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oscillating line - Kendrion Binder

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In<strong>line</strong> vibrators<br />

Type OMW516002 (Fig. 3)<br />

Armature plate<br />

the technical background<br />

In the in<strong>line</strong> vibrator the solenoid and its energisation coil<br />

are fixed to a base. Mounted above this is the armature<br />

plate, with pole faces separated by an air gap and parallel<br />

with those of the solenoid. Leaf springs positioned at an<br />

angle (approx. 20°) connect the armature plate to the<br />

base. An attracting force prevails between the armature<br />

and solenoid. When an AC voltage is applied to the energisation<br />

coil, the force effect of the electromagnetic alternating<br />

field is superimposed on the force effect of the permanent<br />

magnet (type OMW516004). The frequency of<br />

the resulting force matches the frequency of the AC<br />

voltage applied, which moves the armature in the same<br />

rhythm. The angled arrangement of the leaf springs<br />

causes the armature plate, and the vibrating conveyor<br />

attached to this, to perform a curving oscillatory movement<br />

and therefore convey loose materials in one<br />

direction.<br />

In the case of larger or relatively wide vibrating conveyors<br />

it is better to use several smaller in<strong>line</strong> vibrators rather<br />

than a single large one.<br />

Curved motion vibrator<br />

Type OAB513001 (Fig. 4)<br />

Sprung component<br />

Unsprung component<br />

Leaf spring<br />

Base<br />

Solenoid<br />

(energisation coil + frame)<br />

The solenoid of the curved motion vibrator, fixed rigidly to<br />

the base of the device, consists of two annular shells which<br />

enclose the energisation coil. The armature, comprising<br />

two annular permanent magnets with opposite poles<br />

arranged axially and two pole discs in each case, is located<br />

between leaf springs fixed on opposite sides of the<br />

base of the device. The system is pre-magnetised by the<br />

two permanent magnets. In the stationary condition one<br />

annular pole of the solenoid is located between each pair<br />

of pole discs of the armature. When an AC voltage is applied<br />

to the energisation coil, the unlike poles of armature<br />

and solenoid attract. The frequency of the curving armature<br />

movement matches the frequency of the AC voltage<br />

applied.<br />

The curved motion vibrator can be used as a vibratory<br />

drive and, fitted with an additional weight on the<br />

armature shaft, as a vibrator.<br />

Fig. 4: Curved motion vibrator (OAB513001)<br />

1 Solenoid<br />

2 Energisation coil<br />

3 Armature<br />

4 Permanent magnet<br />

5 Spring<br />

6 Base<br />

Vibrating solenoids<br />

OAC... series (Fig. 5)<br />

Sprung load<br />

Sprung<br />

component<br />

Unsprung<br />

load<br />

Unsprung<br />

component<br />

Vibrating<br />

solenoid<br />

Vibrating solenoids are primarily incorporated in<br />

spring–mass systems that constantly exploit the<br />

resonant frequency proximity of the entire vibrating<br />

system (drive and sprung device). The vibrating<br />

solenoid generates directional, <strong>line</strong>ar oscillations in<br />

the sprung device.<br />

Coil and bobbin are encapsulated in casting resin.<br />

They are therefore not susceptible to moisture and<br />

dust and thus suitable for rough conditions.<br />

The direction of the oscillations is achieved by the<br />

geometrical arrangement of the springs, which means<br />

that, for conveying, a certain <strong>oscillating</strong> angle is<br />

always necessary. The effective amplitude here corresponds<br />

to twice the amplitude of the <strong>oscillating</strong> frequency<br />

of the whole system. Vibrating solenoids can<br />

be infinitely regulated via the operating voltage. They<br />

reach the full conveying power immediately after<br />

being switched on and there are no troublesome imbalance<br />

effects upon starting and stopping. This is<br />

particularly important for metering, packaging, etc.<br />

www.kendrionmt.com<br />

Armature plate<br />

∆L = air gap<br />

Tuning<br />

a) Explanation of symbols used<br />

fo fa = natural frequency<br />

= operating frequency<br />

= mains frequency<br />

Hz<br />

Hz<br />

c = spring constant N/mm<br />

cs = spring constant of rubber<br />

buffer in shearing direction N/mm<br />

d = spring thickness mm<br />

mF = weight of unsprung component<br />

mN of oscillator with 2 eccentric weights kg<br />

= weight of sprung component<br />

of oscillator with 2 eccentric weights kg<br />

mR = resultant weight<br />

mR =<br />

m .<br />

N mF<br />

mN + mF kg<br />

sF = vibration amplitude of unsprung mm<br />

component<br />

sN = vibration amplitude of sprung<br />

component<br />

mm<br />

s = total vibration amplitude<br />

s = sF + sN mm<br />

a = air gap mm<br />

1N = 0.102 kg<br />

b) General<br />

All vibrators must be detuned for reasons of amplitude<br />

stability, i.e. the natural frequency fo of the device must not<br />

be equal to the operating frequency fa. As a rule, the<br />

detuning amounts to 10-20%. All vibrators used for<br />

conveying purposes must be tuned subcritically, i.e. the<br />

natural frequency fo of the system must be greater than<br />

the operating frequency fa. The resonance curve is damped by the loose materials<br />

being conveyed (Fig. 6). Both subcritical and supercritical<br />

tuning results in the amplitude being reduced from a (A) to<br />

b (B).<br />

Subcritical tuning<br />

Damped curve<br />

1<br />

Supercritical<br />

tuning<br />

Fig. 6: Vibration amplitude s plotted against the ratio of<br />

operating frequency fa to natural frequency f0. Notes:<br />

- to DIN VDE 0580 (July 2000) ICS29.020.53.020.01<br />

(valid as manufacturer’s Declaration of Conformity)<br />

- directives 98/37/EC and 73/23/EEC<br />

- CCC certificate for China not required<br />

We reserve the right to make changes to the<br />

product design.<br />

5

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