling is −10log⁡10a-10\log_{10}a. Nine log-frequency midpoint samples approximate each third-octave band's mean transmitted power, assuming equal incident energy per logarithmic frequency interval.

Before fitting, round the band values within the shared rating function: to the nearest integer dB for STC (ASTM E413-22 §5.2), and to the nearest 0.1 dB for Rw (ISO 717-1:2020 §4.4, printed p.4 / attached preview p.10). Accumulate deficits in integer dB or integer tenths of a dB so numerical roundoff cannot alter the 32 dB limit. This rounding applies to modeled and measured band inputs, not only their displayed precision.

Fit the highest integer contour: ASTM E413-22 STC uses 125–4000 Hz, a total deficit no greater than 32 dB and an individual deficit no greater than 8 dB. ISO 717-1:2020 Rw uses 100–3150 Hz and the 32 dB total rule. Both are evaluated at 500 Hz. Functional contour descriptions implement the method without reproducing standard tables or figures. These are estimates from modeled bands, not standard-compliant measurements; check against the standard in force.

Assumptions

  • Fixed air properties: density 1.2 kg/m³ and sound speed 343 m/s, representative of room-temperature air. Empirical function arguments are normalized to Hz, kg/m² and metres before evaluation.
  • Broad, thin, effectively homogeneous leaves. Surface mass and effective critical frequency are independent user data; no automatic stiffness model for bonded laminates or multilayer boards is assumed.
  • Double leaves have separate supports, fibrous cavity absorption, sealed perimeters except the entered opening, and no structural bridges or flanking paths. Absorber flow resistivity and fill distribution are not modeled.
  • The default 800 kg/m³ and 12.5 mm per leaf give 10 kg/m². This matches the surface masses in NRC TL-93-279; the 205 mm cavity also follows that test. The default density/thickness pair is an illustrative way to enter the mass, not a material specification. The 3000 Hz critical frequency, 0.03 leaf loss and 0.15 air-spring loss are illustrative assumptions, not measured properties of that specimen.
  • The lumped resonance extension and power interpolation are derived here. The dip's depth is particularly uncertain. This is a static frequency-domain sizing tool; no animation is needed.

Where it applies

Use for preliminary comparisons over 50–5000 Hz with the stated separated-leaf assumptions. The band calculations extend slightly past the plotted limits to integrate the end bands. This is an estimate, not a lab rating.

NRC IR-761 provides independent checks, not fitted coefficients. For TL-93-279 (printed p.316, attached PDF p.319), the default sealed model gives STC 52 versus measured 53, and about 59.1 dB at the 500 Hz band versus 60.0 dB measured. Across 125–2000 Hz the largest band discrepancy is approximately 3 dB. Across the complete plotted range, error approaches 14 dB near resonance, and approximately 9 dB near coincidence. The fixed comparison chart shows these differences. For TL-93-262 (printed p.330, PDF p.333), 11.6/11.4 kg/m² leaves and 205 mm depth give approximately STC 54 versus measured 58 using an assumed 2500 Hz critical frequency. Reference-case tolerances of 3–5 dB are limited screening checks at specified points; they are not a universal accuracy claim.

No prediction of room-to-room level difference, reverberation, flanking, shared studs, resilient mounts, empty cavities, absorber-product performance, slit diffraction, duct resonances, triple leaves, heavy masonry shear waves or fire resistance. Do not use the open-area model as a ventilation or narrow-crack acoustic design method.

STC/Rw fitting follows ASTM E413-22 and ISO 717-1:2020 respectively; standards and scope checked on 29 October 2026. Obtain measured assembly ratings for specifications and check against the standard in force. Installation work belongs to a qualified person.

References

  • B. H. Sharp (1978), Prediction Methods for the Sound Transmission of Building Elements, Noise Control Engineering 11(2), 53–63. https://doi.org/10.3397/1.2832099
  • K. O. Ballagh (2004), Accuracy of Prediction Methods for Sound Transmission Loss, Inter-Noise 2004, pp.2–3. https://static1.squarespace.com/static/62b943270a6d6d4fa1970dee/t/66862bbb9374252e7a84f6d9/1720069056129/10_accuracy_of_prediction_methods_for_sound_transmission_loss.pdf
  • AAS Acoustics 2015 paper p74, Sound insulation of vacuum insulated glazing, PDF p.3, Sharp single-leaf equations. https://acoustics.asn.au/conference_proceedings/AAS2015/papers/p74.pdf
  • R. E. Halliwell et al. (1998), Gypsum Board Walls: Transmission Loss Data, NRC IRC-IR-761, printed pp.17, 316 and 330. https://doi.org/10.4224/20331556
  • ASHRAE Handbook—Fundamentals (2025), Chapter 8, Eq.41 and the 40 dB wall/1% opening example. https://handbook.ashrae.org/Handbooks/F25/IP/F25_Ch08/F25_Ch08_ip.aspx
  • ASTM E413-22, Classification for Rating Sound Insulation, §5.2 band rounding and contour-fitting procedure. https://store.astm.org/e0413-22.html
  • ISO 717-1:2020, Acoustics—Rating of sound insulation, Part 1, §4.4 band rounding before comparison (printed p.4). https://cdn.standards.iteh.ai/samples/77435/7e658360f54d4ddc9e6f23c0a1e7d41e/ISO-717-1-2020.pdf

Inputs

InputSymbolUnitDefault
Wall model
Double leaf assumes independent frames with no rigid bridges and fibrous cavity absorption. Shared studs, empty cavities and triple leaves are outside this model.
constructionSeparated double leaf, absorbent cavity
Leaf 1 effective density
Mass divided by solid leaf volume. With known surface mass m and total thickness t, use density = m/t. For example, 10 kg/m² over 12.5 mm means 800 kg/m³. This is an editable scenario, not a material catalogue.
rho_1kg/m^3800
Leaf 1 total material thickness
Sum of material thicknesses in this leaf. Surface mass = effective density × total thickness. The effective critical frequency remains a separate input, especially for layered or bonded leaves.
t_1mm12.5
Leaf 1 critical frequency
Lowest coincidence frequency, from measured material data or plate theory. Around 3 kHz is a scenario for 13 mm gypsum, not a certified material property. Laminated layers need their own effective value.
f_c1Hz3000
Leaf 2 effective density
Mass divided by solid leaf volume. For mixed layers use their thickness-weighted mean density, so density × total thickness equals the total mass per area.
rho_2kg/m^3800
Leaf 2 total material thickness
Total material thickness on the second side, excluding the cavity and the first leaf.
t_2mm12.5
Leaf 2 critical frequency
Different leaf critical frequencies can separate coincidence dips. Use measured data for multilayer or bonded leaves.
f_c2Hz3000
Leaf loss factor
Dimensionless effective structural damping, assumed the same for both leaves. The 0.03 default is a screening assumption; measured damping varies with mounting and frequency.
eta_leaf0.03
Face-to-face cavity depth
Distance between the inner faces of the two leaves, including both frame depths. Default: 90 + 25 + 90 mm as in NRC TL-93-279. Absorbent material occupies this space; do not subtract its thickness.
d_gapmm205
Air-spring loss factor
Dimensionless assumed damping near mass–air–mass resonance. This sensitivity parameter does not specify an insulation product or its thickness.
eta_cavity0.15
Total partition area
Gross wall area, including any openings. Area affects only the opening fraction; finite-panel vibration and room modes are not calculated.
A_wallm^210
Total equivalent open area
Sum of unobstructed openings through the entire assembly. For a continuous gap use gap width × gap length. This is a conservative τ = 1 bypass; narrow slits and ducts can behave differently. Enter 0 for a sealed wall.
A_leakcm^210
Inspect frequency
Read the continuous-frequency transmission loss and opening sensitivity here. STC and Rw use all their bands, not this frequency.
f_probeHz500

Results

With the default inputs above, the calc gives:

ResultValue
STC estimate · with opening40
Rw estimate · with opening40 dB
TL at inspect frequency · with opening39.9 dB
Loss caused by opening at inspect frequency19.3 dB
Sealed-wall STC estimate52
Sealed-wall Rw estimate53 dB
Resonance59.1 Hz mass–air–mass resonance
Open-area limit40 dB opening ceiling

Checked against sources

Each case below was calculated by this calc and agrees with the value from its source (within the tolerance where one is shown).

NRC TL-93-279: sealed separate 13 mm gypsum leaves

Source: NRC IR-761 (1998), TL-93-279, printed p.316 / PDF p.319. Two 10 kg/m² leaves; 90+25+90 mm cavity; one 90 mm glass-fibre batt. 3000 Hz and damping are independent screening assumptions. Model checked within 3 dB only at these bands and STC; the comparison chart retains the larger low-frequency/coincidence mismatch.

Inputs: Total equivalent open area = 0 cm²; the others as above.

ResultSourceThis calc
Sealed third-octave TL at 125 Hz29 ± 3 dB28.024 dB
Sealed third-octave TL at 500 Hz60 ± 3 dB59.114 dB
Sealed-wall STC estimate53 ± 352

NRC TL-93-262: sealed separate 16 mm gypsum leaves

Source: NRC IR-761 (1998), TL-93-262, printed p.330 / PDF p.333. Surface masses 11.6 and 11.4 kg/m²; cavity 205 mm with two 65 mm glass-fibre batts. 2500 Hz is an assumed critical frequency for 16 mm gypsum, not a fitted NRC property. The wider 5 dB low-band/STC tolerance acknowledges unmodeled fill and finite-panel effects.

Inputs: Leaf 1 critical frequency = 2,500 Hz; Leaf 2 critical frequency = 2,500 Hz; Total equivalent open area = 0 cm²; Leaf 1 effective density = 725 kg/m³; Leaf 1 total material thickness = 16 mm; Leaf 2 effective density = 712.5 kg/m³; Leaf 2 total material thickness = 16 mm; the others as above.

ResultSourceThis calc
Sealed third-octave TL at 125 Hz34.4 ± 5 dB30.446 dB
Sealed third-octave TL at 500 Hz61.2 ± 3 dB61.541 dB
Sealed-wall STC estimate58 ± 554

Rating algorithm: measured NRC TL-93-279 spectrum

Source: NRC IR-761, TL-93-279 published STC 53. This verifies contour fitting from the independent measured spectrum, not prediction accuracy.

Inputs: the default inputs above.

ResultSourceThis calc
STC computed from NRC TL-93-279 measured data5353

Rating algorithm: measured NRC TL-93-262 spectrum

Source: NRC IR-761, TL-93-262 published STC 58. This verifies contour fitting from the independent measured spectrum.

Inputs: the default inputs above.

ResultSourceThis calc
STC computed from NRC TL-93-262 measured data5858

ASHRAE: 40 dB wall with 1% open area

Source: ASHRAE Handbook—Fundamentals (2025), Ch.8 Eq.41 worked example: 40 dB partition with 1% open area gives 20 dB overall. The exact energy sum is 19.957 dB; tolerance covers the published rounding. https://handbook.ashrae.org/Handbooks/F25/IP/F25_Ch08/F25_Ch08_ip.aspx

Inputs: the default inputs above.

ResultSourceThis calc
Published leakage benchmark: 40 dB wall, 1% open20 ± 0.05 dB19.957 dB

Review regression: 7 cm² opening gives STC 42

Source: Independent reviewer boundary example supplied with this review: default wall with A_leak = 7 cm² must give STC 42 after integer band rounding. Rounding rule: ASTM E413-22 §5.2, https://store.astm.org/e0413-22.html. This is a contour-rounding regression, not a published laboratory wall result.

Inputs: Total equivalent open area = 7 cm²; the others as above.

ResultSourceThis calc
STC estimate · with opening4242

Review regression: 7.2 cm² opening gives Rw 41 dB

Source: Independent reviewer boundary example supplied with this review: default wall with A_leak = 7.2 cm² must give Rw 41 dB after rounding bands to 0.1 dB. Rule: ISO 717-1:2020 §4.4, printed p.4 / attached preview p.10. This is a contour-rounding regression, not a laboratory measurement.

Inputs: Total equivalent open area = 7.2 cm²; the others as above.

ResultSourceThis calc
Rw estimate · with opening41 dB41 dB

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