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Design Guide - Solvay Plastics

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Figure 78: Cantilever Type Snap Fit<br />

Figure 79: Cantilever Beam - Concentrated Load<br />

at Free End<br />

F<br />

b<br />

d<br />

L<br />

Y<br />

L<br />

Y<br />

Molded-In Threads<br />

One of the benefits of using plastic materials instead<br />

of metals is the ability to mold thread forms directly<br />

into the part. This eliminates the secondary machining<br />

operations needed with metal parts to form the threads.<br />

molded-in threads can be either external or internal. In<br />

the case of internal threads, some type of unscrewing<br />

or collapsible core is required. External threads can<br />

be formed more easily if the parting line of the mold is<br />

perpendicular to the thread.<br />

<strong>Design</strong>ing with Snap Fits<br />

The use of snap fits in plastics is very prevalent. All snap<br />

fit designs require the plastic to flex like a cantilever<br />

spring as it moves past an interference that is designed<br />

on the mating part. Once the flexible arm moves past<br />

the interference, it returns to its normal unflexed,<br />

unstressed position. Usually a step or protrusion has<br />

been designed on the cantilever that engages and locks<br />

into the mating part, creating a simple assembly method<br />

without additional parts. This is shown in Figure 78.<br />

Each cantilever arm must deflect a distance “Y” in order<br />

to be inserted. The key to proper snap design is to not<br />

exceed the strain/stress limits of the material being<br />

used. A snap fit design that has been used for a ductile,<br />

low modulus plastic will probably not be suitable for a<br />

highly reinforced, very rigid plastic.<br />

For rigid materials, the length of the cantilever may be<br />

increased or the interference deflection "Y" reduced.<br />

Adding a "stop" can prevent over deflection of the<br />

cantilever during assembly.<br />

Straight Cantilever Beam Equation<br />

The relationship between maximum deflection and<br />

strain for a straight cantilevered beam was calculated as<br />

follows: From Table 46, the cantilever beam was chosen<br />

and the drawing is repeated as Figure 79. The maximum<br />

stress, is given by the following:<br />

σ = FL<br />

Z<br />

Since this beam has a rectangular cross section,<br />

Z =<br />

I =<br />

Therefore:<br />

bd 2<br />

6<br />

bd 3<br />

12<br />

σ = FLd<br />

2I<br />

and<br />

The deflection of the beam, Y, is given by:<br />

Y =<br />

FL 3<br />

3EI<br />

76 Amodel ® PPA <strong>Design</strong> <strong>Guide</strong><br />

www.<strong>Solvay</strong>SpecialtyPolymers.com

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