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Welcome to the page on lecture 14, which I am setting up as an outline of
the material in lecture 14 on March 2, 2000.
The information will help you to focus on what is important.
If you have questions, email me!
- Analysis of statically indeterminate structure
-
A structure is statically indeterminate when the number of unknowns exceeds
the number of equilibrium equations in the analysis. Indeterminancy may
arise as a result of added supports or members.
Although analysis is more involved than statically determinate structures.
There are some major advantages to statically indeterminate structure.
Advantages
- The maximum stresses and deflections in indeterminate structures are
smaller than its statically determinate counterpart.
- Statically determinate structures have a tendency to redistribute its
load to redundant supports in the case of faulty design or overloading
occurs.
- Statically indeterminate structures can support loads with support
loading on thinner members with increased stability. (Cost $ saving)
Disadvantages
- More costly to make an indeterminate structure
- Redundant structures can induce problems such as differential
displacement i.e. A stress created by settlement of a support.
- Method of Analysis of indeterminate structures
-
It is necessary to satisfy equilibrium, compatibility, and force displacement
requirements.
- Equilibrium reaction forces
- Compatibility for multiple supports.
- Force Displacement requirements (two methods).
- Force method with consistant deformation
- Displacement method with consistant force.
We will look at the force method first using virtual work to analysis
structures.
Force Method
- Establish the degree of indeterminacy of the structure.
- Remove sufficient number of unknown forces fro the indeterminate structure
to make the structure determinate and stable. This structure is known as
the primary structure and the extra forces that are removed are known as
redundants.
- Compute the unrestrained deformation of the primary structure at each
redundant location.
- Find the compatibility conditions for solving the structure.
- Solve for the compatibility conditions.
For a single redundant reaction component we can use:
| dD +
VDddd |
= |
0 |
| | |
|
VD |
= |
- dD /
ddd
|
| | &
| |
|
Fi |
= |
F'iprimary + VD *
Fvi
|
where,
| dD | -- |
Displacement in the redundant location |
| ddd | -- |
Displacement in the force applied at the redundant location |
| VD | -- |
Magnitude of the force required to obtain the
compatibility condition. |
| Fi | -- |
Internal force in the member |
| Fvi | -- |
Virtual internal force in the truss |
| F'primaryi | -- |
Internal forces due to the primary loading in the member |
- Example problem of statically indeterminate truss --
External Redundant Support (1)
The truss has an additional support and uses virtual work to find the force
required to meet the compatibility condition, i.e. the deflection at the
redundant force is zero.
- Example problem of statically indeterminate truss --
Internal Redundant Member (1)
The truss is statically determinate however the interior is indeterminate.
If the problem solves it similar to external redundant supports.
- More than one redundant member
The problem requires that you remove the redundant structures. For this
example setup, we will deal with two redundant members. Remove the two
redundant members from the truss and solve for the primary structure. There
will be two compatibility conditions:
|
dB +
VBdbb +
VCdbc
|
= |
0
|
| | |
|
dC +
VBdcb +
VCdcc
|
= |
0
|
where,
| dB | -- |
Displacement at B due to the primary forces |
| dC | -- |
Displacement at C due to the primary forces |
| dbb | -- |
Displacement at B due to the force applied at B |
| dbc | -- |
Displacement at B due to the force applied at C |
| dcb | -- |
Displacement at C due to the force applied at B |
| dcc | -- |
Displacement at C due to the force applied at C |
| VB | -- |
Magnitude of the force applied at B |
| VC | -- |
Magnitude of the force applied at C |
We can substitute for the d terms in summations
and two compatibility conditions.
|
S F'i Fvbi
Li / Ai Ei
| + |
VB S Fvbi
Fvbi Li / Ai Ei
| + |
VC S Fvbi
Fvci Li / Ai Ei
|
= |
0
|
| | |
|
S F'i Fvci
Li / Ai Ei
| + |
VB S Fvci
Fvbi Li / Ai Ei
| + |
VC S Fvci
Fvci Li / Ai Ei
|
= |
0
|
This can be written in a matrix vector type format. So it resembles:
|
Fvb |
Fcb |
| | |
| | | | |
|
| Fvb |
A11
|
A12
|
VB | |
- S F'i Fvbi
Li / Ai Ei
|
| | | | = |
|
| Fcb |
A21
|
A22
|
VC | |
- S F'i Fvci
Li / Ai Ei
|
| A11 | = |
S Fvbi
Fvbi Li / Ai Ei
|
| | |
| A12 | = |
S Fvbi
Fvci Li / Ai Ei
|
| | |
| A21 | = |
S Fvci
Fvbi Li / Ai Ei
|
| | |
| A22 | = |
S Fvci
Fvci Li / Ai Ei
|
|
|