Dwelling Airtightness Testing Report

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Dwelling Airtightness Testing Report

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Dwelling Airtightness Testing Report BSRIA Airtightness Old Bracknell Lane West Bracknell, Berkshire RG12 7AH Phone: 0800 5871000 Fax: 01344 465691 Report N : DAT-DRA01-NA01-SOU01-1-PL1-T1 Date: 14/05/2010 Accreditation Body: ATTMA Client: Region: Dr Antony Cowling N/A Address: 7 South Drive Sonning Reading Berkshire RG4 6GB Telephone: 0118 969 8326 Facsimile: Test Results at 50 Pascals Measured Air Permeability (m³/(h.m²)): 0.98 Airtightness Engineer: P Dooley Registration Number: 0005 Plot N : 1 Developers Type: Development Name: Development Address: Did the dwelling achieve the required air permeability as specified in the SAP calculations? Building Leakage Curve Air Flow Coefficient (C env ): 30.3 Test Information Exponent (n): 0.72 N/A South Drive 7 South Drive Sonning Reading Berkshire RG4 6GB Q 50 : Airflow (m³/h): 506 Design Air Permeability (m³/(h.m²)): 1.00 YES Air Leakage Coefficient (C L ): 30.5 Correlation Coefficient (r²): 0.9983 TS1 Leakage Area (m²): 0.025 Type of Test: Depressurisation Test Method: B Test Standard: TS1 800 700 600 500 400 Building 300 Leakage (m³/h) 200 Regulation Complied With: ADL1A 100 90 80 4 5 6 7 8 9 10 20 30 40 50 60 70 80 Building Pressure (Pa)

Dwelling Airtightness Testing Report Page 2 of 7 Date of Test: 14/05/2010 Report N : DAT-DRA01-NA01-SOU01-1-PL1-T1 Dwelling Information Type Detached Envelope Area 516.00 Gross Floor Area 240.00 Storeys 3.0 Cold Floor Present No Warm Roof Construction No Envelope Area Verified Yes Construction Traditional Heating Type of Air Conditioning Type of Ventilation HRV Year of Construction 2010 Equipment Information Type Manufacturer Model Identifier Calibration Identifier Calibration Expiry Fan Energy Conservatory Model 3 (110V) BDS12-1 57753 02/09/2010 Micromanometer Energy Conservatory DG700 BDS12-2 57754 03/09/2010 Barometer Testo 511 BDS12-9 57757 04/09/2010 Thermometer Testo 110 BDS12-3 57756 04/09/2010 Anemometer Kaindl Windtronic 2 BDS12-13 57758 04/09/2010 HRV system sealed at source Water traps filled Internal doors opened Windows closed Kitchen extract sealed (taped) Dwelling Preparation Comments

Dwelling Airtightness Testing Report Page 3 of 7 Date of Test: 14/05/2010 Report N : DAT-DRA01-NA01-SOU01-1-PL1-T1 Depressurization Test: Environmental Data Internal Temperature( C) External Temperature( C) Barometric Pressure(mbar) Wind Speed (m/s) Pre-Test 19.5 12.9 1006.1 0.0 Post-Test 19.9 12.9 1006.1 0.0 Average 19.7 12.9 1006.1 0.0 Pre-Test Fan-Off Pressure Data Post-Test Δp 0,1 - Δp 0,1 + Δp 0,1 0.0 2.7 2.7 Δp 0,2 - Δp 0,2 + Δp 0,2 0.0 2.9 2.9 Data Points Dwelling Pressure (Pa) Fan Pressure (Pa) Uncorrected Flow (m³/h) Corrected Flow (m³/h) % Error Fan Configuration 2.7 n/a -23.0 80.2 319 314-0.2 Ring C -30.7 116.1 388 382 0.7 Ring C -36.4 137.8 425 419-1.4 Ring C -41.5 25.5 481 474 2.2 Ring B -46.1 27.4 499 492-1.2 Ring B -50.7 31.7 538 530-0.2 Ring B -57.0 37.4 585 576 0.2 Ring B 2.9 n/a Deviations from Standard - Comments Deviations from Standard - Test Parameters

Dwelling Airtightness Testing Report Page 4 of 7 Equations Used to Calculate Test Data as Specified in ATTMA-TS1, Appendix A, 13/07/07 A1.1. Corrections for zero flow pressure differences Zero flow pressure difference corrections are applied to the observed building differential pressures for wind and stack effects. The average zero-flow pressure difference is subtracted from each of the measured pressure differences, Δp m, to obtain the induced pressure differences, Δp env, using equation: Δp env = Δp m (Δp 0,1 + Δp 0,2 )/2 where Δp 0,1 is the average of all zero flow pressure differences at the start of the test and Δp 0,2 is the average of all zero flow pressure differences at the end of the test. A1.2. Calculation of air density The air density, ρ, in kg/m 3, at a temperature, θ, in o C and the absolute pressure, p bar, in Pa, is obtained by using the following equation. This is calculated as an average of temperature and absolute pressure readings taken immediately before, during and immediately after the test. ρ = (p bar /287.055 (θ + 273.15) A1.3. Correction for actual and observed airflow through the measuring device The actual flow rate through the fan is a function of the measured values at the last fan calibration and measured values during the air test. This is calculated by equation: Q m = Q c (ρ c /ρ m ) where Q m is the actual volumetric flow rate through the fan during the test, Q c is the airflow rate from the last calibration of the fan, ρ m is the density of air passing through the fan (kg/m 3 ) and ρ c is the air density recorded during fan calibration. A1.4. Correction for internal/external air density differences A correction is made for the internal/external density differences between air passing through the airflow measuring device and air passing through the building envelope. The applied correction depends on whether the building is being pressurised or depressurised. A1.4.1. Corrections to airflow rate for pressurisation tests: The measured airflow rate, Q m, is converted to airflow through the building envelope, Q env(out), for pressurisation using equation: Q env(out) = Q m (ρ e /ρ i ) where Q env(out) is the actual air flow volume out through the envelope, ρ e is the mean external air density (kg/m 3 ) and ρ i is the mean internal air density (kg/m 3 ).

Dwelling Airtightness Testing Report Page 5 of 7 A1.4.2. Corrections to airflow rate for depressurisation tests: The measured airflow rate, Q m, is converted to airflow through the building envelope, Q env(in), for depressurisation using equation: Q env(in) = Q m (ρ i /ρ e ) Where Q env(in) is the actual air flow volume out through the envelope, ρ e is the mean external air density (kg/m 3 ) and ρ i is the mean internal air density (kg/m 3 ). A1.5. Determination of constants C and n using a least squares technique The results from a steady state building test give a dataset comprised of building differential pressures (ΔP env ) and corresponding fan flow rates (Q). A linear least squares curve fitting approximation is used to produce a best-fit line between these points. The most straightforward of these is the least squares approximation. For this, the straight line y = mx + b is fitted through the given points (x 1, y 1 ),.,(x n, y n ) so that the sum of the squares of the distances of those points from the straight line is minimum, where the distance is measured in the vertical direction. The airflow rates and corresponding pressure differences are plotted on a log-log graph for pressurisation and depressurisation as required. The calculation of the factors m and b for a given pressurisation test are as follows: dsumxy = Σ( In ΔP env * In Qc) dsumxx = Σ( In ΔP env * In ΔPenv) dsumx = Σ(In ΔP env ) dsumy = Σ(ln Q C ) m = (dsumx * dsumy - Numpnts * dsumxy) / (dsumx * dsumx - dsumxx * Numpnts) b = (dsumx * dsumxy - dsumxx * dsumy) / (dsumx * dsumx - dsumxx * Numpnts) From this the air flow coefficient, C env, and air flow exponent, n, are obtained: C env = exp b n = m

Dwelling Airtightness Testing Report Page 6 of 7 A1.6. Correction of airflow rates through the envelope to STP The relationship is established between volumetric flow rate through the fan and the induced building envelope pressure difference: Q env = C env (Δp env ) where Q env is the air flow rate through the building envelope (m 3 /h) and Δp env is the induced pressure difference, in Pascals. The air leakage coefficient, C L, is obtained by correcting the air flow coefficient, C env, to standard conditions (i.e. 20 oc and 101325 Pa) for pressurisation using equation: C L = C env (ρ i /ρ s ) 1-n where ρ i is the indoor air density (kg m -3 ) and ρ s is the air density at standard conditions (kg/m 3 ). The air leakage coefficient, C L, is obtained by correcting the air flow coefficient, C env, to standard conditions (i.e. 20 o C and 101325 Pa) for depressurisation using equation: C L = C env (ρ e /ρ s ) 1-n where ρ e is the outdoor air density (kg/m 3 ) and ρs is the air density at standard conditions (kg/m 3 ) The air leakage rate, Q, for a given building differential pressure, Δp env, can be calculated using equation: Q = C L (Δp env ) n where CL is the air leakage coefficient, in m 3 /(h Pa n ), Δp env is the induced pressure difference (Pa) and n is the air flow exponent. A1.7. Air permeability The air permeability, Q 50 /(S+F), is the air leakage rate at a pressure difference of 50 Pa, divided by the building envelope area S + F (m 2 ). Units are m 3 h -1 per m 2 of envelope area. The air permeability is calculated from: Q 50 = C * (ΔP) n Air Permeability = 3600 * Q 50 / (S + F) where S is the exposed surface area of the walls and roof, and F is the area of the solid ground floor. A1.8. Correlation coefficient (r 2 ) The correlation coefficient (r 2 ) is a measure of the strength of association between the observed values of building differential pressure (Δρenv) and corresponding fan flow rates. Correlation coefficient = S xy / (σ 2 ) where; σ 2 = (Numpnts * dsumxx - dsumx * dsumx) * (Numpnts * dsumyy - dsumy * dsumy) S xy = Numpnts * dsumxy - dsumx * dsumy.

C. Equivalent Leakage Area Dwelling Airtightness Testing Report Page 7 of 7 It is often useful for the test engineer to translate the results of an air leakage test in to a more readily understandable form such as equivalent leakage area, m. Area of holes left in the structure can be a useful guide, but it is only an aerodynamic equivalent area based on a sharp edged orifice and should therefore be regarded as approximate. The flow rate of air can be expressed by: Q = A.C d {2Δp/ρ} 0.5 m 3.s -1 Where the discharge coefficient, C d for a sharp edged orifice can be taken as 0.61 and if ρ is taken as 1.2 kg.m -3 this can be simplified to: Q Δp = 0.788. A (Δp) 0.5 m 3.s -1 or at a test pressure of 50 pascals, Equivalent Leakage Area is: A = Q 50 /5.57 m 2