Abstract
The electromagnetic response to impact excitation in high-ohmic composite materials may contain three components. The first component is determined by a change in the dipole moment induced by a striker approaching the surface of a sample possessing a random (surface or bulk) charge; the second component is due to the electrization of a sample material at the point of impact; and the third component is determined by mechanoelectric transformations at the matrix-filler phase boundary.
| Original language | English |
|---|---|
| Pages (from-to) | 825-826 |
| Number of pages | 2 |
| Journal | Technical Physics Letters |
| Volume | 27 |
| Issue number | 10 |
| DOIs | |
| Publication status | Published - Oct 2001 |
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ASJC Scopus subject areas
- Physics and Astronomy (miscellaneous)
Cite this
The mechanism of mechanoelectric transformations in composite materials. / Fursa, T. V.; Khorsov, N. N.; Romanov, D. B.
In: Technical Physics Letters, Vol. 27, No. 10, 10.2001, p. 825-826.Research output: Contribution to journal › Article
}
TY - JOUR
T1 - The mechanism of mechanoelectric transformations in composite materials
AU - Fursa, T. V.
AU - Khorsov, N. N.
AU - Romanov, D. B.
PY - 2001/10
Y1 - 2001/10
N2 - The electromagnetic response to impact excitation in high-ohmic composite materials may contain three components. The first component is determined by a change in the dipole moment induced by a striker approaching the surface of a sample possessing a random (surface or bulk) charge; the second component is due to the electrization of a sample material at the point of impact; and the third component is determined by mechanoelectric transformations at the matrix-filler phase boundary.
AB - The electromagnetic response to impact excitation in high-ohmic composite materials may contain three components. The first component is determined by a change in the dipole moment induced by a striker approaching the surface of a sample possessing a random (surface or bulk) charge; the second component is due to the electrization of a sample material at the point of impact; and the third component is determined by mechanoelectric transformations at the matrix-filler phase boundary.
UR - http://www.scopus.com/inward/record.url?scp=0035541491&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=0035541491&partnerID=8YFLogxK
U2 - 10.1134/1.1414446
DO - 10.1134/1.1414446
M3 - Article
AN - SCOPUS:0035541491
VL - 27
SP - 825
EP - 826
JO - Technical Physics Letters
JF - Technical Physics Letters
SN - 1063-7850
IS - 10
ER -