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12.1 Definitions
12.1.1 Shock
Shock occurs when a force, a position, a velocity, or an acceleration is abruptly modified and creates a
transient state in the system considered. The modification is normally regarded as abrupt if it occurs in
a time period that is short compared with the natural period concerned (AFNOR, 1993). Shock is defined
as a vibratory excitation having a duration between the natural period of the excited mechanical system
and two times that period (Figure 12.1).
12.1.2 Simple (or Perfect) Shock
A shock whose signal can be represented exactly in simple mathematical terms is called a simple
(or perfect) shock. Standards generally specify one of the three following: half-sine (approached by a
versed sine waveform), terminal peak sawtooth, and rectangular shock (approached by a trapezoidal
waveform).
12-2 Vibration and Shock Handbook
© 2005 by Taylor & Francis Group, LLC
12.1.3 Half-Sine Shock
This is a simple shock for which the acceleration –
time curve has the form of a half-period (part
positive or negative) of a sinusoid.
12.1.4 Versed-Sine (or Haversine)
Shock
This is a simple shock for which the acceleration –
time curve has the form of one period of the curve
representative of the function ½1 2 cosð Þ; with this
period starting from the zero value of this function.
It is thus a signal ranging between two minima of a
sine wave.
12.1.5 Terminal Peak Sawtooth
Shock or Final Peak Sawtooth Shock
This is a simple shock for which the acceleration – time curve has the shape of a triangle, where
acceleration increases linearly up to a maximum value and then instantly decreases to zero.
12.1.6 Rectangular Shock
This is a simple shock for which the acceleration – time curve increases instantaneously up to a given
value, remains constant throughout the signal, and decreases instantaneously to zero. In practice, what is
carried out are trapezoidal shocks.
12.1.6.1 Trapezoidal Shock
This is a simple shock for which the acceleration – time curve grows linearly up to a given value, remains
constant during a certain time period, after which it decreases linearly to zero.
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