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A new face drilling rig for narrow tunnels and ... - Advanced Mining

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Sound power P<br />

Sound power P is the acoustic power that is delivered<br />

by a vibrating element as airborne sound. It is expressed in<br />

Nm/s or W. The sound power is, by analogy to the power<br />

known in the physics, a relative quantity that is not able to<br />

be measured directly.<br />

The sound power P is an emission quantity of a plant,<br />

a machine or a component. It can only be indirectly<br />

determined by measuring a field size. To analyze the sound<br />

power, there are available the sound ranging methods.<br />

The sound ranging can take place in a dead room, in a<br />

free field or in a live room while taking into account the<br />

environmental conditions.<br />

Another possibility of sound ranging is the metering<br />

of the sound intensity on a measuring sur<strong>face</strong> round the<br />

object while eliminating the environmental influences to a<br />

certain degree.<br />

The mathematical link between sound pressure, sound<br />

intensity <strong>and</strong> sound power is described following the<br />

definitions speed of sound, sound particle velocity <strong>and</strong><br />

their effective values.<br />

Link between sound pressure <strong>and</strong> sound<br />

power<br />

The link between sound pressure <strong>and</strong> sound power is the<br />

most important base to be able to underst<strong>and</strong> acoustics.<br />

The sound power is not directly measurable, as already<br />

mentioned be<strong>for</strong>e, but it is to be fixed by measuring the<br />

sound pressure. While doing so, there is to be indicated,<br />

Issue 04 | 2010<br />

TRANSFER OF TECHNOLOGY<br />

Fig. 2:<br />

Überlagerung Schalldruck und<br />

Atmosphärnedruck<br />

among the pressure, the measuring point as well (distance<br />

from source).<br />

This shows the often cited analogy to the thermal<br />

output of a source that is not directly measurable. Through<br />

measurement of temperature at a place in a defined position<br />

towards the source it is enabled the thermal output of a<br />

body to be determined.<br />

It is of importance to be always aware of the conditions<br />

<strong>for</strong> the validity of the link, derived in the following. We<br />

are working on the assumption that it is a homogeneous<br />

source, isotropically radiating in an otherwise isotropic<br />

room. Both conditions are only fulfilled in special cases.<br />

The error resulting from the condition fixed by our end,<br />

however, is negligible as long as we only need a „good<br />

estimation“. All further reflections on this topic are further<br />

based on the incoherence of the sources.<br />

Speed of sound or sound velocity c<br />

Speed of sound or sound velocity c is the speed at<br />

which the sound waves propagate. It is to set apart from<br />

the sound particle velocity. By way of illustration, the wave<br />

motion is represented in figure 1.01. Each point may be<br />

a gas molecule (air particle). The particle itself effects<br />

a harmonic vibration round its neutral position (vertical<br />

lines A – M). Due to excursion neighbouring particles get<br />

expelled from their neutral position, <strong>and</strong> they also effect,<br />

to the neighbouring particle, a phase-shifted, harmonic<br />

vibration round this neutral position. That is how the wave<br />

propagation (blue line) is created. The gradient of the<br />

straight line is a measure <strong>for</strong> the sound velocity.<br />

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