The fixed end moments are reaction moments developed in a beam member under certain load conditions with both ends fixed. A beam with both ends fixed is statically indeterminate to the 3rd degree, and any structural analysis method applicable on statically indeterminate beams can be used to calculate the fixed end moments.
In the following examples, clockwise moments are positive.
The two cases with distributed loads can be derived from the case with concentrated load by integration. For example, when a uniformly distributed load of intensity
q
dx
x
qdx
fixed | |
M | |
right |
=
L | |
\int | |
0 |
qdxx2(L-x) | |
L2 |
=
qL2 | |
12 |
fixed | |
M | |
left |
=
L | |
\int | |
0 |
\left\{-
qdxx2(L-x) | |
L2 |
\right\}=-
qL2 | |
12 |
qdx
For the case with linearly distributed load of maximum intensity
q0
fixed | |
M | |
right |
=
L | |
\int | |
0 |
q0
x | |
L |
dx
x2(L-x) | |
L2 |
=
q0L2 | |
20 |
fixed | |
M | |
left |
=
L | |
\int | |
0 |
\left\{-q0
x | |
L |
dx
x(L-x)2 | |
L2 |
\right\}=-
q0L2 | |
30 |