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6<br />

Effective Weight<br />

Effective weight is an important factor in selecting shock<br />

absorbers . A shock absorber “sees” the impact of an<br />

object in terms of weight and velocity only; it does not<br />

”see” any propelling force . The effective weight can<br />

be thought of as the weight that the shock absorber<br />

“sees” on impact . Effective weight includes the effect<br />

of the propelling force on the performance of the shock<br />

absorber .<br />

Failing to consider the effective weight may result in<br />

improper selection and poor performance of the shock<br />

absorber . Under extreme conditions, an effective weight<br />

that is too low may result in high forces at the start of<br />

stroke (high on-set force) . However, an effective weight<br />

that is too high for the shock absorber may cause high<br />

forces at the end of stroke (high set-down force) .<br />

Consider the following examples:<br />

1 .) A 5 lb (2 .27 kg) weight travelling at 25 ft/sec (7 .62<br />

m/s) has 625 lbs (71 Nm) of kinetic energy (figure A) .<br />

On this basis alone, a MA 3325 would be selected .<br />

However, because there is no propelling force, the<br />

calculated effective weight is five pounds – which is<br />

below the effective weight range of the standard MA<br />

3325 . This is a high on-set force at the start of the<br />

stroke (Figure B) . The solution is to use a speciallyorificed<br />

shock absorber to handle the load .<br />

2 .) A weight of 50 lbs (22 .68 kg) has an impact velocity<br />

of 0 .5 ft/sec (0 .15 m/s) with a propelling force of<br />

800 lbs (111N) (Figure C) . The total impact energy<br />

is 802 .5 inch-pounds . Again, a MA 3325 would be<br />

selected based just on the energy . The effective<br />

weight is calculated to be 16,050 pounds (7,280<br />

kg) . This is well above the range of the standard MA<br />

3325 . If this shock absorber is used, high-set-down<br />

forces will result (Figure D) . In this case, the solution<br />

is to use a ML 3325, which is designed to work in<br />

low-velocity, high-effective weight applications .<br />

Computer-Aided Simulation<br />

By combining application data with a shock absorbers<br />

design parameters, ACE engineers can create a picture<br />

of how the shock will perform when impacted by the<br />

application load . Peak reaction force, peak deceleration<br />

(G’s), time through stroke, and velocity decay are<br />

identified with extreme accuracy . The user benefits by<br />

having the guesswork taken out of sizing decisions and<br />

by knowing before installation how his shock problem<br />

will be solved .<br />

Simulation is also used to maximize the performance<br />

of ACE adjustable models by predicting the ideal<br />

adjustment setting for a particular group of conditions .<br />

By using simulation software during product<br />

development stages, ACE has maximized the<br />

performance of its entire line of deceleration devices for<br />

over two decades .<br />

Figure A<br />

Figure B<br />

ACE Controls <strong>Inc</strong>. · 800-521-3320 · (248) 476-0213 · Fax (248) 476-2470 · www.acecontrols.com · email: shocks@acecontrols.com<br />

Force<br />

Figure C<br />

800 lbs<br />

(111 N)<br />

Figure D<br />

Force<br />

Low Effective Weight<br />

25 ft/sec (7.62 m/s)<br />

5 lbs<br />

(2. 27 kg)<br />

Low Effective Weight<br />

Stroke<br />

High Effective Weight<br />

Example 2: Orifice Area Is<br />

Too Large (High Set-Down)<br />

Linear<br />

Deceleration<br />

Example 1: Orifice Area Is<br />

Too Small (High On-Set)<br />

High Effective Weight<br />

0.5 f/s (0.15 m/s)<br />

50 lbs<br />

(22.68 kg)<br />

<strong>Air</strong>-<strong>Oil</strong> <strong>Systems</strong>, <strong>Inc</strong>. www.airoil.com<br />

Stroke<br />

Linear<br />

Deceleration

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