StrEng007
Structural
- Aug 22, 2014
- 543
I know there are many threads regarding this question... but I can't seem to pin down a final answer on this one.
While tracing out the load path for MWFRS wind, into a diaphragm then lateral system, the question about how these loads make their way to supporting shear walls came up.
My general question here is how loads travel through a diaphragm that is not flat. There are (7) questions numbered below.
Let's start with the windward and leeward walls of a typical rectangular structure with a flat roof.
The half wall height will lend itself two (2) loads, one positive (towards) the diaphragm and one negative (away from) the diaphragm. The generic textbook method sums these two loads as a linear load and applies it directly to the diaphragm of a flat roof. No issues there so far. Since the diaphragm's plane is at a 0° angle, I see this load being transferred through the diaphragm, where the w(diaphragm) = (WW Pressure)x(1/2 wall height) + (LW pressure) x (1/2 wall height). [I'm not making reference to any internal pressure coefficients to keep this as straightforward as possible].
Example
(WW Pressure)x(1/2 wall height) = 300 lb/ft
(LW pressure) x (1/2 wall height) = 300 lb/ft
w(diaphragm) = 600 lb/ft
Now let's suppose the roof was not flat, but instead a gable with a 4:12 roof pitch (18.4°). Plywood sheathing is used on the top of the roof trusses and I'm assuming no ceiling diaphragm action below the truss bottom chords. Load is intended to travel through the roof sheathing, into a lateral resisting system (i.e. drag truss to shear wall, etc.).
Here is where most textbooks don't go into detail. Since the roof is no longer flat, I don't see how the w(diaphragm) can be determined as previously calculated. Now the loads on the system are travelling through a plane that is inclined and will have (2) force components associated with it (x-horizontal and y-vertical). The actual projection of the diaphragm will be the resultant... Therefore, in order to resist the overall x-horizontal movement of both walls, the linear diaphragm load through the windward portion of the roof diaphragm is:
w'(WW)= [600lb/ft]/[2cos18.4°]
and the leeward wall,
w'(LW)= [600lb/ft]/[2cos18.4°]
Here, the overall roof is split into separate planes to illustrate the resultant analogy. In reality, these should act as one combined unit with proper blocking etc... That is a whole separate topic of its own.
Over a wall length of 20 ft (the structure is 20 ft long parallel to the ridge, with a lateral system at each end) the diaphragm will have the resulting loads:
x-component= (20ft/2)x (2[600lb/ft]/[2cos18.4°])x(cos18.4)= 6000lb
Notice how this is equal to = (600lb/ft)x(20ft/2)= 6000lb
So far so good. By comparison, the values for the x-horizontal force are the same for both flat roof and gable roofs.
HOWEVER:
There will be a y-component from the WW panel=(20ft/2)x(1[600lb/ft]/[2cos18.4°])x(sin18.4)=+1000 lb
and the LW panel = (20ft/2)x(1[-600lb/ft]/[2cos18.4°])x(sin18.4)=-1000 lb
1.Where does this get distributed along the length of the roof? For a drag truss, these loads would be added as a couple at the ends of the truss down into the vertical portion of the lateral resisting system. What is done here?
2. Is this vertical component of the force making it's way into each supporting truss as a vertical reaction?
3. If that is the case, then is every truss by nature a drag truss of sorts? Since the horizontal reaction at the truss is inadvertently being dragged through the chords to resolve the forces.
4. Is this component of the force just ignored?
Now, for the next component of loading... the wind normal to the roof's surface. The normal load on each side of the truss can be split into a horizontal and vertical force. For a POSITIVE Windward and NEGATIVE Leeward scenario, the roof will see the following (wind load perpendicular to ridge).
Windward roof:
Horizontal wind from west to east
Vertical wind pushing down
Leeward roof:
Horizontal wind from west to east
Vertical uplift reaction
Here, I would take the vertical reactions out in the vertical system of the structure. However, there is still a horizontal component that wants to move the roof truss from west to east.
5. Is this horizontal load to be added to the horizontal reactions from the windward and leeward walls, calculated with the same procedure above?
6. Will the roof have uplift from wind normal to the surface IN ADDITION TO an uplift component from the portion of the load (question 5) added to the procedure I described above.
7. Why is this not discussed more?
While tracing out the load path for MWFRS wind, into a diaphragm then lateral system, the question about how these loads make their way to supporting shear walls came up.
My general question here is how loads travel through a diaphragm that is not flat. There are (7) questions numbered below.
Let's start with the windward and leeward walls of a typical rectangular structure with a flat roof.
The half wall height will lend itself two (2) loads, one positive (towards) the diaphragm and one negative (away from) the diaphragm. The generic textbook method sums these two loads as a linear load and applies it directly to the diaphragm of a flat roof. No issues there so far. Since the diaphragm's plane is at a 0° angle, I see this load being transferred through the diaphragm, where the w(diaphragm) = (WW Pressure)x(1/2 wall height) + (LW pressure) x (1/2 wall height). [I'm not making reference to any internal pressure coefficients to keep this as straightforward as possible].
Example
(WW Pressure)x(1/2 wall height) = 300 lb/ft
(LW pressure) x (1/2 wall height) = 300 lb/ft
w(diaphragm) = 600 lb/ft
Now let's suppose the roof was not flat, but instead a gable with a 4:12 roof pitch (18.4°). Plywood sheathing is used on the top of the roof trusses and I'm assuming no ceiling diaphragm action below the truss bottom chords. Load is intended to travel through the roof sheathing, into a lateral resisting system (i.e. drag truss to shear wall, etc.).
Here is where most textbooks don't go into detail. Since the roof is no longer flat, I don't see how the w(diaphragm) can be determined as previously calculated. Now the loads on the system are travelling through a plane that is inclined and will have (2) force components associated with it (x-horizontal and y-vertical). The actual projection of the diaphragm will be the resultant... Therefore, in order to resist the overall x-horizontal movement of both walls, the linear diaphragm load through the windward portion of the roof diaphragm is:
w'(WW)= [600lb/ft]/[2cos18.4°]
and the leeward wall,
w'(LW)= [600lb/ft]/[2cos18.4°]
Here, the overall roof is split into separate planes to illustrate the resultant analogy. In reality, these should act as one combined unit with proper blocking etc... That is a whole separate topic of its own.
Over a wall length of 20 ft (the structure is 20 ft long parallel to the ridge, with a lateral system at each end) the diaphragm will have the resulting loads:
x-component= (20ft/2)x (2[600lb/ft]/[2cos18.4°])x(cos18.4)= 6000lb
Notice how this is equal to = (600lb/ft)x(20ft/2)= 6000lb
So far so good. By comparison, the values for the x-horizontal force are the same for both flat roof and gable roofs.
HOWEVER:
There will be a y-component from the WW panel=(20ft/2)x(1[600lb/ft]/[2cos18.4°])x(sin18.4)=+1000 lb
and the LW panel = (20ft/2)x(1[-600lb/ft]/[2cos18.4°])x(sin18.4)=-1000 lb
1.Where does this get distributed along the length of the roof? For a drag truss, these loads would be added as a couple at the ends of the truss down into the vertical portion of the lateral resisting system. What is done here?
2. Is this vertical component of the force making it's way into each supporting truss as a vertical reaction?
3. If that is the case, then is every truss by nature a drag truss of sorts? Since the horizontal reaction at the truss is inadvertently being dragged through the chords to resolve the forces.
4. Is this component of the force just ignored?
Now, for the next component of loading... the wind normal to the roof's surface. The normal load on each side of the truss can be split into a horizontal and vertical force. For a POSITIVE Windward and NEGATIVE Leeward scenario, the roof will see the following (wind load perpendicular to ridge).
Windward roof:
Horizontal wind from west to east
Vertical wind pushing down
Leeward roof:
Horizontal wind from west to east
Vertical uplift reaction
Here, I would take the vertical reactions out in the vertical system of the structure. However, there is still a horizontal component that wants to move the roof truss from west to east.
5. Is this horizontal load to be added to the horizontal reactions from the windward and leeward walls, calculated with the same procedure above?
6. Will the roof have uplift from wind normal to the surface IN ADDITION TO an uplift component from the portion of the load (question 5) added to the procedure I described above.
7. Why is this not discussed more?