Stability & Determinance
Three Important Relationships
The following three relationships are used to solve different types of structural mechanics problems.
| Relationship | Description |
|---|---|
| Equilibrium つり合い |
Relationship between forces and stresses Based on Newton's laws of motion: the sum of all forces acting on a structure at rest is zero. |
| Constitutive Relationships 構成則 |
Relationship between stress and strain Based on the element's material properties and how it reacts to forces. A key example is Hooke's law, which describes linear-elastic material behavior. |
| Compatibility 適合 |
Relationship between strain and displacement Describes geometry of deformation such that there is no rupture or overlapping of the material. |
Force → (Equilibrium) → Stress → (Constitutive) → Strain → (Continuity) → Displacement
On the First Class Architect exam, you will need to be able to use the equations of equilibrium. You will also need to understand how to leverage compatibility and constitutive relationships, although you won't necessarily need to use formal equations, etc.
Constitutive Relationships
As mentioned above, the typical example of a constitutive relationship is Hooke's law: \(F=kx\). This is used to describe spring stiffness and is commonly used, e.g. axial stiffness: \(k=\frac{AE}{L}\). Another form of this same law is well known to engineers and describes the elastic stress-strain relationships: \(\sigma=E\epsilon\) or \(\gamma=G\tau\).
Continuity
You don't need to set up continuum equations, but you do need to identify basic contintuity conditions, i.e., displacement or slope continuity. Example:
Positive Convention
It's important to use a consistent convention for positive forces and moments. The tricky part is that these mean different things, depending on whether you're looking at externally applied forces or internal stresses.
External Forces
For external forces, typically forces acting upwards and rightwards are positive. The US uses the right-hand-rule (RHR), which dictates that positive moments spin counter-clockwise (CCW). In Japan, it's common to defined positive applied moments as spinning clockwise (CW), which is the opposite of the RHR.
Internal Forces
Both countries use the same convention for internal forces:
Equilibrium
Structures in equilibrium satisfy the following three expressions, regardless of the point of reference.
| $$\sum F_X=0$$ | $$\sum F_Y=0$$ | $$\sum M=0$$ |
NOTE: Setting up the equations of equilibrium is a critical step in solving many structural analysis and free-body diagram problems.
Supports and Joints
External Supports
There are four main types of boundary conditions, illustrated in the table below. Typically, the reactions at supports are thought of in terms of a global frame of reference: Fx, Fy and M.
| Free | Roller | Pin | Fixed |
|---|---|---|---|
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| No reactions | 1 reaction | 2 reactions | 3 reactions |
Internal Joints
There are several types of internal joints, which are different releases (degrees of freedom) for forces and moments acting within the structure.
| Rigid | Pin | Axial Slider | Shear Slider |
|---|---|---|---|
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| No releases | Moment release | Axial release | Shear release |
Stability of Structures
| Unstable 不安定 |
Stable 安定 |
|
|---|---|---|
| Determinant 静定 |
Indeterminant 不静定 |
|
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| Unstable structures that do not satisfy equilibrium equations. | Stable structures that can be solved with only equilibrium equations. | Stable structures that require compatibility or constitutive equations in addition to equalibrium equations. |
There are several methods for rapidly assessing whether a simple 2D structure is unstable, determinant or indeterminant.
Japanese Method
The following equation is the commonly used in Japan, although it generates the same results as the alternative below.
| \(m<0\) (Unstable) | $$m=n+s+r-2k$$ |
| \(m=0\) (Determinant) | |
| \(m>0\) (Indeterminant) |
The defintion of each of these variables are as follows:
Example Frame
NOTE: the number of support reactions (n) is the sum of reactions at each individual support, based on the boudnary conditions. Refer to External Supports above.
Counting Nodes (k)
The illustration belows shows the example frame with all the nodes numbered. Nodes are the supports, joints and free-ends of members. Think of them as the dots you'd first have to draw, then connect with lines, to illustrate the structure.
Counting Members Segments (s)
In this method, rather than counting physical members, you must count the number of segments between the nodes. This is why it's helpful to count the nodes first. For example, the three members a-b, c-d-e and f-g are single physical elements in reality, but count as seven segments in this example.
Counting rigid connections (r)
The figure shows a joint with four members (s=4) framing into it. In this case, one of the members is pinned at the joint, the others are rigidly connected. In this case r = 2 because the the maximum number of rigid joints at a node is the number of members framing into it minus 1. Another way to think of it: \(r_{joint}=s_{joint}-pins_{joint}-1\).
The same four-way connection with no pins would have r = 3.
Example Conclusion
Totalling up each of these components gives us the value m:
$$m=n+s+r-2k=6+10+7-2(10)=3$$
Since m > 0, it's clear the structure is indeterminant. In this case it's indeterminant to the third degree, which means we'll need to use equations of compatibility and/or the constitutive relationships in addition to equilibrium to analyze this structure.
For the purposes of the First Class Architecture exam, you'll only need to rapidly assess whether a frame is unstable, determinant or indeterminant. The degree and force analysis are generally not required.
Alternative Method
In North America and Europe, the following method is used. It is very similar, but groups the equalibrium equations slightly differently.
| \(d<0\) (Unstable) | $$d=3m+r-3j-c$$ |
| \(d=0\) (Determinant) | |
| \(d>0\) (Indeterminant) |
The defintion of each of these variables are as follows:
In this case the coefficient of 3 on members and joints comes from the fact that equalibrium satisifies three equations for each member and joint.
Which ever method is easier to remember is completely fine. They both yield the same results everytime.
Example Conclusion
Extending the example from above and summing for d:
$$d=3m+r-3j-c=3(10)+6-3(10)-3=3$$
This demonstrates that the two approaches yeild the same results.
NOTE: Several quantities in both methods are the same, but with different coefficient letters: m (US) = s (Japan), r (US) = n (Japan), j (US) = k (Japan). The key difference is the US method totals internal hinge quantity (c), while the Japanese approach totals the internal rigid joints (r).