Ignition of Coal Microparticles by Laser Pulses of The Second Harmonic of a Ndodymium Laser in the Q-Switched Regime

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Resumo

The ignition of pelletized samples of hard coals of the long-flame gas (DG), gas (G), fat (L), coke (K) grades with particle sizes ≤63 μm by laser pulses (λ = 532 nm, τi = 10 ns) was studied. When the critical radiation energy density Hcr(1), specific for each grade of coal, is exceeded, an optical breakdown occurs and a dense plasma with a continuous emission spectrum is formed. As the plasma expands and rarefies, the spectra show the emission of carbon ions CII, excited nitrogen atoms N, excited carbon molecules C2, and carbon monoxide CO. The plasma glow intensity peaks at the end of the laser pulse, and the glow relaxation time is ~1 μs. The plasma glow amplitude increases nonlinearly with increasing laser pulse energy density. At radiation energy density H ≥ Hcr(2), specific for each grade of coal, thermochemical reactions are initiated in the volume of microparticles and coal particles are ignited in a submillisecond time interval.

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Sobre autores

B. Aduev

Institute of Coal Chemistry and Material Science, Russian Academy of Sciences

Autor responsável pela correspondência
Email: lesinko-iuxm@yandex.ru
Rússia, Kemerovo

D. Nurmukhametov

Institute of Coal Chemistry and Material Science, Russian Academy of Sciences

Email: lesinko-iuxm@yandex.ru
Rússia, Kemerovo

Ya. Kraft

Institute of Coal Chemistry and Material Science, Russian Academy of Sciences

Email: lesinko-iuxm@yandex.ru
Rússia, Kemerovo

Z. Ismagilov

Institute of Coal Chemistry and Material Science, Russian Academy of Sciences

Email: lesinko-iuxm@yandex.ru
Rússia, Kemerovo

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2. Fig. 1. Functional scheme of the experimental setup: 1 - neutral light filters; 2 - beam splitter plate; 3 - rotating mirror; 4 - lens (F = 25 cm); 5 - experimental assembly with sample; 6, 8, 9 - lenses (F = 10 cm); 7 - spectral-temporal slit; L - pulsed Nd: YAG-laser, F - photodiode, FX - photochronograph, P - polychromator, SFX - spectrophotochronograph “VZGLYAD-2A”, BS - synchronization unit, PC - personal computer, PEU - photomultiplier tube, K - experimental camera.

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3. Fig. 2. Typical oscillograms of the first (a) and second (b) luminescence types of DG coal (the inset shows the initial section of luminescence in the time interval 0-60 ns; the dashed line is a laser pulse).

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4. Fig. 3. Dependence of the probability of occurrence (P) of the detected types of luminescence for DG coal on the energy density of laser pulses: 1 - first type of luminescence, Hcr(1) = (0.40 ± 0.05) J/cm2 (Fig. 2a); 2 - second type of luminescence, Hcr(2) = (3.9 ± 0.4) J/cm2 (Fig. 2b).

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5. Fig. 4. Dependence of the luminescence intensity amplitude I on the energy density H at the moment of time corresponding to the end of the laser pulse for the following coal grades: a - DG, b - G, c - Zh, d - K.

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6. Fig. 5. Luminescence spectra of samples at the moment of time 20 ns from the beginning of the laser pulse for the following coal grades: a - DG, b - G, c - Zh, d - K.

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7. Fig. 6. Luminescence spectra of samples at the moment of time 100 ns from the beginning of the laser pulse of the following coal grades: a - DG, b - G, c - Zh, d - K

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8. Fig. 7. Luminescence spectra of samples at the time moments corresponding to maxima on the kinetic curves of Fig. 2b for the following coal types: a - DG, b - G, c - Zh, d - K. Dashed curves - approximation by Planck's formula at temperature (2400 ± 100) K.

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9. Fig. 8. Dependences of Hcr(1) (a) and Hcr(2) (b) on the volatile yield, V daf, measured when exposed to radiation with λ = 1064 (1) and 532 nm (2).

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