



It is interesting to note that the house is built directly onto the rock cliff. For this reason we assume the rock in the cliff, and thus in the house, to be igneous. That is, a very strong type of rock.
We assumed the spacing of the beams in the living room to be about six feet on center. The roof framing throughout the rest of the house is typical residential wood framing, sixteen or twenty-four inches on center. The walls of the house are solid stone , varying in thickness of two to three feet.
The roof framing system differs internally between the exposed, load bearing beams of the living room and the typical residential framing found in the rest of the house where the ceilings are plastered. Starting with the living room, the exposed beams re st only on the walls. There is no ridge beam to support the beams on their upper ends. This transfers some lateral load to the walls as well as vertical loads. We assume this by looking at the floor plan of the living room. It shows no indication of a ridge beam, but does show the presence of other beams. This is further confirmed by examination of the longitudinal axis of the room where we find a large window at one end and a relatively small portion of wall at the other. One would expect more thic kness in the wall at these points, if it were bearing the load of the roof. Looking at the wall where we know, without a doubt, that the beams are bearing, we see a definite thickening of the wall directly under the ends of the beams. The more typical f raming of the rest of the house sits on the walls with very little lateral load created by its presence. A load on the roof over this part of the house would transfer down along the rafters to the wall. There, its lateral loads would be resolved by the collar ties, or ceiling joists, which connect to the roof rafters at their bottom ends creating a triangular shape to a roof framing bay. Returning to the load, we see it now pass into the walls where it is taken down to the footings. The footings then pass the load into the ground where it is dissipated.
Lateral Load
The lateral loads that the building whithstands are winds from the ocean, the lateral component of the loading from the beams in the living room, and occasionally, earthquakes. We believe that the design force of the wind for the California coast is 80 m
ph. The highest lateral load that any portion of the stone wall would receive is the force of the wind straight on, or perpendicular to the direction of the wind. The two foot thick wall at eight feet high is still thick enough, we believe, to easily wi
thstand this force, simply because of its mass. The other constant lateral load comes from the living room rafters. In both cases, the resultant force vectors would follow lines similar to those that one finds when examining Gothic cathedrals. That is,
the lateral force the wall receives, is not great enough to overcome the vertical force of its own dead weight, along with that of the roof. Thus, the resultant force vector gets directed downward at a sharp enough angle to pass out the middle third of
the wall at its base. This is assuming that calculating the loads will prove this out. We guess it will be a good candidate for mathematical examination on the next portion of the case study.
Gordon Hicks and Yi-Hsiu Yeh
ARCH 461/561 Spring 1995
Do you have questions about adding a case? or a building to suggest??????? send a message to me....... chrisl@aaa.uoregon.edu