Method 1
Sample & Velocity Traverses
Complete interactive guide for determining the number and location of sampling points in stationary source stacks and ducts — with built-in calculators for every equation.
☰ Table of Contents
Scope & Applicability
EPA Method 1 is titled "Sample and Velocity Traverses for Stationary Sources." It provides the procedure for determining the number of sampling or velocity measurement points and their location across a stack or duct cross-section.
The method applies to all EPA reference methods (Methods 2 through 8 and beyond) that require measuring gas velocity, extracting a gas sample, or both. Every test that uses a pitot tube, a sampling probe, or any other measurement device inserted into a stack depends on Method 1 to define where those measurements must be taken.
The method covers two duct geometries:
- Circular (round) stacks and ducts — uses the log-linear rule to place points along two perpendicular diameters.
- Rectangular ducts — uses the log-Tchebycheff rule to distribute points across the cross-section grid.
The goal is always the same: ensure the set of measurement points is statistically representative of the entire gas flow so that the final calculated velocity and emission rate are accurate.
Principle & Summary
The velocity profile in a duct is NOT uniform — it is higher near the center and lower near the walls due to friction and boundary layer effects. If you measure velocity at only one point, you get a wrong answer. Method 1 solves this by creating a traverse: a pattern of points that, when averaged, reproduces the true mean velocity.
How it works for circular ducts:
- Measure the stack inner diameter (D).
- Determine the minimum number of traverse points from a lookup table based on D.
- Place points along two diameters at distances specified by the log-linear rule (as fractions of D from the wall).
- Measure velocity or extract sample at each point.
- Compute the arithmetic average of all point values.
How it works for rectangular ducts:
- Measure duct width (W) and height (H) to compute area A = W × H.
- Determine minimum number of points from a lookup table based on A.
- Distribute points in a grid using the log-Tchebycheff rule for fractional positions.
- Measure and average as above.
Circular Duct — Number of Traverse Points
For a circular stack, the minimum number of traverse points depends on the inside diameter D. The total number of points is always 2 × n, where n is the number of points per diameter. Points are placed on two perpendicular diameters.
| Stack Diameter (ft) | Min. Points per Diameter (n) | Total Points (2n) |
|---|---|---|
| 0.12 – 0.25 | 3 | 6 |
| > 0.25 – 0.50 | 4 | 8 |
| > 0.50 – 1.0 | 5 | 10 |
| > 1.0 – 2.0 | 6 | 12 |
| > 2.0 – 4.0 | 7 | 14 |
| > 4.0 – 8.0 | 8 | 16 |
| > 8.0 | 9 | 18 |
Log-Linear Rule — Point Locations
Once you know how many points per diameter (n), the log-linear rule gives the fractional distance from the inside wall for each point. These fractions are multiplied by the radius (R = D/2) to get the actual insertion depth from each wall.
The points are arranged symmetrically: if the fractional distance from one wall is p, the corresponding point on the opposite side is at (1 − p) from that wall.
| Points per Diameter (n) | Fractional Distances from Wall (pi) |
|---|---|
| 3 | 0.0594, 0.2500, 0.7500 |
| 4 | 0.0359, 0.1942, 0.6458, 0.8058 |
| 5 | 0.0257, 0.1463, 0.5000, 0.8537, 0.9743 |
| 6 | 0.0200, 0.1175, 0.4063, 0.5937, 0.8825, 0.9800 |
| 7 | 0.0163, 0.0983, 0.3404, 0.5000, 0.6596, 0.9017, 0.9837 |
| 8 | 0.0138, 0.0846, 0.2935, 0.4372, 0.5628, 0.7065, 0.9154, 0.9862 |
| 9 | 0.0119, 0.0746, 0.2590, 0.3866, 0.5000, 0.6134, 0.7410, 0.9254, 0.9881 |
- di
- = insertion depth from wall for point i
- pi
- = fractional distance from wall (from table above)
- R
- = stack inside radius
- D
- = stack inside diameter
Rectangular Duct — Number of Traverse Points
For rectangular ducts, the minimum number of points is based on the cross-sectional area. Points are distributed in a grid pattern.
| Duct Area (ft²) | Minimum Total Points |
|---|---|
| < 4 | 9 |
| 4 – 12 | 12 |
| > 12 – 25 | 16 |
| > 25 – 36 | 20 |
| > 36 – 49 | 24 |
| > 49 – 64 | 30 |
| > 64 | 36 |
The total points must be arranged in a grid as close to square as possible. For example, 12 points could be arranged as 4 × 3 or 3 × 4.
Log-Tchebycheff Rule — Rectangular Point Positions
For rectangular ducts, point positions along each axis are determined by the log-Tchebycheff rule. The fractional positions depend on the number of measurement lines along that axis.
| Lines per Axis | Fractional Positions from Wall |
|---|---|
| 3 | 0.136, 0.500, 0.864 |
| 4 | 0.097, 0.394, 0.606, 0.903 |
| 5 | 0.076, 0.321, 0.500, 0.679, 0.924 |
| 6 | 0.063, 0.270, 0.440, 0.560, 0.730, 0.937 |
| 7 | 0.054, 0.235, 0.390, 0.500, 0.610, 0.765, 0.946 |
| 8 | 0.047, 0.209, 0.351, 0.452, 0.548, 0.649, 0.791, 0.953 |
| 9 | 0.042, 0.189, 0.321, 0.413, 0.500, 0.587, 0.679, 0.811, 0.958 |
- ti, tj
- = fractional positions from log-Tchebycheff table
- W
- = duct width
- H
- = duct height
Cross-Sectional Area Calculation
The cross-sectional area is needed to convert average velocity to volumetric flow rate. It is calculated differently for circular and rectangular ducts.
- A
- = cross-sectional area
- D
- = inside diameter
- π
- = 3.14159265
- W
- = duct width
- H
- = duct height
Pitot Tube Velocity Equation
The standard (Type S) pitot tube measures the velocity pressure (ΔP), which is the difference between total pressure and static pressure. This is converted to gas velocity using the following equation from EPA Method 2 (which relies on Method 1 for point placement).
- vs
- = stack gas velocity (ft/s or m/s)
- Kp
- = pitot tube coefficient (typically 0.84 for standard Type S)
- Cp
- = 85.49 (for ft/s) or 34.97 (for m/s)
- ΔP
- = velocity pressure (in. H2O)
- Ts
- = absolute stack gas temperature (°R or °K)
- Ms
- = molecular weight of stack gas (lb/lb-mole)
- Ps
- = absolute stack gas pressure (atm)
Gas Density Calculation
The dry gas density is needed for several emission calculations. It can be derived from the ideal gas law using molecular weight, temperature, and pressure.
- ρd
- = dry gas density (lb/ft³ or kg/m³)
- Md
- = dry molecular weight (lb/lb-mole or kg/kg-mole)
- Ps
- = absolute pressure (atm)
- R
- = 0.7302 (for lb, ft³, atm, °R) or 0.08206 (for g, L, atm, °K)
- Ts
- = absolute temperature (°R or °K)
- Ms
- = wet molecular weight of stack gas
Volumetric Flow Rate
The volumetric flow rate is the product of the average velocity (determined from Method 1 traverse + Method 2 pitot measurements) and the cross-sectional area.
- Qs
- = volumetric flow rate (actual cubic feet per minute, ACFM)
- vs
- = average stack gas velocity (ft/s)
- A
- = cross-sectional area (ft²)
- 60
- = conversion from seconds to minutes
- Qsd
- = dry standard volumetric flow rate (DSCFM)
- Bws
- = moisture fraction (from Method 4)
- Tstd
- = 528 °R (68 °F) or 293 °K (20 °C)
- Pstd
- = 1.0 atm
Stack Diameter from Circumference
In the field, it is often easier to measure the stack circumference (by wrapping a tape around the outside) than the diameter directly. The inside diameter must be derived by accounting for the wall thickness.
- D
- = inside diameter
- C
- = outside circumference (measured with tape)
- π
- = 3.14159265
- t
- = wall thickness
Quick Reference Summary
Use this table as a field reference card. All the key decisions and equations in one place.
| Task | Method / Rule | Key Input |
|---|---|---|
| Circular: Number of points | Diameter lookup table | Inside diameter D |
| Circular: Point positions | Log-linear rule | n (points/diameter), R = D/2 |
| Rectangular: Number of points | Area lookup table | A = W × H |
| Rectangular: Point positions | Log-Tchebycheff rule | Grid lines per axis |
| Inside diameter | D = C/π − 2t | Circumference C, thickness t |
| Cross-sectional area (circle) | A = πD²/4 | Diameter D |
| Velocity | v = KpCp√(ΔPT/MsPs) | ΔP, Ts, Ms, Ps |
| Gas density | ρ = MP/(RT) | M, Ps, Ts |
| Volumetric flow (ACFM) | Q = v × A × 60 | v, A |
| Dry std. flow (DSCFM) | Qsd = Qs(1−Bws)(Tstd/Ts)(Ps/Pstd) | Qs, Bws, Ts, Ps |
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