ME3311 · Hydraulic & Pneumatic
Theme 3 · Lines & losses

Sizing the line

Choosing a pipe bore is one short calculation: pick a speed from the recommended band, and the flow fixes the diameter.

Source: Rabie, Fluid Power Engineering, Ch. 3.

Before you start

What you need first

  • Flow = area × speed, \(Q=Av\) (Topic 3).
  • Recommended line speeds (Topic 14).

What you'll be able to do

  • Find oil speed from flow and bore, \(v=\tfrac{4Q}{\pi D^2}\).
  • Size a bore from a target speed, \(D=\sqrt{\tfrac{4Q}{\pi v}}\).
  • Check a line against the recommended band.

Start here · the relation

Speed from flow and bore

The pipe's cross-section is a circle, \(A=\tfrac{\pi}{4}D^2\), so \(v=Q/A\) becomes:

$$v = \dfrac{Q}{A} = \dfrac{4Q}{\pi D^2}$$
where:
SymbolMeaningSI unit
voil velocity in the pipem/s
Qflow ratem³/s
Dpipe inside diameter (bore)m
Because \(D\) is squared, velocity is very sensitive to bore: \(v\propto 1/D^2\).

Pick a diameter from a target speed

To design a line, choose a speed from the recommended band and rearrange for the bore:

$$D = \sqrt{\dfrac{4Q}{\pi v}}$$

Then round up to the next standard pipe size (rounding up keeps the actual speed at or below your target).

bore D slow bore D/2 fast (×4) same flow Q in both
Same \(Q\): halve the bore and the speed rises four-fold (\(v\propto 1/D^2\)).

Which speed to choose

Take the speed from the recommended band for that line (Topic 14), then size the bore:

LineDesign speedNote
Pressure2 – 6 m/sHigher → the thinnest pipe
Suction0.6 – 1.6 m/sKept lowest → the fattest pipe (avoids cavitation)
Return / low-pressure0.6 – 1.6 m/sSame low band as suction (Rabie)
For the same flow, the low-pressure lines (suction & return) are the fattest because they run far slower than the pressure line — and the suction, designed at the lowest speed, is the largest of all. A frequent exam point.

✏️ Try it yourself — no numbers needed

A line carries a fixed flow at 2 m/s. To save space, someone swaps it for a pipe of half the bore. What happens to the oil speed, and why does that matter for losses?

Speed ×4 → 8 m/s. Since \(v=4Q/\pi D^2\), halving \(D\) makes the area \(4\times\) smaller, so the oil runs four times faster. Why it matters: friction loss grows with \(v^2\) (and the laminar loss with \(1/D^4\) — next topics), so a "small" bore saving causes a large jump in lost pressure and heat. 8 m/s is also well above the recommended band.

Common mistakes to avoid

MistakeFix
Leaving \(Q\) in L/minConvert: ÷60,000 to get m³/s.
Putting bore in mm into the formulaUse metres: \(25~\text{mm}=0.025~\text{m}\).
Rounding the bore down to a standard sizeRound up — a bigger bore keeps the speed at/below target.

Recap — the whole topic on one screen

$$v=\dfrac{4Q}{\pi D^2}\qquad D=\sqrt{\dfrac{4Q}{\pi v}}$$
IdeaWhat you own now
Speed from bore\(v=4Q/\pi D^2\); \(v\propto 1/D^2\)
Size a boreChoose \(v\) from the band, then \(D=\sqrt{4Q/\pi v}\), round up
Suction is fattestLowest design speed → biggest bore

Next topic

Laminar, turbulent & the Reynolds number

Now that we know the speed, we can ask: is the flow smooth or chaotic? That decides how much pressure friction will cost — and it's settled by the Reynolds number.

→ Laminar, turbulent & Reynolds number