beebe - balancing by timed oscillation (aus)

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BALANCING USING YOUR MOBILE PHONE By Ray Beebe Unbalance is one of the most common causes of high vibration in machines. If the largest vibration component in the spectra is at 1X (i.e. at the frequency corresponding to rotation speed) then unbalance is the likely cause. Balancing is therefore a regular maintenance activity in many workplaces. Ray Beebe explains a method that has been successfully used on rotors large and small, with the only instrumentation required for balancing being the stopwatch feature of a mobile phone. It is assumed that the severity of vibration has been assessed as unacceptable according to sources such as the relevant part of ISO 10816 (Ref 1). Even if a machine’s vibration meets such criteria, it may be causing annoying vibration of adjacent parts. Looseness is another of the most common causes, and a check of foundation tightness is recommended before proceeding to balancing. If the unbalance is due to deposition on the rotor, such as with fans handling dirty gas, the rotor should be cleaned. In cases where a deposit is difficult or expensive to remove, it may be expedient to balance out its effect until a more convenient time for cleaning. The Timed Oscillation Method This method has been used successfully for short rotors such as overhung fans up to 2m diameter, and for pump impellers. It has also been used on smaller fans with two bearings that are nearer to what are considered “long” rotors. The rotor must be in rolling element bearings, or set up on a mandrel and parallel ways, and not be affected by crosswinds. For field balancing, the usual safety precautions for opening any machine must of course be taken so that the machine cannot be switched on while the work is in progress. I do not know the source of the method, but I learnt it in my first job at a power station in the 1960s. Published in Ref 2, the equation is derived from the theory of the compound pendulum. Mark numbers around the rotor, evenly spaced. For bladed rotors, mark at the blades. Choose a swing mass to fasten (by clamp or magnet) on the rotor, to give to-and-fro oscillation time of about 20 seconds. (This gives some allowance for reaction time in operating the stopwatch feature of your mobile phone) With the swing mass fixed to the rotor at Position 1, turn the rotor so that the mass is at one horizontal position and stationary. Release the rotor and let it swing freely under its own inertia do not push it in any way. Time the to-and-fro oscillation from the horizontal position. The left part of the sketch below illustrates the process. Turn the rotor so that the mass is at the horizontal position on the other side, and repeat. Calculate the mean time of swing for this position, and plot on a graph of time against position as shown in the sketch. With position numbers evenly spaced, one position appears twice - at the start and the end of the position axis. Move the swing mass to Position 2, etc. and repeat the process. Connect the graphed points with a smooth sine wave shape, and read off the maximum and minimum times of swing: T and t.

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Page 1: Beebe - Balancing by timed oscillation (AUS)

BALANCING USING YOUR MOBILE PHONE

By Ray Beebe

Unbalance is one of the most common causes of high vibration in machines. If the

largest vibration component in the spectra is at 1X (i.e. at the frequency

corresponding to rotation speed) then unbalance is the likely cause. Balancing is

therefore a regular maintenance activity in many workplaces. Ray Beebe explains a

method that has been successfully used on rotors large and small, with the only

instrumentation required for balancing being the stopwatch feature of a mobile

phone.

It is assumed that the severity of vibration has been assessed as unacceptable according to sources such as

the relevant part of ISO 10816 (Ref 1). Even if a machine’s vibration meets such criteria, it may be

causing annoying vibration of adjacent parts.

Looseness is another of the most common causes, and a check of foundation tightness is recommended

before proceeding to balancing. If the unbalance is due to deposition on the rotor, such as with fans

handling dirty gas, the rotor should be cleaned. In cases where a deposit is difficult or expensive to

remove, it may be expedient to balance out its effect until a more convenient time for cleaning.

The Timed Oscillation Method This method has been used successfully for short rotors such as overhung fans up to 2m diameter, and for pump impellers. It has also been used on smaller fans with two bearings that are nearer to what are considered “long” rotors. The rotor must be in rolling element bearings, or set up on a mandrel and parallel ways, and not be affected by crosswinds. For field balancing, the usual safety precautions for opening any machine must of course be taken so that the machine cannot be switched on while the work is in progress. I do not know the source of the method, but I learnt it in my first job at a power station in the 1960s. Published in Ref 2, the equation is derived from the theory of the compound pendulum.

Mark numbers around the rotor, evenly spaced. For bladed rotors, mark at the blades.

Choose a swing mass to fasten (by clamp or magnet) on the rotor, to give to-and-fro oscillation time of about 20 seconds. (This gives some allowance for reaction time in operating the stopwatch feature of your mobile phone)

With the swing mass fixed to the rotor at Position 1, turn the rotor so that the mass is at one

horizontal position and stationary. Release the rotor and let it swing freely under its own inertia – do not push it in any way.

Time the to-and-fro oscillation from the horizontal position. The left part of the sketch below

illustrates the process.

Turn the rotor so that the mass is at the horizontal position on the other side, and repeat.

Calculate the mean time of swing for this position, and plot on a graph of time against position as shown in the sketch. With position numbers evenly spaced, one position appears twice - at the start and the end of the position axis.

Move the swing mass to Position 2, etc. and repeat the process.

Connect the graphed points with a smooth sine wave shape, and read off the maximum and

minimum times of swing: T and t.

Page 2: Beebe - Balancing by timed oscillation (AUS)

Calculate the size of balance mass required from:

Balance mass = Swing mass × 22

22

tT

tT

Make a balance mass, and fix it on the rotor at position of maximum swing time. The fixing

must of course be sufficiently strong not to allow the mass to fly off at operating speed. If

welded, allow for the mass of the weld.

o If the correction is to be made by removing mass from the rotor, remove it from the

position of minimum swing.

o If the correction mass is at a different radius to that of the swing mass, then calculate the

mass size to achieve the same moment (i.e. Mass × Radius).

If required, verify the result by repeating the swing test for three spaced points.

Application to balance pump impellers

The method was developed and used for each impeller of a high-speed 10-stage pump of the ring-section

design (where each stage impeller is assembled in turn with its matching stationary section). We clamped

parallel ways to the bed of a milling machine. A mandrel was made to suit the impeller and a pot magnet

used as the swing magnet.

The correction was made on the adjacent milling machine using an end cutter. A table was calculated

and drawn up giving the depth of cut required in each case. The position was marked clearly on the

impeller, and it was passed to the machinist who cut the required mass from the back shroud.

The method gave satisfactory results. At the time, the only balancing machine available could only hold

the total rotor assembly, and corrections would be made on each of the end impellers. Arguably, the

impeller-by-impeller method gave a more satisfactory result.

Balancing by trial and error Another method that may be satisfactory does not require any instrumentation. A story will illustrate the method.

Among the cars that I have owned was a second-hand 1971 Ford Falcon (in-line 6 cylinder 4 litre engine). It came with an after-market twin extractor exhaust system. This gave a “boy racer” burble, and the salesman explained that it was the cause of severe vibration of the whole car that was evident at around 90 km/h.

I tolerated this for some time before deciding that with my growing knowledge of vibration problem solving, and fresh from solving a pump problem, I should be able to fix it. With the bonnet up, I revved the engine, expecting to see the exhaust pipes shake about when the critical speed range was reached. To

Page 3: Beebe - Balancing by timed oscillation (AUS)

my surprise, they did not move at all from an equilibrium position. Then I placed my hand on the alternator and was horrified to feel it shaken off by its rough vibration! I should have figured this out much earlier, because the alternator support bracket had been repaired by brazing, and I had replaced it with a new one. I removed the alternator, leaving the rotor in its end casing bearing. When spun by hand and allowed to come to rest, it settled at the same angular position each time. So, I drilled holes in this “heavy” pole face until the spin test showed the position at rest to vary each time. On reassembling and back in the car, the vibration no longer occurred. This alternator must have slipped through manufacturing QC unnoticed. (When telling this story, I usually leave out the bit about having to ask our instrument workshop people to repair the screw thread that I had mangled just a little!) Methods of balancing This table outlines the several methods available.

Situation Method Equipment needed Comments

Rotor out of machine Balancing machine Balancing machine -usually done

by an external service

Refer ISO 1940/1-1986(E)

for criteria

Timed oscillation

(single plane)

Parallel ways, rotor in mandrel.

Stop watch. Swing mass (e.g. pot

magnet for small rotors).

Systematic method. Can use on short

and some longer rotors.

Trial & error (single

plane)

Parallel ways, rotor in mandrel.

Swing masses of various sizes.

Sometimes cost-effective.

Rotor in machine

("field", "in situ")

Off-speed

Timed oscillation

Trial & error

Rotor must be in anti-friction

bearings

See above

On-speed Single plane

(sometimes called

“static” balancing)

Vibration 1X and phase angle

measurement

For "short" rotors. 3 runs. Can do in

one shot with past history data.

Vibration measurement, no phase

angle

The “4 Runs” method (or less, with

50% chance of correct position for

balance weight). Assumes that the

vibration is predominantly 1X. (Ref

2).

Two planes (sometimes

called “dynamic

balancing”)

Vibration 1X and phase angle at

each end bearing

For "long" rotors.

4 runs using "Influence coefficients"

method. (Ref 2).

3 runs in some cases, using

"components" method where “static”

(i.e. in-phase) and “dynamic” (i.e.

anti-phase) components are treated

separately (Ref 2).

Multiple planes (but in

field on a rotor often

only two are

accessible)

Vibration and phase angles at each

end bearing

Modal balancing for flexible rotors,

rather like components method.

Computer system is usual.

Some vibration data collector/analyser devices can have capability for field balancing, using a phase angle reference. I think that the earlier method where a vector diagram is drawn has the advantage of visualising the process, step by step.

References

1. ISO 10816 Mechanical vibration – Evaluation of machine vibration by measurements on non-rotating parts.

(Several parts for specific machine types)

2. Beebe, Ray S Machine condition monitoring, MCM Consultants, 2009 reprint. ISBN 0646250884