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THz applications for NDT
(2017)
Electromagnetic waves in the frequency range between 0.1 and 10 THz are described as THz-radiation (T-ray). The ability to penetrate dielectric materials, to operate contactless and to be non-ionizing as well as be-ing insensitive to ambient temperatures makes THz technologies for NDT applications attractive especially where other techniques are not available or less suitable. Today T-rays are applied in non-destructive testing for quality control and condition monitoring issues. The operation is based on the combination of both transmission and/or reflection measurements and specially developed reconstruction procedures. Firstly, THz-TDS measurements will be presented to demonstrate the opportunities for spectroscopy and imaging of polymer materials. A SAFT algorithm and an Optical Layer-Model will be presented and discussed in more detail to demonstrate the opportunities of image reconstruction for visualization of the inner structures of op-tically and far infra-red opaque polymer composites.
Electromagnetic waves with frequencies between 0.1 and 10 THz are described as THz-radiation (T-ray). The ability to penetrate dielectric materials makes T-rays attractive to reveal discontinuities in polymer and ceramic materials. THz-Time Domain Spectroscopy Systems (THz-TDS) are available on the market today which operates with THz-pulses transmitted and received by optically pumped semiconductor antennas. In THz-TDS the travelling time (ToF) and shape of the pulse is changed if it interacts with the dielectric material and its inherent disconti-nuities. A tomogram of the object under the test can be reconstructed from time of flight diffraction (ToFD) scans if a synthetic focusing aperture (SAFT) algorithm is applied. Otherwise, planar discontinuities like cracks in plastics or delaminated lay-ers in composites can be abstracted as layers located at any angle in relation to the outer sample surface direction. A tomogram from the scanned sample can then be reconstructed in case the interactions of electromagnetic pulses with the existing in-herent interfaces are detectable and a model is assumed which describes the device under the test as multilayer structure composed of thin layers with different dielec-tric properties.
A short description of both the SAFT – and Optical Layer algorithm for the recon-struction of the inherent structure is initially given. Measurements on representative samples with a variety of artificially produced small and large scale. Reconstructed tomograms are presented to discuss and evaluate the benefits and limits of the two different reconstruction approaches.