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13

Electricity

+

Control

JULY 2017

<<Author>>

Glyn Craig is a

director of Techlyn.

glyn@techlyn.co.za

+27 (0) 11 835 1174

Force = mass X acceleration. Note the use of

mass

and not

weight

. Therefore, in a weightless

situation the above equation will apply. The equiv-

alent electrical analogue is impedance. Rotational

systems have

rotary inertia

.

This is easily calculated if the dimensions of the

object and its density are known. The SI (Systeme

International) unit for inertia is metre.kilogram

2

although kg.cm

2

is commonly used as results in

more easily visualised numbers.

1 kg.m

2

= 10 000 kg.cm

2

A 3,4 inch stepper motor rotor is 1,2 kg.cm

2

.

The inertia of the load needs to bematched to the driv-

ing motor’s rotor inertia. Conventional wisdom states

that a mismatch up to 10:1 is permissible. Note, that

the reflected inertia is reduced by the square of the

gearbox ratio. Thus, a 3:1 gearbox will reduce the re-

flected load inertia by 3 squared, which is then 9:1.

This is the same as a transformer which changes load

impedance by the square of the turns ratio.

Worked example

We conclude with a real life example.

A laboratory carousel carries 24 test tubes and has to

position them one by one beneath a dosing needle.

The following information is available

Carousel dimensions:

• 300 mm diameter

• 10 mm thickness

• Material – aluminium

Friction of carousel: 0,1 Nm

Time available for move: 1 s

Positioning accuracy: 0,1

0

Move times are moderate, therefore a stepper

solution will be used.

Step 1:

Calculate the load inertia:

We use the empirical formula for an aluminium disc

J = D

4

L/3 800

= 30

4

X 1/3 800

= 213 kg.cm

2

Where:

J = inertia in kg.cm

2

D = diameter (cm)

L = thickness (cm)

This value far exceeds the inertia of moderately

priced motors.

Step 2:

Choose a possible speed reducer:

• The required positioning accuracy is 0,1

0

(i.e. 360/0,1 = 3 600 increments per revolution)

• If we base the ratio on a motor resolution of

200 steps per rev. (1,8

0

), the required ratio =

3 600/200 = 18:1. This is a popular worm gear-

box ratio

• The motor can then be half stepped (400 steps/

rev) or quarter stepped (800 steps/rev) to give

additional smoothness and correct small errors

• Assuming a maximum motor speed of 10 rev/

sec (600 rpm), the table will rotate at 600/18 =

33,3 rpm which is more than fast enough

Step 3:

Select a suitable motor. The load inertia is

reduced by the square of the ratio

.

Reflected inertia = 213/18

2

= 0,66 kg.cm

2

This looks like an encouraging number. Referring

to a motor catalogue reveals that a single stack

34 frame motor has a rotor inertia 0f 0,6 kg.cm

2

.

This is a popular, moderately priced motor.

Available torque is 1,2 Nm, which is more than ad-

equate.

The reflected inertia should not exceed the

motor rotor inertia of a stepper by more than

about 10:1, as this gives rise to resonance prob-

lems.

In this case, the worm gearbox will also have

high internal friction, and this slightly oversize motor

will ensure that there is adequate torque available.

Very often an iterative process is needed

where steps 2 and 3 above are repeated until a

satisfactory compromise is reached.

Conclusion

After all this we see that speed reducer selection

is not a simple process.

At the forefront

of successful

designs lies

the correct

specification of

the mechanical

components

used.

DRIVES, MOTORS + SWITCHGEAR