Differenze tra le versioni di "Progettazione geotecnica"
(Pagina sostituita con '= PROGETTAZIONE GEOTECNICA = == Indice dei Brick == * Indice * Figure * Progettazione_geotecnic...') (Etichetta: Sostituito) |
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Riga 1: | Riga 1: | ||
− | = | + | {{EquationPg|pg=p.'''003'''|eq=<math> E_d \leq R_d</math>|id=1.1}} |
+ | LaTeX → E_d \leq R_d | ||
− | == | + | {{EquationPg|pg=p.'''004'''|eq=<math> E_d=E\left[\gamma_F F_k ; \frac{X_k}{\gamma_M} ; a_d\right]</math>|}} |
+ | LaTeX → E_d=E\left[\gamma_F F_k ; \frac{X_k}{\gamma_M} ; a_d\right] | ||
− | + | {{EquationPg|pg=p.'''004'''|eq=<math> E_d=\gamma_E E\left[F_k ; \frac{X_k}{\gamma_M} ; {a}_d\right] \quad\left(\gamma_E=\gamma_F\right)</math>|}} | |
− | + | LaTeX → E_d=\gamma_E E\left[F_k ; \frac{X_k}{\gamma_M} ; {a}_d\right] \quad\left(\gamma_E=\gamma_F\right) | |
− | + | ||
− | + | {{EquationPg|pg=p.'''004'''|eq=<math> R_d=\frac{1}{\gamma_R}\left[\gamma_F F_k ; \frac{X_k}{\gamma_M} ; {a}_d\right]</math>|}} | |
− | + | LaTeX → R_d=\frac{1}{\gamma_R}\left[\gamma_F F_k ; \frac{X_k}{\gamma_M} ; {a}_d\right] | |
+ | |||
+ | {{EquationPg|pg=p.'''004'''|eq=<math> E_d \leq R_d</math>|}} | ||
+ | LaTeX → E_d \leq R_d | ||
+ | |||
+ | {{EquationPg|pg=p.'''004'''|eq=<math> E_d=E\left[\gamma_F F_k ; \frac{X_k}{\gamma_M} ; a_d\right]</math>|id=1.2}} | ||
+ | LaTeX → E_d=E\left[\gamma_F F_k ; \frac{X_k}{\gamma_M} ; a_d\right] | ||
+ | |||
+ | {{EquationPg|pg=p.'''004'''|eq=<math> E_d=\gamma_E E\left[F_k ; \frac{X_k}{\gamma_M} ; {a}_d\right]</math>|id=1.2}} | ||
+ | LaTeX → E_d=\gamma_E E\left[F_k ; \frac{X_k}{\gamma_M} ; {a}_d\right] | ||
+ | |||
+ | {{EquationPg|pg=p.'''004'''|eq=<math> R_d=\frac{1}{\gamma_R} R\left[\gamma_F F_k ; \frac{X_k}{\gamma_M} ; {a}_d\right]</math>|id=1.3}} | ||
+ | LaTeX → R_d=\frac{1}{\gamma_R} R\left[\gamma_F F_k ; \frac{X_k}{\gamma_M} ; {a}_d\right] | ||
+ | |||
+ | {{EquationPg|pg=p.'''005'''|eq=<math> \gamma_{G1} \cdot G_1+\gamma_{G2} \cdot G_{2}+\gamma_P \cdot P+\gamma_{Q1} \cdot Q_{k1} +\gamma_{Q2} \cdot \Psi_{02} \cdot Q_{k2}+\gamma_{Q3} \cdot \Psi_{03} \cdot Q_{k 3}+\ldots</math>|id=1.4}} | ||
+ | LaTeX → \gamma_{G1} \cdot G_1+\gamma_{G2} \cdot G_{2}+\gamma_P \cdot P+\gamma_{Q1} \cdot Q_{k1} +\gamma_{Q2} \cdot \Psi_{02} \cdot Q_{k2}+\gamma_{Q3} \cdot \Psi_{03} \cdot Q_{k 3}+\ldots | ||
+ | |||
+ | {{EquationPg|pg=p.'''007'''|eq=<math> DA1-C1 : (A1+M1+R1)</math>|id=1.5}} | ||
+ | LaTeX → DA1-C1 : (A1+M1+R1) | ||
+ | |||
+ | {{EquationPg|pg=p.'''007'''|eq=<math> DA1-C2 : (A2+M2+R2)</math>|id=1.6}} | ||
+ | LaTeX → DA1-C2 : (A2+M2+R2) | ||
+ | |||
+ | {{EquationPg|pg=p.'''007'''|eq=<math> DA2 : (A1+M1+R3)</math>|id=1.7}} | ||
+ | LaTeX → DA2 : (A1+M1+R3) | ||
+ | |||
+ | {{EquationPg|pg=p.'''008'''|eq=<math> G_{1k}+G_{2k}+\psi_{21} Q_{k1}+\psi_{22} Q_{k2}+\ldots</math>|}} | ||
+ | LaTeX → G_{1k}+G_{2k}+\psi_{21} Q_{k1}+\psi_{22} Q_{k2}+\ldots | ||
+ | |||
+ | {{EquationPg|pg=p.'''008'''|eq=<math> E_d=E\left[F_d ; X_k ; {a}_d\right]</math>|}} | ||
+ | LaTeX → E_d=E\left[F_d ; X_k ; {a}_d\right] | ||
+ | |||
+ | {{EquationPg|pg=p.'''008'''|eq=<math> E_d \leq C_d</math>|}} | ||
+ | LaTeX → E_d \leq C_d | ||
+ | |||
+ | {{EquationPg|pg=p.'''011'''|eq=<math> \sigma_{ij}^\prime=\sigma_{ij}-u \delta_{ij}</math>|id=1.8}} | ||
+ | LaTeX → \sigma_{ij}^\prime=\sigma_{ij}-u \delta_{ij} | ||
+ | |||
+ | {{EquationPg|pg=p.'''011'''|eq=<math> \tau=\sigma^\prime \cdot \tan \varphi^\prime</math>|id=1.9}} | ||
+ | LaTeX → \tau=\sigma^\prime \cdot \tan \varphi^\prime | ||
+ | |||
+ | {{EquationPg|pg=p.'''012'''|eq=<math> \tau=c^\prime+\sigma^\prime \cdot \tan \varphi^\prime</math>|id=1.10}} | ||
+ | LaTeX → \tau=c^\prime+\sigma^\prime \cdot \tan \varphi^\prime | ||
+ | |||
+ | {{EquationPg|pg=p.'''016'''|eq=<math> \varphi^\prime-\varphi_{cv}^\prime=m \cdot DI <12^\circ</math>|id=1.11}} | ||
+ | LaTeX → \varphi^\prime-\varphi_{cv}^\prime=m \cdot DI <12^\circ | ||
+ | |||
+ | {{EquationPg|pg=p.'''016'''|eq=<math> DI=D_R\left(10-\ln \left(p_F^\prime\right)\right)-1</math>|id=1.11}} | ||
+ | LaTeX → DI=D_R\left(10-\ln \left(p_F^\prime\right)\right)-1 | ||
+ | |||
+ | {{EquationPg|pg=p.'''023'''|eq=<math> \tau=C_u</math>|id=1.12}} | ||
+ | LaTeX → \tau=C_u | ||
+ | |||
+ | {{EquationPg|pg=p.'''024'''|eq=<math> \frac{c_u}{\sigma_{v 0}^\prime}=0.23 \cdot OCR^{0.8}</math>|id=1.13}} | ||
+ | LaTeX → \frac{c_u}{\sigma_{v 0}^\prime}=0.23 \cdot OCR^{0.8} | ||
+ | |||
+ | {{EquationPg|pg=p.'''026'''|eq=<math> E + G_1 + G_2 + P + \psi_{21} \cdot Q_{k1} + \psi_{22} \cdot Q_{k2}+\ldots</math>|id=1.14}} | ||
+ | LaTeX → E + G_1 + G_2 + P + \psi_{21} \cdot Q_{k1} + \psi_{22} \cdot Q_{k2}+\ldots | ||
+ | |||
+ | {{EquationPg|pg=p.'''027'''|eq=<math> E_d=E_k=E \left[F_k ; X_k ; a_d\right]</math>|}} | ||
+ | LaTeX → E_d=E_k=E \left[F_k ; X_k ; a_d\right] | ||
+ | |||
+ | {{EquationPg|pg=p.'''027'''|eq=<math> R_d=\frac{1}{\gamma_R}\left[F_k ; X_k ; a_d\right]</math>|}} | ||
+ | LaTeX → R_d=\frac{1}{\gamma_R}\left[F_k ; X_k ; a_d\right] | ||
+ | |||
+ | {{EquationPg|pg=p.'''027'''|eq=<math> E_d \leq R_d</math>|}} | ||
+ | LaTeX → E_d \leq R_d | ||
+ | |||
+ | {{EquationPg|pg=p.'''028'''|eq=<math> E_d=E \left[F_k ; X_k ; a_d\right]</math>|}} | ||
+ | LaTeX → E_d=E \left[F_k ; X_k ; a_d\right] | ||
+ | |||
+ | {{EquationPg|pg=p.'''028'''|eq=<math> E_d \leq C_d</math>|}} | ||
+ | LaTeX → E_d \leq C_d | ||
+ | |||
+ | {{EquationPg|pg=p.'''029'''|eq=<math> T_R=-\frac{V_R}{\ln \left(1-P_{VR}\right)}</math>|id=1.15}} | ||
+ | LaTeX → T_R=-\frac{V_R}{\ln \left(1-P_{VR}\right)} | ||
+ | |||
+ | {{EquationPg|pg=p.'''032'''|eq=<math> S=S_S \cdot S_T</math>|id=1.16}} | ||
+ | LaTeX → S=S_S \cdot S_T | ||
+ | |||
+ | {{EquationPg|pg=p.'''032'''|eq=<math> V_{S, eq}=\frac{H}{\sum_{i=1}^{N} \frac{h_i}{V_{S, i}}}</math>|id=1.17}} | ||
+ | LaTeX → V_{S, eq}=\frac{H}{\sum_{i=1}^{N} \frac{h_i}{V_{S, i}}} | ||
+ | |||
+ | {{EquationPg|pg=p.'''036'''|eq=<math> a_{\max }=S \cdot a_G=\left(S_s \cdot S_T\right) \cdot a_G</math>|id=1.18}} | ||
+ | LaTeX → a_{\max }=S \cdot a_G=\left(S_s \cdot S_T\right) \cdot a_G | ||
+ | |||
+ | {{EquationPg|pg=p.'''037'''|eq=<math> F_h=k_h \cdot {W}</math>|id=1.19}} | ||
+ | LaTeX → F_h=k_h \cdot {W} | ||
+ | |||
+ | {{EquationPg|pg=p.'''037'''|eq=<math> F_v=k_v \cdot {W}</math>|id=1.20}} | ||
+ | LaTeX → F_v=k_v \cdot {W} | ||
+ | |||
+ | {{EquationPg|pg=p.'''038'''|eq=<math> k_h=\beta \cdot \frac{a_\max}{g}</math>|id=1.21}} | ||
+ | LaTeX → k_h=\beta \cdot \frac{a_\max}{g} | ||
+ | |||
+ | {{EquationPg|pg=p.'''038'''|eq=<math> k_v=\pm 0,5 \cdot k_h</math>|id=1.22}} | ||
+ | LaTeX → k_v=\pm 0,5 \cdot k_h | ||
+ | |||
+ | {{EquationPg|pg=p.'''039'''|eq=<math> k_h=\alpha \cdot \beta \cdot \frac{a_\max}{g}</math>|id=1.23}} | ||
+ | LaTeX → k_h=\alpha \cdot \beta \cdot \frac{a_\max}{g} |
Versione delle 17:45, 9 lug 2019
p.003 | (1.1) |
LaTeX → E_d \leq R_d
p.004 |
LaTeX → E_d=E\left[\gamma_F F_k ; \frac{X_k}{\gamma_M} ; a_d\right]
p.004 |
LaTeX → E_d=\gamma_E E\left[F_k ; \frac{X_k}{\gamma_M} ; {a}_d\right] \quad\left(\gamma_E=\gamma_F\right)
p.004 |
LaTeX → R_d=\frac{1}{\gamma_R}\left[\gamma_F F_k ; \frac{X_k}{\gamma_M} ; {a}_d\right]
p.004 |
LaTeX → E_d \leq R_d
p.004 | (1.2) |
LaTeX → E_d=E\left[\gamma_F F_k ; \frac{X_k}{\gamma_M} ; a_d\right]
p.004 | (1.2) |
LaTeX → E_d=\gamma_E E\left[F_k ; \frac{X_k}{\gamma_M} ; {a}_d\right]
p.004 | (1.3) |
LaTeX → R_d=\frac{1}{\gamma_R} R\left[\gamma_F F_k ; \frac{X_k}{\gamma_M} ; {a}_d\right]
p.005 | (1.4) |
LaTeX → \gamma_{G1} \cdot G_1+\gamma_{G2} \cdot G_{2}+\gamma_P \cdot P+\gamma_{Q1} \cdot Q_{k1} +\gamma_{Q2} \cdot \Psi_{02} \cdot Q_{k2}+\gamma_{Q3} \cdot \Psi_{03} \cdot Q_{k 3}+\ldots
p.007 | (1.5) |
LaTeX → DA1-C1 : (A1+M1+R1)
p.007 | (1.6) |
LaTeX → DA1-C2 : (A2+M2+R2)
p.007 | (1.7) |
LaTeX → DA2 : (A1+M1+R3)
p.008 |
LaTeX → G_{1k}+G_{2k}+\psi_{21} Q_{k1}+\psi_{22} Q_{k2}+\ldots
p.008 |
LaTeX → E_d=E\left[F_d ; X_k ; {a}_d\right]
p.008 |
LaTeX → E_d \leq C_d
p.011 | (1.8) |
LaTeX → \sigma_{ij}^\prime=\sigma_{ij}-u \delta_{ij}
p.011 | (1.9) |
LaTeX → \tau=\sigma^\prime \cdot \tan \varphi^\prime
p.012 | (1.10) |
LaTeX → \tau=c^\prime+\sigma^\prime \cdot \tan \varphi^\prime
p.016 | (1.11) |
LaTeX → \varphi^\prime-\varphi_{cv}^\prime=m \cdot DI <12^\circ
p.016 | (1.11) |
LaTeX → DI=D_R\left(10-\ln \left(p_F^\prime\right)\right)-1
p.023 | (1.12) |
LaTeX → \tau=C_u
p.024 | (1.13) |
LaTeX → \frac{c_u}{\sigma_{v 0}^\prime}=0.23 \cdot OCR^{0.8}
p.026 | (1.14) |
LaTeX → E + G_1 + G_2 + P + \psi_{21} \cdot Q_{k1} + \psi_{22} \cdot Q_{k2}+\ldots
p.027 |
LaTeX → E_d=E_k=E \left[F_k ; X_k ; a_d\right]
p.027 |
LaTeX → R_d=\frac{1}{\gamma_R}\left[F_k ; X_k ; a_d\right]
p.027 |
LaTeX → E_d \leq R_d
p.028 |
LaTeX → E_d=E \left[F_k ; X_k ; a_d\right]
p.028 |
LaTeX → E_d \leq C_d
p.029 | (1.15) |
LaTeX → T_R=-\frac{V_R}{\ln \left(1-P_{VR}\right)}
p.032 | (1.16) |
LaTeX → S=S_S \cdot S_T
p.032 | (1.17) |
LaTeX → V_{S, eq}=\frac{H}{\sum_{i=1}^{N} \frac{h_i}{V_{S, i}}}
p.036 | (1.18) |
LaTeX → a_{\max }=S \cdot a_G=\left(S_s \cdot S_T\right) \cdot a_G
p.037 | (1.19) |
LaTeX → F_h=k_h \cdot {W}
p.037 | (1.20) |
LaTeX → F_v=k_v \cdot {W}
p.038 | (1.21) |
LaTeX → k_h=\beta \cdot \frac{a_\max}{g}
p.038 | (1.22) |
LaTeX → k_v=\pm 0,5 \cdot k_h
p.039 | (1.23) |
LaTeX → k_h=\alpha \cdot \beta \cdot \frac{a_\max}{g}