Final Memo1. To: Professor Goodrich
From: Section 2 Group 9: M. Feigert, T. Tredway, Z. Jones, W. Kudela, M. Sills
Date: 11 December 2014
Subject: Final Memo: Project 2
Introduction
As a team, we were tasked with developing a subassembly for a 12inch by 12inch
platform that would be able to support at least a nominal load of 2 pounds and a maximum
load of 4 pounds while submerged in water. Implied by this stipulation is that the design must
have a factor of safety of no less than 2.00. As another explicit requirement, upon addition of
the maximum load, the subassembly must not sink more than 70% of the change in depth
resulting from the nominal loading case. The project document implicitly requires that the
subassembly promote stability while accounting for uncertainty. Finally, the subassembly
must fit within a predetermined testing area and should be constructed using only specified
building materials.
Design Process/Equations
First and foremost, the subassembly must hold both the nominal and maximum loads.
In order for the platform to float, the buoyant force acting upwards on the platform must be
greater than the force of gravity due to the weight of the platform and any added load. The
buoyant force, the force exerted by a fluid on a body that is submerged in it, is defined as:
V gFb = ρ fluid (1)
where Fb is the buoyant force in Newtons (N), pfluid is the density of the fluid in which the object
is submerged in kilograms per liter (kg/L), V is the volume of the fluid displaced by the object
in liters (L), and g is the acceleration due to gravity in meters per second squared (m/s2
). The
force of gravity due to the weight of the platform and added load is given by:
gF = m (2)
where F is the force in Newtons (N), m is the mass of the object in kilograms (kg), and g is the
acceleration due to gravity in meters per second squared (m/s2
). As previously mentioned, in
order to float, the force component of equation (1) must be no less than the force component
of equation (2). Since the liquid in question for this project is water and acceleration due to
gravity is constant, equations (1) and (2) can be combined and simplified to form:
≥ mV (3)
where V refers to the total volume of floats necessary measured in centimeters cubed (cm3
)
and m is the mass of the object in grams (g). Thus, to support the maximum load of 4 pounds
or 2,789.39 grams, the subassembly must consist of at least 2,789.39 cm3
of floats. Also
important to consider when it came to designing the subassembly was stability. We
developed a design in which all added floats were located around the outside edge of the
platform. In doing this, we created a subassembly whose average center of buoyancy was
2. located in the center of the platform, directly below the intended center of gravity. Finally, we
had to deal with perhaps the most difficult explicit requirement: the 70% stipulation. To do so,
we decided on a twotier design in which the total area of floats in contact with the water
increased as more weight was added. After a period of idea pitching and trialanderror, our
team decided on a design using one cube (of side length 8.2 centimeters) in each corner of
the platform with rectangular prisms (of dimensions 14.08 cm x 8.2 cm x 4.1 cm) connecting
each cube in a picture framelike manner.
Though this initial design did meet all implicit and explicit requirements, we realized
the change in height between our nominal and maximum loading cases, at 66% of the initial
change in height, was uncomfortably close to failing to meet the 70% stipulation. In order to
increase the robustness of the design, we decided to add a small rectangular prism (of
dimensions 8.2 cm x 8.2 cm x 2.0 cm) to each of the four corner cubes as can be seen in the
mechanical drawings at the end of the memo. This slight adjustment vastly decreased our
projected percent change in height to a value of only 45%. Indirectly, the change also
increased the maximum load our subassembly could support, influencing the factor of safety
in a positive way.
Finalized Design and Experimental Results
In designing the subassembly, our goal factor of safety was 4.04. Upon testing the
design to failure though, we found our actual factor of safety to be 16.8% larger at 4.72.
Looking back, we attribute this increased factor of safety primarily to the increased buoyancy
created by an “air bubble” located underneath the platform within the perimeter of rectangular
prisms. Less significantly, we slightly overestimated the mass of the building materials and
platform.
To our team, optimization for cost was important. For this reason, the projected cost
of our initial design was relatively low at only $48.21. The actual cost of designing our
subassembly was much higher at $171.56. We attribute this miscalculation to several
factors. First, while estimating the cost of the supplies, we planned on cutting the wide
packing tape twice lengthwise to accomplish more with the same length of tape. While
actually applying the tape however, we decided not to cut it lengthwise in order to better
waterproof the pieces. Furthermore, after testing the platform, we noticed that it took on a
significant amount of water, so in efforts to rectify this, we applied a second layer of tape in
several locations. Finally, our initial cost calculation assumed we would use plastic wrap as a
waterproofing material instead of simply using packing tape.
As for the displacement of our subassembly in water, our theoretical and experimental
data is captured in Figure 1 located on the following page. As can be seen in the chart, our
theoretical change in height between the unloaded and nominal load conditions was 2.80
centimeters, whereas our theoretical change in height between the nominal and maximum
load conditions was 45% of this value, or 1.25 centimeters. Experimentally, our first change
in height was 2.50 centimeters. Our second change in height was 56% of this value at 1.40
centimeters. There was a 24.4% difference between our experimental and theoretical percent
of change in height.