EXPERIMENTAL SETUPS

M.Sc. Thesis Experiment Set-up

Representation of the incident and reflected wave components in the inlet and outlet ducts

Educational Muffler Test Set-up

Noise reduction characteristics of muffler models can be measured by use of the travelling microphone method. This method depends on measuring the maximum SPL values in the inlet and outlet pipes. The crucial point in the measurements is the cut-off frequency of the pipes used in the tests. Match between the predicted and measured values show a fairly good agreement in the frequency region under the first cut-off frequency. Theoretical computations can be carried out by use of the plane wave propagation which gives satisfactory results in most automobile exhaust applications.

FFT Analysis Using the Educational Four Cylinder Engine and B&K 2148 Signal Analyzer

Complex Modulus Apparatus and Auxiliary Equipments

The reduction of vibration resonances is a problem of the greatest importance, in the case of many simple devices, in which only a few natural resonances are present, they can be rejected outside the range of the exciting frequencies by suitably modifiying the stiffness-mass ratios in the design of the article. Generally, mechanical constructions present an extremely large number of resonances, and the only practical solution to the problems caused by their existence, is to reduce the resonance amplitude by means of damping materials or special absorbents. A direct consequence of these developments is a great need for objective, internal damping measuring technique. The internal damping properties of materials are characterized by means of the loss factor d which is defined as the inverse of the quality factor of the resonances produced by the materials.

Measuring techniques, for the measurement of the loss factor d, should cover the great variety of modern construction materials and also the ever extending range of temperature in which modern machinery is used. One of the methods to measure the internal damping factor is the frequency response method. In this method a bar shaped sample is excited into vibration with a variable amplitude periodic force and the vibration amplitude is plotted as a function of frequency. From such a curve, at a resonance peak the loss factor is calculated as

where is the bandwidth at the half power points (3 dB points ), is the resonance frequency and index n is the order of the resonance, or mode number.