Der Modul…
…ergibt sich aus:[ 1]
(
K
,
E
)
{\displaystyle (K,\,E)}
(
K
,
λ
)
{\displaystyle (K,\,\lambda )}
(
K
,
G
)
{\displaystyle (K,\,G)}
(
K
,
ν
)
{\displaystyle (K,\,\nu )}
(
E
,
λ
)
{\displaystyle (E,\,\lambda )}
(
E
,
G
)
{\displaystyle (E,\,G)}
(
E
,
ν
)
{\displaystyle (E,\,\nu )}
(
λ
,
G
)
{\displaystyle (\lambda ,\,G)}
(
λ
,
ν
)
{\displaystyle (\lambda ,\,\nu )}
(
G
,
ν
)
{\displaystyle (G,\,\nu )}
(
G
,
M
)
{\displaystyle (G,\,M)}
Kompressionsmodul
K
{\displaystyle K\,}
K
{\displaystyle K}
K
{\displaystyle K}
K
{\displaystyle K}
K
{\displaystyle K}
(
E
+
3
λ
)
/
6
+
{\displaystyle (E+3\lambda )/6+}
(
E
+
3
λ
)
2
−
4
λ
E
6
{\displaystyle {\tfrac {\sqrt {(E+3\lambda )^{2}-4\lambda E}}{6}}}
E
G
3
(
3
G
−
E
)
{\displaystyle {\tfrac {EG}{3(3G-E)}}}
E
3
(
1
−
2
ν
)
{\displaystyle {\tfrac {E}{3(1-2\nu )}}}
λ
+
{\displaystyle \lambda +}
2
G
3
{\displaystyle {\tfrac {2G}{3}}}
λ
(
1
+
ν
)
3
ν
{\displaystyle {\tfrac {\lambda (1+\nu )}{3\nu }}}
2
G
(
1
+
ν
)
3
(
1
−
2
ν
)
{\displaystyle {\tfrac {2G(1+\nu )}{3(1-2\nu )}}}
M
−
{\displaystyle M-}
4
G
3
{\displaystyle {\tfrac {4G}{3}}}
Elastizitätsmodul
E
{\displaystyle E\,}
E
{\displaystyle E}
9
K
(
K
−
λ
)
3
K
−
λ
{\displaystyle {\tfrac {9K(K-\lambda )}{3K-\lambda }}}
9
K
G
3
K
+
G
{\displaystyle {\tfrac {9KG}{3K+G}}}
3
K
(
1
−
2
ν
)
{\displaystyle 3K(1-2\nu )\,}
E
{\displaystyle E}
E
{\displaystyle E}
E
{\displaystyle E}
G
(
3
λ
+
2
G
)
λ
+
G
{\displaystyle {\tfrac {G(3\lambda +2G)}{\lambda +G}}}
λ
(
1
+
ν
)
(
1
−
2
ν
)
ν
{\displaystyle {\tfrac {\lambda (1+\nu )(1-2\nu )}{\nu }}}
2
G
(
1
+
ν
)
{\displaystyle 2G(1+\nu )\,}
G
(
3
M
−
4
G
)
M
−
G
{\displaystyle {\tfrac {G(3M-4G)}{M-G}}}
1. Lamé-Konstante
λ
{\displaystyle \lambda \,}
3
K
(
3
K
−
E
)
9
K
−
E
{\displaystyle {\tfrac {3K(3K-E)}{9K-E}}}
λ
{\displaystyle \lambda }
K
−
{\displaystyle K-}
2
G
3
{\displaystyle {\tfrac {2G}{3}}}
3
K
ν
1
+
ν
{\displaystyle {\tfrac {3K\nu }{1+\nu }}}
λ
{\displaystyle \lambda }
G
(
E
−
2
G
)
3
G
−
E
{\displaystyle {\tfrac {G(E-2G)}{3G-E}}}
E
ν
(
1
+
ν
)
(
1
−
2
ν
)
{\displaystyle {\tfrac {E\nu }{(1+\nu )(1-2\nu )}}}
λ
{\displaystyle \lambda }
λ
{\displaystyle \lambda }
2
G
ν
1
−
2
ν
{\displaystyle {\tfrac {2G\nu }{1-2\nu }}}
M
−
2
G
{\displaystyle M-2G\,}
Schubmodul
G
{\displaystyle G}
bzw.
μ
{\displaystyle \mu }
(2. Lamé-Konstante)
3
K
E
9
K
−
E
{\displaystyle {\tfrac {3KE}{9K-E}}}
3
(
K
−
λ
)
2
{\displaystyle {\tfrac {3(K-\lambda )}{2}}}
G
{\displaystyle G}
3
K
(
1
−
2
ν
)
2
(
1
+
ν
)
{\displaystyle {\tfrac {3K(1-2\nu )}{2(1+\nu )}}}
(
E
−
3
λ
)
+
{\displaystyle (E-3\lambda )+}
(
E
−
3
λ
)
2
+
8
λ
E
4
{\displaystyle {\tfrac {\sqrt {(E-3\lambda )^{2}+8\lambda E}}{4}}}
G
{\displaystyle G}
E
2
(
1
+
ν
)
{\displaystyle {\tfrac {E}{2(1+\nu )}}}
G
{\displaystyle G}
λ
(
1
−
2
ν
)
2
ν
{\displaystyle {\tfrac {\lambda (1-2\nu )}{2\nu }}}
G
{\displaystyle G}
G
{\displaystyle G}
Poissonzahl
ν
{\displaystyle \nu \,}
3
K
−
E
6
K
{\displaystyle {\tfrac {3K-E}{6K}}}
λ
3
K
−
λ
{\displaystyle {\tfrac {\lambda }{3K-\lambda }}}
3
K
−
2
G
2
(
3
K
+
G
)
{\displaystyle {\tfrac {3K-2G}{2(3K+G)}}}
ν
{\displaystyle \nu }
−
(
E
+
λ
)
+
{\displaystyle -(E+\lambda )+}
(
E
+
λ
)
2
+
8
λ
2
4
λ
{\displaystyle {\tfrac {\sqrt {(E+\lambda )^{2}+8\lambda ^{2}}}{4\lambda }}}
E
2
G
{\displaystyle {\tfrac {E}{2G}}}
−
1
{\displaystyle -1}
ν
{\displaystyle \nu }
λ
2
(
λ
+
G
)
{\displaystyle {\tfrac {\lambda }{2(\lambda +G)}}}
ν
{\displaystyle \nu }
ν
{\displaystyle \nu }
M
−
2
G
2
M
−
2
G
{\displaystyle {\tfrac {M-2G}{2M-2G}}}
Longitudinalmodul
M
{\displaystyle M\,}
3
K
(
3
K
+
E
)
9
K
−
E
{\displaystyle {\tfrac {3K(3K+E)}{9K-E}}}
3
K
−
2
λ
{\displaystyle 3K-2\lambda \,}
K
+
{\displaystyle K+}
4
G
3
{\displaystyle {\tfrac {4G}{3}}}
3
K
(
1
−
ν
)
1
+
ν
{\displaystyle {\tfrac {3K(1-\nu )}{1+\nu }}}
E
−
λ
+
E
2
+
9
λ
2
+
2
E
λ
2
{\displaystyle {\tfrac {E-\lambda +{\sqrt {E^{2}+9\lambda ^{2}+2E\lambda }}}{2}}}
G
(
4
G
−
E
)
3
G
−
E
{\displaystyle {\tfrac {G(4G-E)}{3G-E}}}
E
(
1
−
ν
)
(
1
+
ν
)
(
1
−
2
ν
)
{\displaystyle {\tfrac {E(1-\nu )}{(1+\nu )(1-2\nu )}}}
λ
+
2
G
{\displaystyle \lambda +2G\,}
λ
(
1
−
ν
)
ν
{\displaystyle {\tfrac {\lambda (1-\nu )}{\nu }}}
2
G
(
1
−
ν
)
1
−
2
ν
{\displaystyle {\tfrac {2G(1-\nu )}{1-2\nu }}}
M
{\displaystyle M}