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ПОВЫШЕНИЕ ДОСТОВЕРНОСТИ ИНТЕРПРЕТАЦИИ

ДАННЫХ ГИС С ИСПОЛЬЗОВАНИЕМ ФИЗИЧЕСКИХ

И КОЛЛЕКТОРСКИХ ХАРАКТЕРИСТИК ОБРАЗЦОВ

А.В. Дахнов, В.С. Жуков, О.В. Иселидзе, И.Б. Крюкова,

Е.О. Семенов

Ɉɞɧɨɣ ɢɡ ɨɫɧɨɜɧɵɯ ɡɚɞɚɱ ɢɫɫɥɟɞɨɜɚɧɢɹ ɤɟɪɧɚ ɹɜɥɹɟɬɫɹ ɩɨ-

ɫɬɪɨɟɧɢɟ ɢɧɬɟɪɩɪɟɬɚɰɢɨɧɧɵɯ ɦɨɞɟɥɟɣ. Ⱦɥɹ ɫɨɡɞɚɧɢɹ ɩɟɬɪɨɮɢɡɢ-

ɱɟɫɤɨɣ ɨɫɧɨɜɵ ɢɧɬɟɪɩɪɟɬɚɰɢɢ ɦɚɬɟɪɢɚɥɨɜ ɝɟɨɮɢɡɢɱɟɫɤɢɯ ɢɫɫɥɟ-

ɞɨɜɚɧɢɣ ɫɤɜɚɠɢɧ (Ƚɂɋ) ɢ ɩɨɜɵɲɟɧɢɹ ɞɨɫɬɨɜɟɪɧɨɫɬɢ ɨɩɪɟɞɟɥɟɧɢɹ

ɤɨɥɥɟɤɬɨɪɫɤɢɯ ɫɜɨɣɫɬɜ ɩɨɪɨɞ ɧɟɨɛɯɨɞɢɦɨ ɩɪɨɜɟɞɟɧɢɟ ɫɩɟɰɢɚɥɶ-

ɧɵɯ ɢɫɫɥɟɞɨɜɚɧɢɣ ɤɟɪɧɚ ɜ ɭɫɥɨɜɢɹɯ, ɦɨɞɟɥɢɪɭɸɳɢɯ ɩɥɚɫɬɨɜɵɟ.

ɇɚɢɛɨɥɟɟ ɨɩɬɢɦɚɥɶɧɵɦ ɞɥɹ ɨɩɪɟɞɟɥɟɧɢɹ ɩɟɬɪɨɮɢɡɢɱɟɫɤɢɯ ɡɚɜɢ-

ɫɢɦɨɫɬɟɣ ɩɪɢ ɬɟɪɦɨɛɚɪɢɱɟɫɤɢɯ ɭɫɥɨɜɢɹɯ ɹɜɥɹɟɬɫɹ ɩɪɹɦɨɟ ɷɤɫ-

ɩɟɪɢɦɟɧɬɚɥɶɧɨɟ ɢɡɭɱɟɧɢɟ ɤɟɪɧɨɜɨɝɨ ɦɚɬɟɪɢɚɥɚ ɜ ɥɚɛɨɪɚɬɨɪɧɵɯ

ɭɫɥɨɜɢɹɯ, ɩɪɢ ɤɨɬɨɪɨɦ ɛɭɞɟɬ ɭɱɬɟɧɨ ɜɥɢɹɧɢɟ ɜɫɟɯ ɥɢɬɨɥɨɝɢɱɟɫɤɢɯ

ɨɫɨɛɟɧɧɨɫɬɟɣ ɩɨɪɨɞ [1–5].

ɋɥɟɞɭɟɬ ɨɬɦɟɬɢɬɶ ɜɤɥɚɞ Ʌ.Ⱥ. Ȼɭɪɹɤɨɜɫɤɨɝɨ, Ȼ.ɘ. ȼɟɧɞɟɥɶɲ-

ɬɟɣɧɚ, ȼ.ɇ. Ⱦɚɯɧɨɜɚ, ȼ.Ɇ. Ⱦɨɛɪɵɧɢɧɚ, Ʌ.ɉ. Ⱦɨɥɢɧɨɣ, Ɇ.Ƚ. Ʌɚɬɵ-

ɲɨ ɜɨɣ, ȿ.ɂ. Ʌɟɨɧɬɶɟɜɚ, ȼ.ɇ. Ʉɨɛɪɚɧɨɜɨɣ, Ƚ.ɋ. Ɇɨɪɨɡɨɜɚ, ɋ.Ⱥ. ɋɭɥ-

ɬɚ ɧɨɜɚ, Ɇ.Ɇ. ɗɥɚɧɫɤɨɝɨ, Ɏ.Ⱥ. Ɍɪɟɛɢɧɚ, Ⱦɠ. Ⱥɦɢɤɫɚ, ɉ. Ⱦɠɨɧɫɚ,

ɋ.Ⱦ. ɉɢɪɫɨɧɚ ɢ ɞɪɭɝɢɯ ɜ ɢɡɭɱɟɧɢɟ ɡɚɜɢɫɢɦɨɫɬɟɣ ɦɟɠɞɭ ɮɢɥɶɬɪɚ-

ɰɢɨɧɧɨ-ɟɦɤɨɫɬɧɵɦɢ ɫɜɨɣɫɬɜɚɦɢ ɢ ɩɟɬɪɨɮɢɡɢɱɟɫɤɢɦɢ ɩɚɪɚɦɟɬɪɚ-

ɦɢ ɪɚɡɥɢɱɧɵɯ ɝɨɪɧɵɯ ɩɨɪɨɞ.

Ʉɚɤ ɢɡɜɟɫɬɧɨ, ɫɭɳɟɫɬɜɟɧɧɨɟ ɜɥɢɹɧɢɟ ɧɚ ɮɢɥɶɬɪɚɰɢɨɧɧɨ-ɟɦ-

ɤɨɫɬɧɵɟ ɫɜɨɣɫɬɜɚ ɩɨɪɨɞ ɨɤɚɡɵɜɚɸɬ ɬɚɤɢɟ ɮɚɤɬɨɪɵ, ɤɚɤ: ɥɢɬɨɥɨɝɨ-

ɦɢɧɟɪɚɥɨɝɢɱɟɫɤɢɣ ɫɨɫɬɚɜ; ɫɬɪɭɤɬɭɪɚ ɩɨɪɨɜɨɝɨ ɩɪɨɫɬɪɚɧɫɬɜɚ;

ɫɜɨɣɫɬɜɚ ɩɥɚɫɬɨɜɵɯ ɮɥɸɢɞɨɜ; ɬɢɩ ɢ ɯɚɪɚɤɬɟɪ ɪɚɫɩɪɟɞɟɥɟɧɢɹ ɰɟ-

ɦɟɧɬɚ, ɤɨɬɨɪɵɟ ɨɩɪɟɞɟɥɹɸɬ ɭɞɟɥɶɧɨɟ ɷɥɟɤɬɪɢɱɟɫɤɨɟ ɫɨɩɪɨɬɢɜɥɟ-

132

СБОРНИК НАУЧНЫХ СТАТЕЙ

ɧɢɟ, ɫɤɨɪɨɫɬɶ ɪɚɫɩɪɨɫɬɪɚɧɟɧɢɹ ɭɩɪɭɝɢɯ ɜɨɥɧ, ɩɥɨɬɧɨɫɬɶ, ɪɚɞɢɨɚɤ-

ɬɢɜɧɨɟ ɢɡɥɭɱɟɧɢɟ ɢ ɦɧɨɝɢɟ ɞɪɭɝɢɟ ɯɚɪɚɤɬɟɪɢɫɬɢɤɢ [2–5].

ɐɟɥɶɸ ɞɚɧɧɨɣ ɪɚɛɨɬɵ ɹɜɥɹɥɨɫɶ ɢɫɫɥɟɞɨɜɚɧɢɟ ɜɡɚɢɦɨɫɜɹɡɢ

ɮɢɥɶɬɪɚɰɢɨɧɧɨ-ɟɦɤɨɫɬɧɵɯ ɫɜɨɣɫɬɜ ɫ ɩɚɪɚɦɟɬɪɨɦ ɩɨɪɢɫɬɨɫɬɢ, ɢɧ-

ɬɟɪɜɚɥɶɧɵɦ ɜɪɟɦɟɧɟɦ, ɚɤɭɫɬɢɱɟɫɤɢɦ ɢɦɩɟɞɚɧɫɨɦ ɝɨɪɧɵɯ ɩɨɪɨɞ.

ɂɫɫɥɟɞɨɜɚɧɢɹ ɩɪɨɜɨɞɢɥɢɫɶ ɧɚ ɤɨɥɥɟɤɰɢɢ ɨɛɪɚɡɰɨɜ ɤɨɥɥɟɤɬɨɪɨɜ

ɸɪɫɤɨɝɨ ɜɨɡɪɚɫɬɚ, ɩɪɟɞɫɬɚɜɥɟɧɧɵɯ ɩɟɫɱɚɧɢɤɚɦɢ ɢ ɚɥɟɜɪɨɥɢɬɚɦɢ.

ȼ ɪɟɡɭɥɶɬɚɬɟ ɩɪɨɜɟɞɟɧɧɵɯ ɷɤɫɩɟɪɢɦɟɧɬɚɥɶɧɵɯ ɢɫɫɥɟɞɨɜɚ-

ɧɢɣ ɜ ɭɫɥɨɜɢɹɯ, ɦɨ

ɞɟɥɢɪɭɸɳɢɯ ɩɥɚɫɬɨɜɵɟ, ɛɵɥɢ ɩɨɫɬɪɨɟɧɵ ɢ

ɢɡɭɱɟɧɵ ɡɚɜɢɫɢɦɨɫɬɢ, ɩɨɡɜɨɥɹɸɳɢɟ ɨɰɟɧɢɬɶ ɜɡɚɢɦɨɫɜɹɡɶ ɦɟɠ-

ɞɭ ɮɢɥɶɬɪɚɰɢɨɧɧɨ-ɟɦɤɨɫɬɧɵɦɢ ɫɜɨɣɫɬɜɚɦɢ (ɩɨɪɢɫɬɨɫɬɶɸ ɢ ɩɪɨ-

ɧɢɰɚɟɦɨɫɬɶɸ) ɢ ɮɢɡɢɱɟɫɤɢɦɢ ɩɚɪɚɦɟɬɪɚɦɢ ɝɨɪɧɵɯ ɩɨɪɨɞ. Ɋɚɫ-

ɫɦɨɬɪɢɦ ɡɚɜɢɫɢɦɨɫɬɢ ɪɹɞɚ ɩɟɬɪɨɮɢɡɢɱɟɫɤɢɯ ɩɚɪɚɦɟɬɪɨɜ ɨɬ ɩɨ-

ɪɢɫɬɨɫɬɢ.

Пористость

Ɉɩɪɟɞɟɥɟɧɢɟ ɤɨɷɮɮɢɰɢɟɧɬɚ ɩɨɪɢɫɬɨɫɬɢ (Ʉ

) ɧɚ ɦɟɫɬɨɪɨɠɞɟɧɢ-

ɹɯ ɧɟɮɬɢ ɢ ɝɚɡɚ ɩɪɨɜɨɞɢɬɫɹ ɩɨ ɞɚɧɧɵɦ ɝɟɨɮɢɡɢɱɟɫɤɢɯ ɢɫɫɥɟɞɨɜɚ-

ɧɢɣ ɫɤɜɚɠɢɧ ɫ ɢɫɩɨɥɶɡɨɜɚɧɢɟɦ ɢɧɬɟɪɩɪɟɬɚɰɢɨɧɧɵɯ ɦɨɞɟɥɟɣ, ɩɨ-

ɥɭɱɟɧɧɵɯ ɩɪɢ ɢɫɫɥɟɞɨɜɚɧɢɢ ɤɟɪɧɨɜɨɝɨ ɦɚɬɟɪɢɚɥɚ. ȼɨɡɦɨɠɧɨɫɬɢ

ɢɡɜɥɟɱɟɧɢɹ ɡɚɩɚɫɨɜ ɭɝɥɟɜɨɞɨɪɨɞɨɜ ɯɚɪɚɤɬɟɪɢɡɭɸɬɫɹ ɩɪɨɧɢɰɚɟɦɨ-

ɫɬɶɸ ɩɨɪɨɞɵ.

ɉɨɪɢɫɬɨɫɬɶ ɢ ɩɪɨɧɢɰɚɟɦɨɫɬɶ. ɋɨɩɨɫɬɚɜɥɟɧɢɟ ɤɨɷɮɮɢɰɢɟɧ-

ɬɚ ɩɪɨɧɢɰɚɟɦɨɫɬɢ (Ʉ

ɩɪ

) ɢ ɤɨɷɮɮɢɰɢɟɧɬɚ ɩɨɪɢɫɬɨɫɬɢ (Ʉ

) ɩɨɤɚɡɵɜɚ-

ɟɬ ɧɚɥɢɱɢɟ ɫɜɹɡɢ ɦɟɠɞɭ ɧɢɦɢ (ɤɨɷɮɮɢɰɢɟɧɬ ɤɨɪɪɟɥɹɰɢɢ r = 0,6) ɢ

ɫ ɜɵɫɨɤɨɣ ɫɬɟɩɟɧɶɸ ɞɨɫɬɨɜɟɪɧɨɫɬɢ (R

= 0,8) ɨɩɢɫɵɜɚɟɬɫɹ ɷɤɫɩɨ-

ɧɟɧɰɢɚɥɶɧɨɣ ɡɚɜɢɫɢɦɨɫɬɶɸ (ɪɢɫ.1):

ɩɪ

= 0,014ɟ

0,473Ʉ

. (1)

ɇɟɫɦɨɬɪɹ ɧɚ ɞɨɜɨɥɶɧɨ ɜɵɫɨɤɭɸ ɫɬɟɩɟɧɶ ɞɨɫɬɨɜɟɪɧɨɫɬɢ ɚɩ-

ɩɪɨɤɫɢɦɚɰɢɢ, ɡɚɜɢɫɢɦɨɫɬɶ (1) ɦɨɠɧɨ ɢɫɩɨɥɶɡɨɜɚɬɶ ɞɥɹ ɨɰɟɧɤɢ ɩɨ

ɢɡɜɟɫɬɧɵɦ ɡɧɚɱɟɧɢɹɦ ɩɨɪɢɫɬɨɫɬɢ ɫ ɨɩɪɟɞɟɥɟɧɧɨɣ ɫɬɟɩɟɧɶɸ ɨɫɬɨ-

ɪɨɠɧɨɫɬɢ, ɬɚɤ ɤɚɤ ɤɨɷɮɮɢɰɢɟɧɬ ɤɨɪɪɟɥɹɰɢɢ ɦɟɠɞɭ Ʉ

ɢ Ʉ

ɩɪ

ɞɨɜɨɥɶ-

ɧɨ ɧɢɡɤɢɣ ɢ ɫɜɹɡɶ ɦɟɠɞɭ ɧɢɦɢ ɧɟ ɹɜɥɹɟɬɫɹ ɬɟɫɧɨɣ ɢ ɭɫɬɨɣɱɢɜɨɣ ɜ

ɪɚɦɤɚɯ ɢɫɫɥɟɞɨɜɚɧɧɨɣ ɤɨɥɥɟɤɰɢɢ ɨɛɪɚɡɰɨɜ. ɇɟɜɵɫɨɤɢɣ ɤɨɷɮɮɢ-

133

АКТУАЛЬНЫЕ ВОПРОСЫ ИССЛЕДОВАНИЙ ПЛАСТОВЫХ СИСТЕМ МЕСТОРОЖДЕНИЙ УГЛЕВОДОРОДОВ

ɰɢɟɧɬ ɤɨɪɪɟɥɹɰɢɢ (r = 0,6) ɦɨɠɧɨ ɨɛɴɹɫɧɢɬɶ ɬɟɦ, ɱɬɨ ɩɨ Ʉɨɡɟɧɢ-

Ʉɚɪɦɚɧɚ ɤɨɷɮɮɢɰɢɟɧɬ ɩɪɨɧɢɰɚɟɦɨɫɬɢ ɡɚɜɢɫɢɬ ɧɟ ɬɨɥɶɤɨ ɨɬ ɟɦɤɨ-

ɫɬɢ ɤɨɥɥɟɤɬɨɪɚ, ɧɨ ɢ ɨɬ ɫɨɞɟɪɠɚɧɢɹ ɜ ɧɟɦ ɬɨɧɤɨɞɢɫɩɟɪɫɧɨɣ ɮɪɚɤ-

ɰɢɢ, ɭɜɟɥɢɱɢɜɚɸɳɟɣ ɭɞɟɥɶɧɭɸ ɩɨɜɟɪɯɧɨɫɬɶ ɩɨɪɨɞɵ.

ɉɨɪɢɫɬɨɫɬɶ ɢ ɩɚɪɚɦɟɬɪ ɩɨɪɢɫɬɨɫɬɢ. ɂɡɜɟɫɬɧɨ, ɱɬɨ ɩɚɪɚ-

ɦɟɬɪ ɩɨɪɢɫɬɨɫɬɢ, ɪɚɫɫɱɢɬɵɜɚɟɦɵɣ ɤɚɤ ɨɬɧɨɲɟɧɢɟ ɭɞɟɥɶɧɨɝɨ ɷɥɟɤ-

ɬɪɢɱɟɫɤɨɝɨ ɫɨɩɪɨɬɢɜɥɟɧɢɹ ɜɨɞɨɧɚɫɵɳɟɧɧɨɣ ɩɨɪɨɞɵ (ȡ

ɜɩ

) ɤ ɭɞɟɥɶ-

ɧɨɦɭ ɷɥɟɤɬɪɢɱɟɫɤɨɦɭ ɫɨɩɪɨɬɢɜɥɟɧɢɸ ɧɚɫɵɳɚɸɳɟɣ ɟɝɨ ɜɨɞɵ (ȡ

)

ɩɪɟɠɞɟ ɜɫɟɝɨ ɯɚɪɚɤɬɟɪɢɡɭɟɬ ɨɛɴɟɦ ɬɨɤɨɩɪɨɜɨɞɹɳɟɝɨ ɩɪɨɫɬɪɚɧɫɬɜɚ

ɩɨɪɨɞ ɢ ɟɝɨ ɫɬɪɭɤɬɭɪɭ. Ɂɚɜɢɫɢɦɨɫɬɶ ɦɟɠɞɭ ɩɚɪɚɦɟɬɪɨɦ ɢ ɤɨɷɮɮɢ-

ɰɢɟɧɬɨɦ ɩɨɪɢɫɬɨɫɬɢ ɹɜɥɹɟɬɫɹ ɨɫɧɨɜɧɨɣ ɢɧɬɟɪɩɪɟɬɚɰɢɨɧɧɨɣ ɦɨɞɟ-

ɥɶɸ ɞɥɹ ɨɩɪɟɞɟɥɟɧɢɹ Ʉ

ɩɨ ɞɚɧɧɵɦ ɷɥɟɤɬɪɨɦɟɬɪɢɢ ɫɤɜɚɠɢɧ.

ɉɪɢɜɟɞɟɧɧɚɹ ɧɚ ɪɢɫ. 2 ɡɚɜɢɫɢɦɨɫɬɶ ɩɚɪɚɦɟɬɪɚ ɩɨɪɢɫɬɨɫɬɢ ɨɬ

ɩɨɪɢɫɬɨɫɬɢ ɫ ɜɵɫɨɤɨɣ ɫɬɟɩɟɧɶɸ ɞɨɫɬɨɜɟɪɧɨɫɬɢ R

= 0,94 ɦɨɠɟɬ

ɛɵɬɶ ɨɩɢɫɚɧɚ ɫɬɟɩɟɧɧɨɣ ɡɚɜɢɫɢɦɨɫɬɶɸ (2):

= 1,644 / Ʉ

1,471

, (2)

ɝɞɟ Ʉ

– ɩɨɪɢɫɬɨɫɬɶ ɝɨɪɧɨɣ ɩɨɪɨɞɵ, ɜɵɪɚɠɟɧɧɚɹ ɜ ɞɨɥɹɯ ɟɞɢɧɢɰɵ.

Рис. 1. Зависимость проницаемости от пористости

0,1

1,0

10,0

100,0

1000,0

0,0 5,0 10,0 15,0 20,0 25,0

ɉɨɪɢɫɬɨɫɬɶ, %

ɉɪɨɧɢɰɚɟɦɨɫɬɶ, ɦȾ

134

СБОРНИК НАУЧНЫХ СТАТЕЙ

ɇɚɥɢɱɢɟ ɜɵɫɨɤɨɣ ɫɬɟɩɟɧɢ ɞɨɫɬɨɜɟɪɧɨɫɬɢ ɚɩɩɪɨɤɫɢɦɚɰɢɢ ɢ ɜɟ-

ɥɢɱɢɧɵ ɤɨɷɮɮɢɰɢɟɧɬɚ ɤɨɪɪɟɥɹɰɢɢ (r = 0,93), ɫɜɢɞɟɬɟɥɶɫɬɜɭɸɳɟɟ

ɨ ɬɟɫɧɨɣ ɫɜɹɡɢ ɦɟɠɞɭ ɩɨɪɢɫɬɨɫɬɶɸ ɢ ɩɚɪɚɦɟɬɪɨɦ ɩɨɪɢɫɬɨɫɬɢ, ɩɨ-

ɡɜɨɥɹɟɬ ɢɫɩɨɥɶɡɨɜɚɬɶ ɩɨɥɭɱɟɧɧɭɸ ɡɚɜɢɫɢɦɨɫɬɶ ɩɪɢ ɢɧɬɟɪɩɪɟɬɚ-

ɰɢɢ ɞɚɧɧɵɯ ɷɥɟɤɬɪɨɦɟɬɪɢɢ ɫɤɜɚɠɢɧ. Ɉɞɧɚɤɨ ɧɟ ɜɨ ɜɫɟɯ ɫɥɭɱɚɹɯ

ɫɤɜɚɠɢɧɚ ɜɫɤɪɵɜɚɟɬ ɜɨɞɨɧɨɫɧɭɸ ɱɚɫɬɶ ɤɨɥɥɟɤɬɨɪɚ, ɢ ɜɨɡɧɢɤɚɸɬ

ɬɪɭɞɧɨɫɬɢ ɜ ɨɩɪɟɞɟɥɟɧɢɢ ȡ

ɜɩ

, ɚ ɫɥɟɞɨɜɚɬɟɥɶɧɨ, ɜ ɪɚɫɱɟɬɟ ɩɚɪɚɦɟ-

ɬɪɚ ɩɨɪɢɫɬɨɫɬɢ.

ɉɨɪɢɫɬɨɫɬɶ ɢ ɢɧɬɟɪɜɚɥɶɧɨɟ ɜɪɟɦɹ. ȼɬɨɪɵɦ ɝɟɨɮɢɡɢɱɟɫɤɢɦ

ɦɟɬɨɞɨɦ, ɚɤɬɢɜɧɨ ɢɫɩɨɥɶɡɭɟɦɵɦ ɩɪɢ ɨɰɟɧɤɟ ɤɨɷɮɮɢɰɢɟɧɬɚ ɩɨɪɢ-

ɫɬɨɫɬɢ, ɹɜɥɹɟɬɫɹ ɚɤɭɫɬɢɱɟɫɤɢɣ ɦɟɬɨɞ (ȺɄ).

ɉɪɟɞɫɬɚɜɥɟɧɧɚɹ ɧɚ ɪɢɫ. 3 ɡɚɜɢɫɢɦɨɫɬɶ ɢɧɬɟɪɜɚɥɶɧɨɝɨ ɜɪɟɦɟɧɢ

ǻt ɨɬ ɩɨɪɢɫɬɨɫɬɢ ɯɚɪɚɤɬɟɪɢɡɭɟɬɫɹ ɜɵɫɨɤɢɦ ɤɨɷɮɮɢɰɢɟɧɬɨɦ ɤɨɪɪɟ-

ɥɹɰɢɢ (r = 0,92) ɢ ɜɵɫɨɤɨɣ ɫɬɟɩɟɧɶɸ ɞɨɫɬɨɜɟɪɧɨɫɬɢ ɚɩɩɪɨɤɫɢɦɚ-

ɰɢɢ (R

= 0,91) ɥɢɧɟɣɧɨɣ ɡɚɜɢɫɢɦɨɫɬɶɸ (3), ɱɬɨ ɩɨɡɜɨɥɹɟɬ ɢɫɩɨɥɶ-

ɡɨɜɚɬɶ ɟɟ ɩɪɢ ɢɧɬɟɪɩɪɟɬɚɰɢɢ ɞɚɧɧɵɯ ɚɤɭɫɬɢɱɟɫɤɨɝɨ ɦɟɬɨɞɚ:

ǻt = 5,059Ʉ

+ 206,6. (3)

Рис. 2. Зависимость параметра пористости от пористости

10,0

100,0

1000,0

1,0 10,0 100,0

ɉɨɪɢɫɬɨɫɬɶ, %

ɉɚɪɚɦɟɬɪ ɩɨɪɢɫɬɨɫɬɢ

135

АКТУАЛЬНЫЕ ВОПРОСЫ ИССЛЕДОВАНИЙ ПЛАСТОВЫХ СИСТЕМ МЕСТОРОЖДЕНИЙ УГЛЕВОДОРОДОВ

ɉɨɪɢɫɬɨɫɬɶ ɢ ɚɤɭɫɬɢɱɟɫɤɢɣ ɢɦɩɟɞɚɧɫ. Ⱥɤɭɫɬɢɱɟɫɤɢɣ ɢɦ-

ɩɟɞɚɧɫ, ɤɚɤ ɢ ɢɧɬɟɪɜɚɥɶɧɨɟ ɜɪɟɦɹ, ɞɨɜɨɥɶɧɨ ɱɚɫɬɨ ɨɩɪɟɞɟɥɹɟɬɫɹ

ɩɪɢ ɝɟɨɮɢɡɢɱɟɫɤɢɯ ɢɫɫɥɟɞɨɜɚɧɢɹɯ ɫɤɜɚɠɢɧ. Ɍɚɤɠɟ ɨɧ ɹɜɥɹɟɬɫɹ

ɤɨɦɩɥɟɤɫɧɵɦ ɩɚɪɚɦɟɬɪɨɦ, ɬɚɤ ɤɚɤ ɪɚɫɫɱɢɬɵɜɚɟɬɫɹ ɤɚɤ ɩɪɨɢɡɜɟɞɟ-

ɧɢɟ ɫɤɨɪɨɫɬɢ ɩɪɨɞɨɥɶɧɨɣ ɜɨɥɧɵ ɧɚ ɨɛɴɟɦɧɭɸ ɩɥɨɬɧɨɫɬɶ ɩɨɪɨɞɵ,

ɱɬɨ ɩɨɡɜɨɥɹɟɬ ɪɚɫɫɱɢɬɵɜɚɬɶ ɧɚ ɩɨɜɵɲɟɧɢɟ ɤɚɱɟɫɬɜɚ ɨɩɪɟɞɟɥɟɧɢɹ

ɩɨɪɢɫɬɨɫɬɢ ɩɨ ɞɚɧɧɵɦ ɚɤɭɫɬɢɱɟɫɤɨɝɨ ɢɦɩɟɞɚɧɫɚ. ɂɧɬɟɪɜɚɥɶɧɨɟ

ɜɪɟɦɹ ɡɚɜɢɫɢɬ ɧɟ ɬɨɥɶɤɨ ɨɬ ɩɨɪɢɫɬɨɫɬɢ ɢ ɯɚɪɚɤɬɟɪɚ ɧɚɫɵɳɟɧɢɹ

ɩɨɪɨɞɵ, ɧɨ ɢ ɨɬ ɥɢɬɨɥɨɝɢɢ ɢ ɦɢɧɟɪɚɥɶɧɨɝɨ ɫɨɫɬɚɜɚ, ɤɨɬɨɪɵɟ ɬɟɫɧɨ

ɫɜɹɡɚɧɵ ɫ ɩɥɨɬɧɨɫɬɶɸ.

ɋɨɝɥɚɫɧɨ ɪɢɫ. 4 ɡɚɜɢɫɢɦɨɫɬɶ ɦɟɠɞɭ ɚɤɭɫɬɢɱɟɫɤɢɦ ɢɦɩɟɞɚɧ-

ɫɨɦ ɢ ɩɨɪɢɫɬɨɫɬɶɸ Ʉ

ɞɥɹ ɢɫɫɥɟɞɨɜɚɧɧɵɯ ɨɛɪɚɡɰɨɜ ɯɚɪɚɤɬɟɪɢɡɭɟɬ-

ɫɹ ɜɵɫɨɤɨɣ ɞɨɫɬɨɜɟɪɧɨɫɬɶɸ ɚɩɩɪɨɤɫɢɦɚɰɢɢ (R

= 0,96) ɢ ɤɨɷɮɮɢ-

ɰɢɟɧɬɨɦ ɤɨɪɪɟɥɹɰɢɢ (r = 0,98), ɱɬɨ ɩɨɡɜɨɥɹɟɬ ɢɫɩɨɥɶɡɨɜɚɬɶ ɷɬɭ ɡɚ-

ɜɢɫɢɦɨɫɬɶ ɩɪɢ ɫɨɜɦɟɫɬɧɨɣ ɢɧɬɟɪɩɪɟɬɚɰɢɢ ɞɚɧɧɵɯ ɚɤɭɫɬɢɱɟɫɤɨɝɨ

ɢ ɝɚɦɦɚ-ɝɚɦɦɚ-ɩɥɨɬɧɨɫɬɧɨɝɨ (ȽȽɄɩ) ɦɟɬɨɞɨɜ Ƚɂɋ ɞɥɹ ɨɰɟɧɤɢ ɤɨ-

ɷɮɮɢɰɢɟɧɬɚ ɩɨɪɢɫɬɨɫɬɢ Ʉ

ɢɡɭɱɚɟɦɵɯ ɨɬɥɨɠɟɧɢɣ:

Z = 11,70 – 0,244Ʉ

. (4)

Рис. 3. Зависимость интервального времени от пористости

230

240

250

260

270

280

290

300

310

320

330

5,0 10,0 15,0 20,0 25,0

ɉɨɪɢɫɬɨɫɬɶ, %

ɂɧɬɟɪɜɚɥɶɧɨɟ ɜɪɟɦɹ, ɦɤɫ/ɦ

136

СБОРНИК НАУЧНЫХ СТАТЕЙ

Ɍɚɤɢɦ ɨɛɪɚɡɨɦ, ɤɨɦɩɥɟɤɫɢɪɨɜɚɧɢɟ ɝɟɨɮɢɡɢɱɟɫɤɢɯ ɩɚɪɚɦɟɬɪɨɜ

ɜɟɞɟɬ ɤ ɩɨɜɵɲɟɧɢɸ ɞɨɫɬɨɜɟɪɧɨɫɬɢ ɨɩɪɟɞɟɥɟɧɢɹ ɤɨɷɮɮɢɰɢɟɧɬɚ

ɩɨɪɢɫɬɨɫɬɢ ɨɬɥɨɠɟɧɢɣ.

ȼ ɤɚɱɟɫɬɜɟ ɟɳɟ ɨɞɧɨɝɨ ɤɨɦɩɥɟɤɫɧɨɝɨ ɩɚɪɚɦɟɬɪɚ ɦɨɠɧɨ ɜɡɹɬɶ

ɨɬɧɨɲɟɧɢɟ ǻt/P

. Ɏɢɡɢɱɟɫɤɢɣ ɫɦɵɫɥ ɞɚɧɧɨɝɨ ɤɨɦɩɥɟɤɫɢɪɨɜɚɧɢɹ

ɡɚɤɥɸɱɚɟɬɫɹ ɜ ɬɨɦ, ɱɬɨ ɩɨ ɭɪɚɜɧɟɧɢɸ ɫɪɟɞɧɟɝɨ ɜɪɟɦɟɧɢ ǻt = f (Ʉ

ɥɢɬɨɥɨɝɢɢ), ɬ.ɟ. ɦɨɠɧɨ ɫɤɚɡɚɬɶ, ɱɬɨ ǻt ~ Ʉ

. ɉɚɪɚɦɟɬɪ ɩɨɪɢɫɬɨɫɬɢ

ɬɚɤɠɟ ɡɚɜɢɫɢɬ ɢ ɨɬ ɩɨɪɢɫɬɨɫɬɢ, ɢ ɨɬ ɥɢɬɨɥɨɝɢɢ ɢ ɩɨ ɭɪɚɜɧɟɧɢɸ

Ⱥɪɱɢ P

= 1/Ʉ

. Ɍɚɤɢɦ ɨɛɪɚɡɨɦ, ɤɨɦɩɥɟɤɫɧɵɣ ɩɚɪɚɦɟɬɪ ɨɤɚɡɵɜɚ-

ɟɬɫɹ ɩɪɨɩɨɪɰɢɨɧɚɥɶɧɵɦ Ʉ

, ɬ.ɟ. ɭɫɢɥɢɜɚɟɬɫɹ ɜɤɥɚɞ ɩɨɪɢɫɬɨɫɬɢ.

Ɋɚɫɫɦɨɬɪɢɦ ɜɨɡɦɨɠɧɨɫɬɢ ɢɫɫɥɟɞɭɟɦɨɝɨ ɤɨɦɩɥɟɤɫɧɨɝɨ ɩɚɪɚɦɟɬɪɚ.

ɉɨɪɢɫɬɨɫɬɶ ɢ ɤɨɦɩɥɟɤɫɧɵɣ ɩɚɪɚɦɟɬɪ ǻt/P

. Ɂɚɜɢɫɢɦɨɫɬɶ

ɤɨɦɩɥɟɤɫɧɨɝɨ ɩɚɪɚɦɟɬɪɚ ɢ ɩɨɪɢɫɬɨɫɬɢ, ɩɪɟɞɫɬɚɜɥɟɧɧɚɹ ɧɚ ɪɢɫ. 5,

ɩɨɡɜɨɥɹɟɬ ɝɨɜɨɪɢɬɶ ɨ ɜɵɫɨɤɨɣ ɞɨɫɬɨɜɟɪɧɨɫɬɢ ɚɩɩɪɨɤɫɢɦɚɰɢɢ

= 0,97 ɭɪɚɜɧɟɧɢɟɦ (5):

ǻt/Ɋ

= 1,394ɟ

0,128Ʉ

. (5)

Рис.4. Зависимость акустического импеданса от коэффициента пористости образцов

6,0

6,5

7,0

7,5

8,0

8,5

9,0

9,5

10,0

10,5

11,0

5,0 10,0 15,0 20,0 25,0

ɉɨɪɢɫɬɨɫɬɶ, %

Ⱥɤɭɫɬɢɱɟɫɤɢɣ ɢɦɩɟɞɚɧɫ, 10

ɤɝɦ

137

АКТУАЛЬНЫЕ ВОПРОСЫ ИССЛЕДОВАНИЙ ПЛАСТОВЫХ СИСТЕМ МЕСТОРОЖДЕНИЙ УГЛЕВОДОРОДОВ

ɍɫ ɬ ɚ ɧ ɨ ɜɥ ɟ ɧ ɨ , ɱɬɨ ɬɟɫɧɨɬɚ ɫɜɹɡɢ ɦɟɠɞɭ ɤɨɦɩɥɟɤɫɧɵɦ ɩɚɪɚɦɟ-

ɬɪɨɦ ɢ ɩɨɪɢɫɬɨɫɬɶɸ (ɤɨɷɮɮɢɰɢɟɧɬ ɤɨɪɪɟɥɹɰɢɢ r = 0,97) ɜɵɲɟ, ɱɟɦ

ɩɨɥɭɱɟɧɧɵɟ ɪɚɧɟɟ ɡɧɚɱɟɧɢɹ ɞɥɹ ɫɜɹɡɢ Ɋ

– Ʉ

(r = 0,93) ɢ ǻt – Ʉ

(r = 0,92), ɚ ɬɚɤɠɟ ɛɨɥɟɟ ɜɵɫɨɤɚɹ ɫɬɟɩɟɧɶ ɞɨɫɬɨɜɟɪɧɨɫɬɢ ɚɩɩɪɨɤ-

ɫɢɦɚɰɢɢ R

= 0,97 ɡɚɜɢɫɢɦɨɫɬɢ (5) ɩɨ ɫɪɚɜɧɟɧɢɸ ɫ ɩɨɥɭɱɟɧɧɨɣ ɪɚ-

ɧɟɟ ɫɬɟɩɟɧɶɸ ɞɨɫɬɨɜɟɪɧɨɫɬɢ ɞɥɹ ɭɪɚɜɧɟɧɢɣ (2) (R

= 0,94) ɢ (3)

= 0,91). ɋɨɱɟɬɚɧɢɟ ɛɨɥɟɟ ɜɵɫɨɤɨɣ ɞɨɫɬɨɜɟɪɧɨɫɬɢ ɚɩɩɪɨɤɫɢɦɚ-

ɰɢɢ ɢ ɬɟɫɧɨɬɵ ɫɜɹɡɢ ɩɨɡɜɨɥɹɟɬ ɪɟɤɨɦɟɧɞɨɜɚɬɶ ɤ ɩɪɚɤɬɢɱɟɫɤɨɦɭ ɢɫ-

ɩɨɥɶɡɨɜɚɧɢɸ ɜɵɹɜɥɟɧɧɭɸ ɫɜɹɡɶ ɦɟɠɞɭ ǻt/Ɋ

ɢ Ʉ

(5) ɩɪɢ ɤɨɦɩɥɟɤɫ-

ɧɨɣ ɢɧɬɟɪɩɪɟɬɚɰɢɢ ɞɚɧɧɵɯ ɚɤɭɫɬɢɱɟɫɤɨɝɨ ɢ ɷɥɟɤɬɪɢɱɟɫɤɨɝɨ ɤɚɪɨ-

ɬɚɠɚ ɫɤɜɚɠɢɧ ɫ ɰɟɥɶɸ ɩɨɜɵɲɟɧɢɹ ɬɨɱɧɨɫɬɢ ɨɩɪɟɞɟɥɟɧɢɹ ɩɨɪɢɫɬɨ-

ɫɬɢ ɤɨɥɥɟɤɬɨɪɨɜ.

Проницаемость

ɇɚɢɛɨɥɟɟ ɬɪɭɞɧɵɦ ɜɨɩɪɨɫɨɦ ɹɜɥɹɟɬɫɹ ɨɩɪɟɞɟɥɟɧɢɟ ɝɟɨɮɢɡɢ-

ɱɟɫɤɢɦɢ ɦɟɬɨɞɚɦɢ ɤɨɷɮɮɢɰɢɟɧɬɚ ɩɪɨɧɢɰɚɟɦɨɫɬɢ ɩɨɪɨɞ, ɤɨɬɨɪɨɟ

Рис. 5. Зависимость комплексного параметра 't/P

от пористости образцов

100

0,0 5,0 10,0 15,0 20,0 25,0

ɉɨɪɢɫɬɨɫɬɶ, %

Ʉɨɦɩɥɟɤɫɧɵɣ ɩɚɪɚɦɟɬɪ, ɦɤɫ/ɦ

138

СБОРНИК НАУЧНЫХ СТАТЕЙ

ɜɨɡɦɨɠɧɨ ɩɪɢ ɫɭɳɟɫɬɜɨɜɚɧɢɢ ɧɚɞɟɠɧɵɯ ɩɟɬɪɨɮɢɡɢɱɟɫɤɢɯ ɡɚɜɢɫɢ-

ɦɨɫɬɟɣ ɦɟɠɞɭ ɝɟɨɮɢɡɢɱɟɫɤɢɦɢ ɩɚɪɚɦɟɬɪɚɦɢ ɢ ɩɪɨɧɢɰɚɟɦɨɫɬɶɸ.

ȼ ɨɫɧɨɜɧɨɦ ɩɪɨɧɢɰɚɟɦɨɫɬɶ ɩɥɚɫɬɚ ɨɩɪɟɞɟɥɹɟɬɫɹ ɝɢɞɪɨɞɢɧɚɦɢɱɟ-

ɫɤɢɦɢ ɢɫɫɥɟɞɨɜɚɧɢɹɦɢ ɫɤɜɚɠɢɧ. Ɋɚɫɫɦɨɬɪɢɦ ɜɨɡɦɨɠɧɨɫɬɢ ɦɟɬɨ-

ɞɨɜ Ƚɂɋ ɜ ɨɰɟɧɤɟ ɤɨɷɮɮɢɰɢɟɧɬɚ ɩɪɨɧɢɰɚɟɦɨɫɬɢ.

ɉɪɨɧɢɰɚɟɦɨɫɬɶ ɢ ɩɚɪɚɦɟɬɪ ɩɨɪɢɫɬɨɫɬɢ. Ɂɚɜɢɫɢɦɨɫɬɶ ɩɪɨ-

ɧɢɰɚɟɦɨɫɬɢ ɝɨɪɧɵɯ ɩɨɪɨɞ ɨɬ ɫɬɪɭɤɬɭɪɧɵɯ ɨɫɨɛɟɧɧɨɫɬɟɣ ɨɬɥɨɠɟ-

ɧɢɣ ɨɩɢɫɵɜɚɟɬɫɹ ɭɪɚɜɧɟɧɢɟɦ Ʉɨɡɟɧɢ-Ʉɚɪɦɚɧɚ [3]:

ɩɪ

= Ʉ

/ 2Ɍ

·S

·f, (6)

ɝɞɟ Ɍ

– ɝɢɞɪɚɜɥɢɱɟɫɤɚɹ ɢɡɜɢɥɢɫɬɨɫɬɶ (ɢɡɜɢɥɢɫɬɨɫɬɶ ɷɮɮɟɤɬɢɜ-

ɧɵɯ ɩɨɪɨɜɵɯ ɤɚɧɚɥɨɜ); S

– ɭɞɟɥɶɧɚɹ ɩɨɜɟɪɯɧɨɫɬɶ ɤɚɧɚɥɨɜ ɮɢɥɶ-

ɬɪɚɰɢɢ; f – ɤɨɷɮɮɢɰɢɟɧɬ, ɯɚɪɚɤɬɟɪɢɡɭɸɳɢɣ ɮɨɪɦɭ ɫɟɱɟɧɢɹ ɤɚɩɢɥ-

ɥɹɪɨɜ.

Ɋɚɫɫɦɨɬɪɢɦ ɛɨɥɟɟ ɩɨɞɪɨɛɧɨ ɩɚɪɚɦɟɬɪɵ, ɜɯɨɞɹɳɢɟ ɜ ɭɪɚɜɧɟ-

ɧɢɟ (6). Ɍɚɤ ɤɚɤ ɝɢɞɪɚɜɥɢɱɟɫɤɚɹ ɢɡɜɢɥɢɫɬɨɫɬɶ Ɍ

ɩɪɨɩɨɪɰɢɨɧɚɥɶ-

ɧɚ ɷɥɟɤɬɪɢɱɟɫɤɨɣ Ɍ

[6], ɚ Ɍ

~ Ɋ

·Ʉ

, ɬɨ ɪɨɥɶ ɤɨɷɮɮɢɰɢɟɧɬɚ ɩɨɪɢ-

ɫɬɨɫɬɢ, ɚ ɫɨɨɬɜɟɬɫɬɜɟɧɧɨ ɢ ɩɚɪɚɦɟɬɪɚ ɩɨɪɢɫɬɨɫɬɢ ɜ ɭɪɚɜɧɟɧɢɢ (6),

ɜɟɥɢɤɚ. ɋɥɟɞɨɜɚɬɟɥɶɧɨ, ɢɦɟɸɬɫɹ ɩɪɟɞɩɨɫɵɥɤɢ ɞɥɹ ɢɡɭɱɟɧɢɹ ɫɜɹ-

ɡɢ ɩɚɪɚɦɟɬɪɚ ɩɨɪɢɫɬɨɫɬɢ ɢ ɞɚɧɧɵɯ Ƚɂɋ, ɨɛɭɫɥɨɜɥɟɧɧɵɯ ɩɨɪɢɫɬɨ-

ɫɬɶɸ ɢ ɤɨɷɮɮɢɰɢɟɧɬɨɦ ɩɪɨɧɢɰɚɟɦɨɫɬɢ. ɋɨɝɥɚɫɧɨ ɪɢɫ. 6 ɷɤɫɩɟɪɢ-

ɦɟɧɬɚɥɶɧɨ ɩɨɥɭɱɟɧɧɚɹ ɡɚɜɢɫɢɦɨɫɬɶ ɩɚɪɚɦɟɬɪɚ ɩɨɪɢɫɬɨɫɬɢ ɨɬ ɤɨ-

ɷɮɮɢɰɢɟɧɬɚ ɩɪɨɧɢɰɚɟɦɨɫɬɢ ɫ ɜɵɫɨɤɨɣ ɫɬɟɩɟɧɶɸ ɞɨɫɬɨɜɟɪɧɨɫɬɢ

= 0,90 ɦɨɠɟɬ ɛɵɬɶ ɨɩɢɫɚɧɚ ɫɬɟɩɟɧɧɨɣ ɡɚɜɢɫɢɦɨɫɬɶɸ ɜɢɞɚ:

= 51,725 / Ʉ

ɩɪ

0,204

. (7)

ɋɥɟɞɭɟɬ ɨɬɦɟɬɢɬɶ, ɱɬɨ ɬɟɫɧɨɬɚ ɫɜɹɡɢ ɦɟɠɞɭ ɩɪɨɧɢɰɚɟɦɨɫɬɶɸ

ɢ ɩɚɪɚɦɟɬɪɨɦ ɩɨɪɢɫɬɨɫɬɢ (ɤɨɷɮɮɢɰɢɟɧɬ ɤɨɪɪɟɥɹɰɢɢ r = –0,53) ɞɨ-

ɜɨɥɶɧɨ ɧɢɡɤɚɹ. ȼ ɫɜɹɡɢ ɫ ɷɬɢɦ ɡɚɜɢɫɢɦɨɫɬɶ (7) ɦɨɠɟɬ ɛɵɬɶ ɢɫɩɨɥɶ-

ɡɨɜɚɧɚ ɥɢɲɶ ɞɥɹ ɩɪɟɞɜɚɪɢɬɟɥɶɧɨɣ ɨɰɟɧɤɢ ɡɧɚɱɟɧɢɣ ɩɪɨɧɢɰɚɟɦɨ-

ɫɬɢ ɤɨɥɥɟɤɬɨɪɨɜ ɢɫɫɥɟɞɭɟɦɨɝɨ ɨɛɴɟɤɬɚ ɩɨ ɞɚɧɧɵɦ ɷɥɟɤɬɪɨɦɟɬɪɢɢ

ɫɤɜɚɠɢɧ.

ɉɪɨɧɢɰɚɟɦɨɫɬɶ ɢ ɢɧɬɟɪɜɚɥɶɧɨɟ ɜɪɟɦɹ. Ɂɚɜɢɫɢɦɨɫɬɶ ɩɪɨɧɢ-

ɰɚɟɦɨɫɬɢ ɨɬ ɢɧɬɟɪɜɚɥɶɧɨɝɨ ɜɪɟɦɟɧɢ ɦɨɠɧɨ ɨɛ

ɴɹɫɧɢɬɶ ɢɯ ɬɟɫɧɨɣ

ɡɚɜɢɫɢɦɨɫɬɶɸ ɨɬ ɩɨɪɢɫɬɨɫɬɢ ɩɨɪɨɞ. ɗɬɨ ɩɨɫɥɭɠɢɥɨ ɨɫɧɨɜɚɧɢɟɦ

139

АКТУАЛЬНЫЕ ВОПРОСЫ ИССЛЕДОВАНИЙ ПЛАСТОВЫХ СИСТЕМ МЕСТОРОЖДЕНИЙ УГЛЕВОДОРОДОВ

ɞɥɹ ɫɨɩɨɫɬɚɜɥɟɧɢɹ ɢɡɦɟɧɟɧɢɣ ɢɧɬɟɪɜɚɥɶɧɨɝɨ ɜɪɟɦɟɧɢ ɢ ɩɪɨɧɢɰɚ-

ɟɦɨɫɬɢ. ɉɨɥɭɱɟɧɧɵɟ ɪɟɡɭɥɶɬɚɬɵ ɯɚɪɚɤɬɟɪɢɡɭɸɬɫɹ ɜɵɫɨɤɨɣ ɞɨɫɬɨ-

ɜɟɪɧɨɫɬɶɸ ɚɩɩɪɨɤɫɢɦɚɰɢɢ R

= 0,75 ɷɬɢɯ ɡɚɜɢɫɢɦɨɫɬɟɣ ɥɨɝɚɪɢɮ-

ɦɢɱɟɫɤɢɦ ɭɪɚɜɧɟɧɢɟɦ (ɪɢɫ. 7):

ǻt = 8,83Ln(Ʉ

ɩɪ

) + 258,6. (8)

ɋɥɟɞɭɟɬ ɨɬɦɟɬɢɬɶ, ɱɬɨ ɬɟɫɧɨɬɚ ɫɜɹɡɢ ɦɟɠɞɭ ɢɧɬɟɪɜɚɥɶɧɵɦ ɜɪɟ-

ɦɟɧɟɦ ɢ ɩɪɨɧɢɰɚɟɦɨɫɬɶɸ (ɤɨɷɮɮɢɰɢɟɧɬ ɤɨɪɪɟɥɹɰɢɢ r = 0,55) ɞɨ-

ɜɨɥɶɧɨ ɧɢɡɤɚɹ. ɉɨɷɬɨɦɭ ɜɵɹɜɥɟɧɧɚɹ ɫɜɹɡɶ ɦɟɠɞɭ ɢɧɬɟɪɜɚɥɶɧɵɦ

ɜɪɟɦɟɧɟɦ ɢ ɩɪɨɧɢɰɚɟɦɨɫɬɶɸ ɢɫɫɥɟɞɨɜɚɧɧɨɣ ɤɨɥɥɟɤɰɢɢ ɨɛɪɚɡ-

ɰɨɜ (8), ɩɨ ɦɧɟɧɢɸ ɚɜɬɨɪɨɜ, ɦɨɠɟɬ ɛɵɬɶ ɢɫɩɨɥɶɡɨɜɚɧɚ ɩɪɢ ɢɧɬɟɪ-

ɩɪɟɬɚɰɢɢ ɞɚɧɧɵɯ ɚɤɭɫɬɢɱɟɫɤɨɝɨ ɤɚɪɨɬɚɠɚ ɫɤɜɚɠɢɧ ɫ ɰɟɥɶɸ ɨɰɟɧ-

ɤɢ ɩɪɨɧɢɰɚɟɦɨɫɬɢ ɤɨɥɥɟɤɬɨɪɨɜ ɫ ɜɵɫɨɤɨɣ ɫɬɟɩɟɧɶɸ ɨɫɬɨɪɨɠɧɨɫɬɢ

ɢ ɬɨɥɶɤɨ ɜ ɤɨɦɩɥɟɤɫɟ ɫ ɞɪɭɝɢɦɢ ɦɟɬɨɞɚɦɢ.

ɉɪɨɧɢɰɚɟɦɨɫɬɶ ɢ ɚɤɭɫɬɢɱɟɫɤɢɣ ɢɦɩɟɞɚɧɫ. ɋɨɝɥɚɫɧɨ ɪɢɫ. 7

ɧɚ ɡɚɜɢɫɢɦɨɫɬɶ ɢɧɬɟɪɜɚɥɶɧɨɝɨ ɜɪɟɦɟɧɢ ɨɬ ɩɪɨɧɢɰɚɟɦɨɫɬɢ ɧɚɤɥɚ-

Рис. 6. Зависимость проницаемости от параметра пористости

10,0

100,0

0,1 1,0 10,0 100,0 1000,0

ɉɪɨɧɢɰɚɟɦɨɫɬɶ, ɦȾ

ɉɚɪɚɦɟɬɪ ɩɨɪɢɫɬɨɫɬɢ

140

СБОРНИК НАУЧНЫХ СТАТЕЙ

ɞɵɜɚɸɬɫɹ ɢ ɞɪɭɝɢɟ ɮɚɤɬɨɪɵ, ɤɨɬɨɪɵɟ ɮɨɪɦɢɪɭɸɬ ɡɧɚɱɢɬɟɥɶɧɵɣ

ɪɚɡɛɪɨɫ ɞɚɧɧɵɯ. ɇɚɢɛɨɥɟɟ ɫɢɥɶɧɨɟ ɜɥɢɹɧɢɟ ɧɚ ɚɤɭɫɬɢɱɟɫɤɢɟ ɯɚ-

ɪɚɤɬɟɪɢɫɬɢɤɢ ɨɤɚɡɵɜɚɟɬ ɩɥɨɬɧɨɫɬɶ ɨɬɥɨɠɟɧɢɣ, ɤɨɬɨɪɚɹ ɩɨ ɢɫɫɥɟɞɨ-

ɜɚɧɧɨɣ ɤɨɥɥɟɤɰɢɢ ɢɡɦɟɧɹɟɬɫɹ ɨɬ 2,00 ɞɨ 2,51 ɝ/ɫɦ

. ȼɥɢɹɧɢɟ ɩɥɨɬ-

ɧɨɫɬɢ ɨɬɥɨɠɟɧɢɣ ɦɨɠɧɨ ɭɱɟɫɬɶ, ɢɫɩɨɥɶɡɭɹ ɢɧɬɟɝɪɚɥɶɧɭɸ ɯɚɪɚɤɬɟ-

ɪɢɫɬɢɤɭ ɨɬɥɨɠɟɧɢɣ – ɚɤɭɫɬɢɱɟɫɤɢɣ ɢɦɩɟɞɚɧɫ, ɤɨɬɨɪɵɣ ɜɵɱɢɫɥɹɟɬ-

ɫɹ ɤɚɤ ɩɪɨɢɡɜɟɞɟɧɢɟ ɩɥɨɬɧɨɫɬɢ ɢ ɫɤɨɪɨɫɬɢ ɩɪɨɞɨɥɶɧɨɣ ɜɨɥɧɵ ɝɨɪ-

ɧɨɣ ɩɨɪɨɞɵ.

ɉɪɢɜɟɞɟɧɧɵɟ ɧɚ ɪɢɫ. 8 ɞɚɧɧɵɟ ɚɤɭɫɬɢɱɟɫɤɨɝɨ ɢɦɩɟɞɚɧɫɚ ɢ ɩɪɨ-

ɧɢɰɚɟɦɨɫɬɢ ɞɥɹ ɢɫɫɥɟɞɨɜɚɧɧɵɯ ɨɛɪɚɡɰɨɜ ɦɨɠɧɨ ɚɩɩɪɨɤɫɢɦɢɪɨ-

ɜɚɬɶ ɫɨ ɫɬɟɩɟɧɶɸ ɞɨɫɬɨɜɟɪɧɨɫɬɢ R

= 0,79 ɤɚɤ ɥɨɝɚɪɢɮɦɢɱɟɫɤɭɸ

ɡɚɜɢɫɢɦɨɫɬɶ ɦɟɠɞɭ ɚɤɭɫɬɢɱɟɫɤɢɦ ɢɦɩɟɞɚɧɫɨɦ Z ɢ ɩɪɨɧɢɰɚɟɦɨ-

ɫɬɶɸ Ʉ

ɩɪ

Z = 9,19 – 0,425Ln(Ʉ

ɩɪ

). (9)

Рис. 7. Зависимость интервального времени от проницаемости

200

220

240

260

280

300

320

340

0,1 1,0 10,0 100,0 1000,0

ɉɪɨɧɢɰɚɟɦɨɫɬɶ, ɦȾ

ɂɧɬɟɪɜɚɥɶɧɨɟ ɜɪɟɦɹ, ɦɤɫ/ɦ