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Electrostrictive fluid pressure from a laser beam
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View: Figures


Image of FIG. 1.
FIG. 1.

(Color online) The situation considered: A Gaussian laser beam of width propagates through a medium of relative permittivity ɛ (λ: wavelength). The laser intensity varies in time according to a function T(t).

Image of FIG. 2.
FIG. 2.

(Color online) Coordinate shift: Translating the z axis to the point (ρ,0).

Image of FIG. 3.
FIG. 3.

(Color online) Left: The function for τ 0 = 5. Right: The reduced pressure p(ξ,τ)/χ(0) for τ 0 = 5 as given in Eq. (33b).

Image of FIG. 4.
FIG. 4.

(Color online) The pressure p(0,τ) on the axis, Eq. (38), as function of dimensionless time τ, divided by the prefactor χ(0). The pulse is turned on at τ = 0 and off at τ = τ 0 = 5.

Image of FIG. 5.
FIG. 5.

(Color online) Coordinate transformation to spherical coordinates with origin at (ξ,0,0) in the cylindrical (ξ′,θ′,z′) system, and polar axis x′.

Image of FIG. 6.
FIG. 6.

(Color online) The functions and P on the symmetry axis for τ 0 = 5.

Image of FIG. 7.
FIG. 7.

(Color online) Left: The function from Eq. (45) and (47) for τ 0 = 5. Right: The reduced pressure p(ξ,τ)/χ(0) for τ 0 = 5, as given in Eq. (51).


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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Electrostrictive fluid pressure from a laser beam