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General Design Principles for DuPont Engineering Polymers - Module

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If one part is only vibrated at twice the frequency, the<br />

acceleration and deceleration <strong>for</strong>ces are four times<br />

higher and would have to be compensated <strong>for</strong> by<br />

means of an additional and adjustable device. The<br />

whole gear box would there<strong>for</strong>e be much heavier and<br />

more expensive <strong>for</strong> a machine having the same<br />

capacity. In addition, it has been shown empirically<br />

that it is easier to obtain a good, tight joint if both<br />

parts are vibrating.<br />

Figure 11.73<br />

W<br />

W<br />

Y = 0.635 W<br />

Y<br />

Y<br />

1 revolution<br />

2 Y = 1.27 W<br />

2 Y<br />

W = maximum velocity of each part<br />

Y = average velocity of each part<br />

2 W<br />

Welding Conditions<br />

In order to reach the melting point of the material, two<br />

parts must be pressed together and vibrated at a<br />

certain frequency and amplitude. These conditions can<br />

be defined as a PV value, where P is the specific joint<br />

pressure in MPa and V the surface velocity in m/s.<br />

The two eccentrics generate a sinusoidal velocity<br />

curve as shown in Figure 11.73. Since they move in<br />

opposite directions, the maximum relative velocity<br />

of one part against the other is 2 W. The resulting<br />

relative velocity is there<strong>for</strong>e 1.27 times the maximum<br />

value W.<br />

Example: A machine welding acetal according to<br />

Figure 11.71 has an eccentric distance f of 3 mm and<br />

runs at a speed of 5000 rpm. The circumferential<br />

velocity is there<strong>for</strong>e:<br />

V = f × π × n = 0.003 m × π × 5000 = 0.78 m/s<br />

60<br />

This equals the maximum velocity W in Figure 11.73.<br />

The average relative velocity of one part against the<br />

other would then be:<br />

1.27 × 0.78 = 1 m/s<br />

113<br />

At a specific joint pressure of 3 MPa, the resulting PV<br />

value becomes:<br />

3 × 1 = 3 MPa × m/s<br />

As the generated heat is also a function of the coefficient<br />

of friction, the above PV value must be related to<br />

the materials being welded. Glass-rein<strong>for</strong>ced polyamide<br />

<strong>for</strong> instance has been welded successfully at a<br />

PV value of 1.3. It would there<strong>for</strong>e appear that a<br />

machine which is supposed to weld various materials<br />

and part sizes should be provided with adjustable<br />

pressure, speed and amplitude. Once the best working<br />

conditions are determined <strong>for</strong> a given part, the production<br />

machine would, however, not require any adjustments,<br />

except <strong>for</strong> the pressure.<br />

Weld time is a product of velocity, pressure and<br />

amplitude. Experience has shown, however, that<br />

above a certain pressure, joint strength tends to<br />

decrease, possibly due to squeezing out of the molten<br />

resin. On the other hand, there are certain limits with<br />

regard to the resulting mechanical load on the gear<br />

box. Thus, doubling the speed produces four times<br />

higher acceleration <strong>for</strong>ces of the vibrating masses.<br />

Extensive tests have proven that a frequency of about<br />

100 Hz is very convenient <strong>for</strong> small and medium size<br />

parts whereas larger, heavy parts are welded at a<br />

frequency of 70–80 Hz.<br />

However, successful joints <strong>for</strong> big parts have also<br />

been designed, using frequencies up to 250 Hz, see<br />

also Figure 11.76D.<br />

On linear machines, the distance of the two eccentrics<br />

(f in Figure 11.71) should be adjusted in order to<br />

obtain a relative motion of about 0.9 × joint width, as<br />

shown in Figure 11.74.<br />

The specific surface pressure giving the highest joint<br />

strength must be determined by testing. As a basic rule<br />

it can be said that a machine should be capable of<br />

producing approximately 4 MPa of pressure on the<br />

surface to be welded.<br />

Figure 11.74 Relative motion—joint width<br />

W<br />

0.9 W

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