Vol.3, No 12, 2002 pp. 405-416
UDC 539.3:539:537.61.8
TEMPERATURE, STRAIN AND STRESS FIELDS
PRODUCED BY IMPULSIV ELECTROMAGNETIC RADIATION
IN THE THIN METALLIC PLATE
Vesna Milošević-Mitić
Faculty of Mechanical Engineering, University of Belgrade, 27. marta
80, Yugoslavia
Phone: +(381) 11 3370-379, e-mail: mvesna@alfa.mas.bg.ac.yu
In the paper the case of transversal vibrations of the thin elastic metallic
plate produced by impulsive electromagnetic radiation at the upper surface
is considered. As each electromagnetic wave can be represented as a sum
of simple plane waves, an analytical solution is given for only one plane
wave. It is assumed that all field quantities of the wave vary with time
as exp(j?t) and are represented in the complex form. As a result of time-changing
electromagnetic field conducting currents are appearing. Using complex
calculation we arrive to the distribution of the power of the eddy-current
losses in the plate. That power can be treated as a volume heat source.
Impulsive radiation can be represented mathematically as the sum of Heaviside
functions. Using integral transform technique we can solve differential
equations governing temperature field, transverse vibrations and stress
field. In the case when the skin depth is small compared to the plate thickness,
the problem can be treated as a thermal shock problem. The power which
electromagnetic wave gives to the plate can be calculated by Pointing's
vector. If we want to solve some geometrically complicated problem, we
have to discuss Snellius laws. Using Fresnel coefficients of reflection
and transmission the power of the interrupted wave can be found as a function
of an interrupted angle. The calculation (for example, for radar and air
space structures) can be performed using FEM.
Key words: electromagnetic field, temperature, plate,
induction, heat, vibration, finite element.
POLJA TEMPERATURE, NAPONA I DEFORMACIJE
TANKE METALNE PLOČE IZAZVANA IMPULSNIM ELEKTOMAGNETSKIM TALASOM
U radu su razmatrane poprečne vibracije tanke elastične metalne ploče izazvane
delovanjem impulsnog elektromagnetskog talasa (na gornjoj površini ploče).
Kako svaki elektromagnetski talas može da se prikaže kao zbir prostih ravanskih
talasa, analitičko rešenje je dato samo za jedan ravanski talas. To podrazumeva
da se sve karakteristike polja menjaju po eksponencijalnom zakonu exp(j?t),
pa se prikazuju u kompleksnom obliku. Kao proizvod vremenski promenljivog
elektromagnetskog polja pojavljuju se kondukcione struje. Primenom kompleksnog
računa dolazimo do raspodele snage toplotnih gubitaka u ploči, koja se
može tretirati kao zapreminski izvor toplote. Impulsni talas može se matematički
prikazati preko sume Hevisajdovih funkcija. Primenom tehnike integralnih
transformacija možemo rešiti diferencijalne jednačine koje opisuju polje
temperature, napona i pomeranja. U slučaju kada je dubina prodiranja mala
u poređenju sa debljinom ploče problem može da se tretira kao termički
udar. Energija koju elektromagnetski talas predaje ploči može da se odredi
pomoću Pointingovog vektora. Ako želimo da rešimo geometrijski komplikovaniji
problem moramo da razmotrimo i Snelijusove zakone prelamanja. Primenom
Frenelovih koeficijenata refleksije i transmisije snaga upadnog talasa
može se odrediti na osnovu upadnog ugla. Račun (na primer za radare i aero
strukture) može se izvesti primenom metode konačnih elemenata.