\[
\frac{\partial u_e}{\partial t} = C_v \cdot \frac{\partial^2 u_e}{\partial z^2}
\]
3차원 확장:
\[
\frac{\partial u_e}{\partial t} = C_v \left( \frac{\partial^2 u_e}{\partial z^2} + \frac{\partial^2 u_e}{\partial x^2} + \frac{\partial^2 u_e}{\partial y^2} \right)
\]
\[
C_\alpha = \frac{\Delta e}{\Delta \log t}, \quad
\varepsilon_\alpha = \frac{\Delta H}{H_p \cdot \Delta \log t} = \frac{C_\alpha}{1 + e}
\]
2차 침하량:
\[
S_s = \frac{C_\alpha}{1 + e_p} H_p \log \left( \frac{t_2}{t_1} \right)
\]
기본 침하식:
\[
S = \frac{\Delta e}{1 + e} \cdot H
\]
압축지수 활용:
\[
S = \frac{C_c}{1 + e_0} \cdot H \cdot \log \left( \frac{P_0 + \Delta P}{P_0} \right)
\]
\[
t = \frac{T_v \cdot H^2}{C_v}, \quad
C_v = \frac{T_v}{t_{50}} H^2 = \frac{0.197 H^2}{t_{50}} = \frac{0.848 H^2}{t_{90}}
\]
평균압밀도 기준:
\[
T_v = \frac{\pi}{4} \left( \frac{\bar{U}}{100} \right)^2
\quad \text{또는} \quad
T_v = 1.781 - 0.933 \log (100 - U)
\]
\[
OCR = \frac{P_c}{P_0} = \frac{\text{선행압밀압력}}{\text{현재 유효 상재압력}}
\]
잔류침하 기준:
\[
\bar{U} \geq 90\% \quad \text{또는} \quad \text{잔류침하량 } \leq 10\text{cm}
\]