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22-Mec-B11 Acoustics and Noise Control · May 2017

Question 5 of 7: Composite transmission loss of an enclosure wall

Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)

Notes on this paper

Paper format. National Exams, May 2017 — 16-Mec-B11 Acoustics and Noise Control; 3 hours; CLOSED BOOK (one approved Casio or Sharp calculator). Seven questions of equal value (20 marks each); FIVE questions constitute a complete paper. All seven are solved here so the set works as a study resource.

Reference texts. D. A. Bies, C. H. Hansen and C. Q. Howard, Engineering Noise Control, 5th ed. (CRC Press) — the standard reference for this exam code; L. L. Beranek and I. L. Vér, Noise and Vibration Control Engineering, 2nd ed. (Wiley); L. E. Kinsler, A. R. Frey, A. B. Coppens and J. V. Sanders, Fundamentals of Acoustics, 4th ed. (Wiley); CSA Z107 series and the provincial OH&S noise regulations for the Canadian occupational-exposure context.

Units and constants used throughout. Reference pressure $p_{\text{ref}}=20\ \mu\text{Pa}$; reference power $W_{\text{ref}}=10^{-12}\ \text{W}$; reference intensity $I_{\text{ref}}=10^{-12}\ \text{W/m}^2$. Where a question does not state the air temperature, air at $20\ {}^\circ\text{C}$ is assumed: $c=343\ \text{m/s}$, $\rho_0 c = 413\ \text{rayl}$. Question 3 states its own values and they are used there.

Question 5: Composite transmission loss of an enclosure wall (20 marks)

Question text not reproduced: the examination questions are © Engineers and Geoscientists BC. Open the official past paper (linked at the top of this page) to read the question, then follow the worked solution below.

Given. A 6 m × 3 m enclosure wall pierced by a 0.5 m square window of 28 dB transmission loss and a 1 m × 2 m door of 25 dB transmission loss, with an overall target of 30 dB.

Given data
ElementSizeArea (m$^2$)TL (dB)
Gross wall6 m × 3 m18.00—
Window0.5 m × 0.5 m0.2528
Door1 m × 2 m2.0025
Plain wall (remainder)—15.75to be found
Crack under door (part iii)1 m × 50 mm effective0.050 (open aperture)
Overall target——30

Find. The transmission loss the plain wall must achieve, the ceiling that the window and door impose on the whole construction, and the composite transmission loss once a 25 mm gap is left under the door.

door 1.0×2.0 mTL = 25 dBwindow 0.5×0.5 m, TL = 28 dBplain wallTL = 31.5 dB (required)25 mm crack6.0 mComposite partition — overall TL = 30 dB targetareas add on a transmission-coefficient basis, not in decibels3.0 mthe crack is the weakest path: its transmission coefficient is 1
Figure 5.1 — Elevation of the composite partition. Areas combine through transmission coefficients, so the weakest element dominates.

Approach. Convert every stated transmission loss to a transmission coefficient, area-weight them to form the composite coefficient, and invert; the same relation, solved for the unknown element, answers all three parts.

  1. Write the composite relation. Transmitted power is the sum of the power passing each element, so the area-weighted transmission coefficients add:$$\bar{\tau}=\frac{\sum_i S_i \tau_i}{S_{\text{total}}},\qquad \tau_i = 10^{-TL_i/10},\qquad TL = -10\log_{10}\bar{\tau}$$Decibels themselves never add here — that is the single most important structural fact about composite partitions.
  2. Evaluate the coefficients of the known elements. $\tau_{\text{win}}=10^{-2.8}=1.585\times10^{-3}$ and $\tau_{\text{door}}=10^{-2.5}=3.162\times10^{-3}$, so their contributions are$$S_{\text{win}}\tau_{\text{win}}=0.25(1.585\times10^{-3})=3.962\times10^{-4}$$$$S_{\text{door}}\tau_{\text{door}}=2.00(3.162\times10^{-3})=6.325\times10^{-3}$$summing to $6.721\times10^{-3}$. The door alone accounts for 94 % of that, even though it is only 11 % of the wall area.
  3. Solve for the plain wall (i). The 30 dB target requires $\bar{\tau}=10^{-3}$, hence a total budget of $S_{\text{total}}\bar{\tau}=18\times10^{-3}=1.800\times10^{-2}$. Subtracting the openings leaves $1.800\times10^{-2}-6.721\times10^{-3}=1.128\times10^{-2}$ for the 15.75 m$^2$ of plain wall:$$\tau_{\text{wall}}=\frac{1.128\times10^{-2}}{15.75}=7.161\times10^{-4}$$$$\boxed{TL_{\text{wall}} = -10\log_{10}(7.161\times10^{-4}) = 31.5\ \text{dB}}$$Rebuilding the composite from this answer returns exactly 30.0 dB, which closes the calculation.
  4. Find the theoretical ceiling (ii). Let the plain wall become perfect, $\tau_{\text{wall}}\to 0$. All the leakage is then through the window and door:$$\bar{\tau}_{\min}=\frac{6.721\times10^{-3}}{18}=3.734\times10^{-4}$$$$\boxed{TL_{\max}=34.3\ \text{dB}}$$No amount of investment in the wall itself can beat 34.3 dB while that door and window are in place, and the 30 dB design is already within 4.3 dB of that ceiling. Practically, this means the next design move must be a better door, not a heavier wall.
  5. Add the crack under the door (iii). The gap is 25 mm high, but the floor image doubles it to an effective 50 mm, so over the 1 m door width the effective open area is $S_{\text{crack}}=1.0\times0.050 = 0.05\ \text{m}^2$. At 500 Hz the wavelength is 0.69 m, so the gap is acoustically small and behaves as a simple open aperture with $\tau = 1$ ($TL = 0$ dB). Taking that area out of the door leaf, the new sum is$$\sum S_i\tau_i = 15.75(7.161\times10^{-4}) + 0.25(1.585\times10^{-3}) + 1.95(3.162\times10^{-3}) + 0.05(1.0) = 6.784\times10^{-2}$$$$\bar{\tau}=\frac{6.784\times10^{-2}}{18}=3.769\times10^{-3}$$$$\boxed{TL_{\text{with crack}} = 24.2\ \text{dB}}$$The crack is 0.28 % of the wall area and yet carries 74 % of all transmitted power, costing 5.8 dB of the 30 dB design. It also drops the construction below the 34.3 dB ceiling of part (ii) by more than 10 dB.

The engineering conclusion is unambiguous: sealing is not a finishing detail but a primary acoustic element. A door that is specified at 25 dB but hung with a 25 mm undercut for ventilation delivers roughly 13 dB in service, and the whole partition follows it down. Fitting an automatic drop seal or a threshold gasket recovers the full 5.8 dB at negligible cost compared with upgrading 15.75 m$^2$ of wall.

Check: the crack is modelled as a fully open aperture. Taking $\tau = 1$ for the gap is the standard conservative engineering assumption and is what the 500 Hz wavelength check supports. In reality a narrow slit can show $\tau \gt 1$ at its own resonance frequencies (the slit acts as a short tube), and a viscous, deep slit can show $\tau \lt 1$; both effects are second order beside the area term and neither changes the conclusion.

Final results — Question 5
PartQuantityResult
iRequired TL of the plain wall31.5 dB
iiGreatest theoretically possible overall TL34.3 dB
iiiOverall TL with the 25 mm crack (500 Hz)24.2 dB (a loss of 5.8 dB)
—Share of transmitted power through the crack74 %