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Shaft Alignment & Thermal Growth — Why a Perfect Cold Alignment Is a Defect

The situation on site

A hot-oil pump, 180 °C, driven by a 90 kW motor. The millwright is proud of this one: laser aligned, offset 0.01 mm, angularity 0.01 mm/100 mm, printed report in the file. Best numbers he has ever produced on this unit.

Six weeks later the coupling element is cracked, the pump inboard bearing is running hot, and the vibration spectrum has a strong 2× running-speed peak with high axial amplitude — the textbook misalignment signature.

Guess first: the alignment report says 0.01 mm. Where did the misalignment come from?

The reveal: the pump shaft climbed 0.51 mm as the casing and pedestal reached temperature. The motor climbed 0.16 mm — a 0.35 mm difference at the front feet, which projects to 0.29 mm of offset at the coupling. The machine that was perfect at 25 °C is running four times its 0.07 mm tolerance out at 180 °C. The alignment report was not wrong. It was taken in the one condition the machine never operates in.

The misconception, stated plainly

"Aligned cold = aligned running. Zero is the target; anything else is sloppy work."

Let it stand. It is what every instinct says, and it is what an alignment report measures.

Then dismantle it: alignment is only meaningful at operating temperature. Everything that holds the shaft up — casing, pedestal, bearing housing, baseplate — is metal, and metal that gets hot gets taller. The two machines rarely get hot by the same amount, from the same height, in the same material. So the two shaft centrelines move by different amounts.

Which means the cold alignment must be deliberately wrong, by exactly the difference the heat is going to make, and in the opposite direction. Cold zero is not neutral. Cold zero is a decision to be misaligned hot.

The two misalignments, and why they cost money

OFFSET (parallel)   — the two shaft centrelines are parallel but not collinear.   [mm]
ANGULAR (gap)       — the two centrelines meet at an angle.                       [mm per 100 mm]

Both exist in two planes at once: vertical (fixed by shims) and horizontal (fixed by sideways moves / jack bolts). Four numbers, and a real job sets all four.

Why it matters:

Tolerance is not "as tight as possible" — it is a function of speed, because the damage is a per-revolution event:

Speed Offset — excellent / acceptable Angularity — excellent / acceptable
1 000 rpm 0.06 / 0.13 mm 0.05 / 0.10 mm per 100 mm
1 500 rpm 0.05 / 0.10 mm 0.04 / 0.08 mm per 100 mm
3 000 rpm 0.03 / 0.07 mm 0.03 / 0.06 mm per 100 mm
6 000 rpm 0.02 / 0.03 mm 0.02 / 0.03 mm per 100 mm

(typical vendor / API 686 practice — always use the machine vendor's own table.)

Symbol key — every symbol on this sheet

The one formula, applied four times

g = α · L · ΔT                (growth of one support, mm)

Apply it at each foot of each machine, because each foot can have its own height and its own temperature. Then:

cold target at the coupling   = g_stationary(coupling) − g_movable(coupling)
cold shim at movable foot i   = target evaluated at that foot's position

Sign convention that keeps you out of trouble: whichever machine grows more must start lower. A hot pump grows more than its motor, so the motor is shimmed up cold. It feels wrong every time and it is right every time.

Typical α values (×10⁻⁶ /°C): carbon/alloy steel 11.7, cast iron 10.8, 12 % Cr (410) 9.9, austenitic 304/316 17.3, aluminium 23. A stainless pedestal grows nearly 50 % more than a carbon-steel one at the same height and temperature — material choice alone can be a 0.1 mm error.

Feed real geometry into the cold-target calculator: ▶ open the interactive: rotating alignment calc — enter the two machines' materials, foot heights and operating temperatures and it returns the shim change at each foot, the cold offset and angularity you should read on the laser, and a live picture of the two centrelines cold and hot.

Where exactly is the growth datum?

L is measured from the surface that does not move to the shaft centreline — and choosing it wrongly is the most common way to get a plausible but useless answer.

  • If the pedestals are part of the pump and bolt to a baseplate that stays near ambient, the datum is the top of the baseplate and L is baseplate-to-shaft-centreline.
  • If the whole baseplate heats up (a fully-hot skid, or a baseplate flooded by product spillage), both machines ride up together and the common part cancels. Only the difference above the common datum counts. Using the foundation as the datum then over-states both growths but still gives the right difference — which is why the difference, not the absolute, is the answer.
  • If the pump is centreline-mounted (API 610 hot service), the support feet are at the shaft centreline elevation, so L ≈ 0 and the vertical growth is almost eliminated by design. That is the whole point of centreline mounting, and it is why foot-mounted hot pumps are a bad idea.
  • For a machine on a sliding-foot arrangement, the datum is the sliding plane and the growth along the shaft is taken up by the slide — but only if the slide is free. A seized slide turns axial growth into an angular kick at the feet.

Horizontal (side-to-side) thermal movement is usually ignored for symmetric machines because the casing grows equally both ways about its own centreline. It stops being true for a casing with one hot side, a single side-mounted support, or a machine restrained by a nozzle on one side only.

Worked example — 180 °C pump and its motor

Geometry (coupling centre at x = 0, motor to the right):

Pump (stationary):  shim-plane to shaft CL   L = 350 mm   carbon steel α = 11.7e-6
                    front foot 300 mm from coupling, metal 150 °C
                    rear  foot 900 mm from coupling, metal 180 °C
Motor (movable):    shim-plane to shaft CL   L = 400 mm   carbon steel α = 11.7e-6
                    front foot 250 mm, rear foot 850 mm, metal 60 °C both
Aligned at metal temperature 25 °C.  Speed 2 950 rpm.

Step 1 — growth at each foot.

pump front  g = 11.7e-6 × 350 × (150−25) = 0.512 mm
pump rear   g = 11.7e-6 × 350 × (180−25) = 0.635 mm
motor both  g = 11.7e-6 × 400 × ( 60−25) = 0.164 mm

Step 2 — project each shaft line to the coupling. The pump line rises 0.512 mm at x = −300 and 0.635 mm at x = −900, so its slope is (0.635 − 0.512)/(−600) = −0.000205 mm/mm and at the coupling it has risen 0.512 − 0.000205 × 300 = 0.451 mm. The motor is flat: 0.164 mm.

Step 3 — the cold target.

target at coupling = 0.451 − 0.164 = +0.287 mm      (motor HIGH by 0.29 mm, cold)
target slope       = −0.000205 mm/mm = −0.021 mm per 100 mm

Step 4 — turn it into shims. Evaluate the target line at each motor foot:

front foot (x = 250):  0.287 − 0.000205 × 250 = +0.236 mm   → add 0.24 mm shim
rear  foot (x = 850):  0.287 − 0.000205 × 850 = +0.113 mm   → add 0.11 mm shim

Step 5 — sanity-check against tolerance. At 2 950 rpm the acceptable offset is ~0.07 mm. The cold target is 0.287 mm — four times the tolerance, and that is correct. A cold report reading 0.29 mm offset is the passing report here. A cold report reading 0.01 mm is the failure.

Watch the same thing happen in three dimensions: ▶ open the interactive: rotating alignment 3d — drive the temperature slider with "aligned cold" selected and the shafts break apart as they heat; select "cold target set" and they walk into line.

Before you align anything: soft foot and pipe strain

Two site conditions make every number above meaningless.

Soft foot — the machine does not sit flat, so tightening the bolts bends the frame and moves the shaft. Check it with a dial on each foot while you loosen that bolt alone; > 0.05 mm (0.002 in) of movement is a soft foot and must be corrected before alignment, not after. Four kinds worth knowing apart:

Pipe strain masquerading as misalignment. This is the crossover with the nozzle-load topic — piping that exceeds the API 610 allowable distorts the casing, and the distortion reads on the laser as misalignment you then "correct" with shims. You have now shimmed a bent machine.

The test is simple and is written into API 686 practice: put indicators on the coupling, then slacken the suction and discharge flange bolts. If the shaft moves more than 0.05 mm (0.002 in), the pipe is imposing strain — fix the pipe, not the shims. The flange faces should come together parallel and concentric without being pulled, and no bolt should need a lever.

Reverse dial versus laser — and the sag that ruins dial readings

Reverse dial indicator: two brackets, each carrying an indicator reading the rim of the other shaft. Rotate both together, take readings at 0/90/180/270°. Two rim readings at a known separation give you both offset and angularity by similar triangles, and projecting that line onto the foot positions gives the moves directly. It is geometry, and it is free.

Its one lethal error is bar sag: the bracket droops under the indicator's own weight, and the droop reverses between the 12 o'clock and 6 o'clock readings, so it lands entirely in your vertical answer. Sag must be measured — mount the bracket on a rigid pipe, rotate 180°, record the change — and subtracted from every vertical reading. A 0.10 mm sag left in is a 0.10 mm alignment error, which is the whole budget at 3 000 rpm. Face-and-rim methods share the problem; so does any method that needs the bracket to span a long spacer.

Laser: a detector and emitter on each shaft, no mechanical bridge, so no sag. Resolution in micrometres, it computes the feet moves for you, and — the part that matters for this topic — it takes the thermal-growth targets as an input so the display tells you when you have hit the deliberately-offset cold target, not zero. It also does live "move" mode, so you watch the number go to target as you tap the machine across.

Both methods need the same preconditions: soft foot cured, no pipe strain, shafts free to turn together, backlash and axial float controlled, and readings taken at the same metal temperature you assumed in ΔT.

Common pitfalls

Outcome

Open items

Know why, not just what.

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