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A capillary tube with a bore diameter only 1% above nominal passes approximately 4% more liquid at the same pressure differential, provided the flow is fully developed and laminar. That sensitivity makes bore tolerance a functional requirement, not merely a dimensional detail. A nominal inside diameter and a material certificate do not establish metering accuracy.
The critical distinction is between a tube that meets dimensional limits and one that delivers a specified flow under defined conditions. Reliable qualification connects bore geometry to hydraulic resistance, then verifies that relationship using a measurement method capable of resolving the required tolerance.
For steady, fully developed laminar flow of an incompressible Newtonian liquid through a straight, circular tube, the Hagen–Poiseuille relationship is:
Q = πd4ΔP / (128μL)
Here, Q is volumetric flow rate, d is internal diameter, ΔP is the pressure difference across the tube, μ is dynamic viscosity, and L is tube length. The fourth-power dependence on diameter explains why a small bore deviation can outweigh a comparable percentage deviation in length.
For small changes, the corresponding sensitivity is:
δQ/Q ≈ 4δd/d + δ(ΔP)/ΔP − δμ/μ − δL/L
This is a first-order sensitivity relationship, not automatically a statistical uncertainty calculation. It shows which variables require control; combining their uncertainties requires attention to independence, correlation, and the chosen confidence level.
Consider an illustrative tube with a nominal bore of 0.500 mm and a diameter tolerance of ±0.005 mm. With all other variables fixed, the exact fourth-power relationship gives:
If the entire allowable flow deviation were ±1%, diameter alone would need to remain within approximately ±0.25%, or ±1.25 μm for this bore. In a functioning metering system, pressure, viscosity, length, and measurement uncertainty also consume part of that allowance, leaving a tighter budget for bore variation.
The basic equation assumes a uniform diameter. Drawn specialty-alloy tubing can instead contain axial variation, ovality, or localized restrictions introduced during processing, cutting, joining, or bending. Measuring the two open ends does not establish the geometry between them.
For a circular bore whose diameter changes gradually along its length, a local laminar-flow approximation gives:
ΔP/Q = (128μ/π) ∫0L dx/d(x)4
The consequence is important: hydraulic resistance depends on the accumulated inverse fourth power of diameter, not the arithmetic mean diameter. Narrow sections contribute disproportionately. Their effect still depends on their length; a very short restriction should not automatically be treated as controlling the entire tube. Abrupt restrictions also introduce additional losses that this approximation does not capture.
Ovality creates another limitation. Two bores with the same cross-sectional area but different shapes need not have the same resistance. An equivalent-area diameter, or an average of maximum and minimum bore measurements, cannot by itself establish equivalent metering performance.
A functional specification should therefore distinguish between average dimensions, permitted local restrictions, and acceptable finished-tube flow. These requirements address different failure modes and are not interchangeable.
The diameter relationship is a strong starting point, but it is not a universal capillary-flow law. Its assumptions must match the fluid and operating conditions.
Flow regime and entrance effects. Reynolds number, Re = ρvd/μ, helps assess whether laminar behavior is plausible. Fully developed flow also requires sufficient entrance length. In a short capillary or an assembly with restrictive fittings, entrance, exit, and connection losses can represent a meaningful share of total pressure drop. Pressure measured upstream of an entire assembly is not necessarily the pressure drop across the tube alone.
Gas compressibility. Gas density changes along the bore as pressure falls. Liquid-flow calculations using a single volumetric flow rate can therefore be misleading. Gas qualification must identify absolute inlet and outlet pressures, temperature, and whether flow is reported as mass flow, actual volume, or volume at stated reference conditions. Large pressure ratios may require models addressing choking and other compressible-flow effects.
Fluid behavior and temperature. Non-Newtonian fluids do not have one constant viscosity applicable to every shear condition. For ordinary liquids, temperature-dependent viscosity can still cause appreciable flow changes. Thermal expansion changes the tube dimensions as well, but its contribution must be assessed alongside viscosity rather than assumed to dominate.
Two-phase flow. Flashing, boiling, or entrained gas invalidates a simple single-phase resistance calculation. A capillary carrying a liquid–vapor mixture needs an application-specific model and performance test.
The operating architecture also matters. Under a controlled pressure differential, bore variation changes flow directly. With a positive-displacement source imposing flow, it primarily changes the required pressure until leakage, compliance, or pressure limits affect delivery.
In fully developed laminar flow, surface roughness does not enter the resistance calculation in the same way it does for turbulent flow. It is therefore misleading to assign a universal flow correction based solely on a roughness value. Internal deposits, burrs, weld protrusions, and adhered particles matter because they alter the available passage or create localized losses.
For nickel-based and titanium capillaries, alloy selection helps preserve that passage in service. Corrosion, erosion, or deposition can shift resistance after initial calibration. A 1% increase in uniform bore diameter would produce approximately a 4% increase in flow under the original liquid-flow assumptions; deposit buildup produces the opposite effect.
Material-form documentation must also remain separate from finished-tube qualification. Information supplied for Hastelloy Alloy Strips can support an assessment of starting-stock composition or formability, but strip thickness and strip certification do not demonstrate capillary bore control. Finished-tube geometry, internal condition, and hydraulic performance require their own evidence.
Applicable material standards establish only part of the acceptance basis. ASTM B575 addresses specified nickel-alloy plate, sheet, and strip, while ASTM B626 covers specified welded nickel-alloy tubing. Compliance with an applicable product standard should not be interpreted as a guarantee of application-specific metering accuracy. The purchase specification must identify the relevant grade, product form, standard edition, and supplementary dimensional or functional requirements.
For a metering capillary, useful acceptance requirements include:
Outside diameter and wall thickness measurements can infer an inside diameter, but they do not necessarily reveal eccentricity or local internal defects. Sectioning sacrifices the sample and examines only selected locations. Imaging methods require validated resolution and defect detectability. Flow testing measures effective resistance directly, but cannot uniquely identify the geometry responsible for it.
The strongest qualification combines complementary evidence. Dimensional inspection establishes manufacturing control; flow testing confirms functional resistance. Testing after final cutting, cleaning, and forming captures changes that earlier inspection may miss.
A stable tube with a consistent dimensional offset can be individually calibrated. That corrects its initial flow relationship under specified conditions; it does not establish interchangeability or protect against contamination, corrosion, or installation damage.
Where tubes must be replaced without recalibration, finished-part flow tolerance is often a more direct acceptance criterion than nominal bore alone. Where individual calibration is permitted, bore limits still constrain pressure requirements and sensitivity to service changes. The decisive requirement is a verified resistance–flow relationship across the intended operating range, supported by dimensional controls that keep that relationship repeatable.