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CATALOGUE

GENERAL CATALOGUE - Unimec

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The ambient factor f a<br />

By means of the following table it is possible to calculate the f a factor according to the operation conditions.<br />

Type of load Daily working hours [h] 3 8 24<br />

Light shocks, few insertions, regular movements 0,8 1 1,2<br />

Medium shocks, frequent insertions, regular movements 1 1,2 1,5<br />

High shocks, many insertions, irregular movements 1,2 1,8 2,4<br />

The duration factor f d<br />

The duration factor f d is calculated as a function of the theoretical foreseen lifetime (expressed in hours)<br />

Duration factor f d<br />

2,2<br />

2<br />

1,8<br />

1,6<br />

1,4<br />

1,2<br />

1<br />

0,8<br />

0,6<br />

0,4<br />

1000 10000 100000<br />

foreseen lifetime [h]<br />

D – THE POWER TABLES AND THE EQUIVALENT POWER<br />

Once the equivalent load C e , has been calculated, it is possible to calculate the equivalent output power necessary<br />

for the screw jack-ball spindle system as P e =C e •v, where v is the load’s linear translation speed. Dividing the<br />

equivalent power by the running efficiency η a of the ball spindle (which can be taken from the manufacturer<br />

catalogue) e by the screw jack running efficiency η k the screw jack input equivalent power P ei can be obtained.The<br />

preliminary choice of the K series screw jack is effected by means of the table powers (on page 132), by choosing<br />

the size which, upon a certain rotation speed (input or output) shows an input power higher than the P ei .<br />

Attention: the equivalent power is NOT the power requested by the single screw jack, unless the three correction<br />

factors f g ,f d e f a have a unit value.<br />

E – THE INERTIA POWER<br />

In case of high accelerations and decelerations it is necessary to calculate the inertia power P J . It is the power<br />

necessary to support the inertia forces and torques opposed by the system in presence of a speed change.<br />

First the designer should calculate the system inertia downstream of the screw jack J v by reducing them to<br />

the hollow shaft.The J v inertias are the system inertias (typically masses) as well as the ball spindle and lead<br />

nut inertias.<br />

After that, it is necessary to add the inertia of the screw jack J k , obtainable from the tables below, in order<br />

to have the value of the total inertia J. We remind that inertia is expressed by [kg•m 2 ].<br />

Sizes K 59 K88 K117<br />

J k screw jack inertia [Kgm 2 ] 0,0040608 0,0254982 0,0798326<br />

Given ω v the input rotation speed and α v the input angular speed the inertia torque applied is equal to J•ω v<br />

and the respective inertia power P J is equal to J•ω v •α v. If the time changes of the input speed ω v can be<br />

referred to one of the linear of sinusoidal schemes below, where A is the maximum speed in [rpm] and B is<br />

the cycle frequency in [Hz], it is possible to simplify the inertia power calculation in [kW], by identifying A<br />

and B parameters and by calculating:<br />

P J =<br />

2•J•A 2 •B<br />

91188<br />

126<br />

The power P J is to be added to the equivalent power P ei and a verification on the correctness of the chosen<br />

size must be carried out by means of the descriptive tables. In case the size is not correct it is necessary to<br />

change it and to effect new verifications.

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