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124 Smart Technologies <strong>for</strong> Safety Engineering<br />

Table 4.1 Comparison and summary of impact load identification procedures (F denotes <strong>for</strong>ce; aA<br />

accelerometer (falling body); aB accelerometer (piston rod); p pressure; b photo switch)<br />

Solution map Force and acceleration Momentum conservation<br />

Sensors F F, aB F, aA p, b F, aA<br />

Solution maps 2 1 — 1 1<br />

Operation time [ms] 100–110 80 5/80 5 5<br />

Accuracy (mass) 5 % 5 % 10 % / 5 % 15 % 5 %<br />

Accuracy (velocity) 5 % 10 % — Measured 3 %<br />

In general, the identification of both impact parameters based on the characteristics of the<br />

first impulse is possible relatively quickly, already 5 ms from the very beginning of the impact<br />

process. There<strong>for</strong>e, the approach can operate in real-time.<br />

4.1.7 Comparison of Approaches<br />

A real-time impact mass and velocity estimation is extremely difficult with only one sensor.<br />

Much better results can be obtained with two sensors; in the tested case good results were<br />

obtained with a combination of an accelerometer and a <strong>for</strong>ce sensor. However, the location of<br />

the accelerometer is very important: fixing the accelerometer to the falling body allows precise<br />

mass identification in a short time after the impact, while with the accelerometer placed on the<br />

impacted body the identification is far more difficult and only feasible after a longer period.<br />

There<strong>for</strong>e, mass determination of the impacting body is possible in a short time and with high<br />

accuracy only when one of the sensors is fixed to the impacting object or when the parameters<br />

of its movement are directly measured.<br />

For velocity identification on the basis of acceleration, the initial condition is needed. Thus<br />

in the case of the analysed structure, the velocity identification was feasible only when a joint<br />

movement of the piston rod and the falling mass was observed.<br />

The tested algorithms are summarized and compared in Table 4.1.<br />

4.2 Observer Technique <strong>for</strong> On-Line Load Monitoring<br />

The concept of the observer was introduced by Luenberger in the beginning of 1970s [7].<br />

Originally it was devoted to feedback control systems, since first multivariable control strategies<br />

had assumed that the whole state vector was available <strong>for</strong> feedback [8]. However, from the<br />

practical point of view, it was not always possible to measure all the components of the state. The<br />

state observer, which allows the state vector to be estimated based on only a few measurements,<br />

encountered great interest among the control <strong>engineering</strong> community [9,10]. Another important<br />

issue connected with real-life measurements was noise corrupting the measured signal. With<br />

the aid of the theory of stochastic processes, this problem was solved by Rudolf Kalman and<br />

nowadays his stochastic estimator is frequently called the Kalman filter [11].<br />

Currently, a lot of attention is paid to simultaneous reconstruction of both the state and the<br />

inputs in linear and nonlinear systems [12–15]. In the case of a mechanical system, the state<br />

can be represented by displacements and velocities, while the inputs can be external <strong>for</strong>ces.

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