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Adaptive Impact Absorption 211<br />

Deceleration [g]<br />

10<br />

5<br />

0<br />

Experiment<br />

Simulation<br />

0 40 80 120<br />

Time [ms]<br />

Figure 5.57 Comparison of FE and test results: impacting mass deceleration versus time <strong>for</strong> the active<br />

mode [43]<br />

deflagration chamber (Figure 5.55). Rapidly growing pressure acting on the pyroconnection’s<br />

piston broke the sheared pin made of soldering alloy, causing unlocking of the absorber’s<br />

members. A battery of capacitors, pre-charged to 311 V, on the triggering signal was rapidly<br />

discharged through the initiator wire. The initiator wire vaporized in a time shorter than 250 μs<br />

after receiving the signal coming from the real-time control system. The initiation process was<br />

controlled by the electrical control circuit, which was optically separated from the controller.<br />

The silicon-controlled rectifiers (SCR) were used <strong>for</strong> fast response switching of the initiating<br />

current. The acceleration sensor measured the deceleration of the impacting mass.<br />

During the high-energy mode test, all pyroconnections remained locked through the crushing<br />

time (Figure 5.56, left). The test of the low-energy mode (Figure 5.56, right) was conducted<br />

with the same initial conditions as the passive one. A photocell activated by the dropping head of<br />

the hammer sent the signal to the control system. When the impulse was received by the control<br />

system, the initiation circuit was triggered with a pre-set time offset, causing deflagration of<br />

the powder, opening of the connections and disconnection of the additional members. The<br />

average delay time between the initiation and explosion, due to statistical dispersion, was<br />

around 3–4 ms. A comparison of FE and test results is given in Figure 5.57.<br />

The demonstrated example shows another possible direction of the AIA system development,<br />

which may be applied in wide range of applications.<br />

References<br />

1. J. Holnicki-Szulc, P. Paw̷lowski and M. Wik̷lo, High-per<strong>for</strong>mance impact absorbing materials – the<br />

concept, design tools and applications, Smart Materials and Structures, 12(3), 2003, 461–467.<br />

2. J. Holnicki-Szulc and C. A. Mota Soares, Advances in Smart Technologies in Structural Engineering,<br />

Vol. 1, Computational Methods in Applied Sciences Series, Springer, New York, 2004.<br />

3. N. Jones and T. Wierzbicki, Structural Crashworthiness. Butterworths, London, 1983.<br />

4. N. Jones and T. Wierzbicki, Structural Failure, John Wiley & Sons, Inc., New York, 1989.<br />

5. N. Jones and T. Wierzbicki, Structural Crashworthiness and Failure, Elsevier Applied Science,<br />

1993.<br />

6. C. M. Harris and A. G. Piersol, Harris’ Shock and Vibration Handbook, McGraw-Hill, 2002.<br />

7. R. Grybos, Teoria uderzenia w dyskretnych uk̷ladach mechanicznych (in Polish), PWN, 1969.

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