Unit 6 - Vibration Control Flashcards
Possible effects of mechanical vibrations in structures are:-
- Damage to the structure. This only results from gross vibrations such as result from earthquakes.
- Disturbance of the occupants. The degree of movement may be sight but can create unease especially when the person is lying down. Moreover windows and fitments may rattle which adds to unease and fears about safety.
- Vibrations of partitions creating sound within rooms. Rooms that require particularly low noise levels may need special treatment.
- Vibrations may upset sensitive operations such as the manufacturing of micro components as found in computer chips, or optical lens manufacture.
What does vibration control measures aim for
Vibration control aims to limit the transmission of vibration between one component and another.
Vibration control methods involve decoupling a driven vibration component from another linked component.
Internal sources of vibration
- Industrial machinery: These may be out of balance rotary machines or impact machines (metal bashing, wood machining).
- Building services plant: Air handling units and power generators
- Movement of human beings: Footsteps particularly.
External sources of vibration
Nearby industrial installations
Road traffic, particularly HGVs on poorly maintained roads
Surface railway traffic
Underground railways
Building operations such as pile driving
Blasting for mineral extraction or civil engineering projects
As part of the task of vibration control we may need to;
Measure vibration magnitudes in a building
Predict vibration magnitudes in a planned building
Assess vibration magnitudes in terms of their effects on human beings
Specify measures to reduce vibration magnitudes
Free vibration
Free vibration, where the system is at first displaced from the equilibrium position and then set free. For a perfectly elastic system with no energy loss (damping) the resulting oscillations would continue indefinitely
Forced vibration,
Forced vibration, where the vibrating system is coupled to an external vibration that determines the frequency and amplitude of the vibration
Vibration in six possible motions
Vibration can be analysed into six possible motions, the
- three orthogonal axis and three rotations about those axis.
- These are referred to as six degrees of freedom.
Dealing with anything other than one degree of freedom is complex
- Usually one of the six modes is dominant so can focus on that
Simple one degree of freedom system with vibration along one axis

what are we interested in in a a simple isolating system
In a simple isolating system we are interested in the effect of the driving system upon the mass-spring system.
what will the motion of the mass and force vary with
The motion of the mass and the force transmitted to the mass will vary with the frequency of the driving system.
Force transmissibility, tf , is the ratio of the force applied to the mass-spring system at the driving point to the force transmitted by the isolating system.
Displacement transmissibility, td , is the ratio of the displacement of the driving point to the displacement transmitted.
displacement transmissibility
If the vibration of the machine is such that its rms displacement is xd metres, and the resulting vibration of the support has an rms displacement of xt metres, the displacement transmissibility will be t, where

what is force transmisbilyu
The force transmissibility is the ratio of the force exerted by the isolating system to the farce applied to it;

simple system transmissibility equation
For simple systems (single mass and vibration only in one direction, i.e. single degree of freedom, and without damping like in Figure 6.1), the two transmissibility’s have the same value.
Transmissibility varies with frequency according to the equation

variation of transmissibility with the ratio of frequency to the natural or resonant frequency
The variation of transmissibility with the ratio of frequency to the natural or resonant frequency is shown in Figure 6.2.
- At frequencies far below the resonant frequency [A], transmissibility is close to 1 and the input and output are similar.
- As the frequency rises [B], the transmissibility rises and eventually reaches a peak at the natural or resonant frequency of the system (*f0*) [C**].
- As the frequency increases further, the transmissibility decreases to the neutral value of 1 when the frequency ratio reaches 1.41 (√2) [D].
- At this point the input and output are equal. For driving frequencies greater than this crossover point, transmissibility progressively decreases and the output vibrations will be less than the input vibrations [E]. Thus the mass will be isolated from the driving vibrations.
