analysis diving board by macaulay’s methods and strain rosette
TRANSCRIPT
BDA 3033 - Solid Project
Analysis diving board by Macaulay’s methods and Strain rosette
Project Study For
BDA 3033 Solid Mechanics II
By
MAGENTHRAN KUPPUSAMY
Department of Engineering Mechanics
Faculty of Mechanical and Manufacturing Engineering
University Tun Hussein Onn Malaysia Johor
BDA 3033 - Solid Project
Analysis diving board by Macaulay’s methods and Strain rosette
1.1 Introduction of Diving
On a roof slab of a vast burial vault south of Naples is a painting of a young man diving from
a narrow platform. The discovery of the "Tomba Del Tuffatore" (The Tomb of the Diver) shows us
that the excitement and grace of diving from high places into water has lured people from at least 480
BC - the date established for the construction of the tomb. As with most sports dating back to ancient
times, little information on competitive diving has survived. The origins of modern diving can be
traced to two European venues - Halle in Germany and Sweden.
It was a traditional specialty of the guild of salt boilers, called Halloren to practise certa in
swimming and diving skills. The Halloren used to perform a series of diving feats from a bridge into
the River Saale. In 1840 in contact with the German gymnastics movement the world's first diving
association was formed. Most of its members were gymnasts starting their tumbling routines as a
kind of water gymnastic. Thus diving became very popular in Germany.
In Sweden wooden scaffolding was erected around many lakes, inviting courageous fellows
to perform diving feats. Somersaulting from great heights and swallow-like flights of a whole team
are common. The beginning of competitive diving corresponded to the rise of swimming clubs and
associations. In Germany, the oldest club called "Neptun" started international diving contests from a
lower board and from a tower in 1882. In 1891 the first diving rules were adopted and the following
year the first tables were published in Germany.
At the turn of the century, another branch of diving found numerous followers in the USA -
the bridge and artistic leaping. However, its development was stopped due to the high number of
serious accidents. In 1940 in Saint-Louis, with the support of the Germans, diving was added to the
Olympic programme. German divers dominated the springboard scene during the first two decades.
When high diving from a platform was introduced in 1908, the Swedish athletes dominated these
contests.
BDA 3033 - Solid Project
1.2 Introduction of Frontier III - Cantilever Diving Board
Figure 1: Frontier III - Cantilever Diving Board
The Frontier board is timber reinforced and encased in fiberglass for durability and
appearance. A non-slip top ensures maximum safety. There are no unusual climate
restrictions to consider, the boards are designed to be exposed to the elements and live for
years.
Product features
The diving board includes a streamlined and cantilevered stand with spring.
The units are powder-coated Radiant White as Standard color
Made of strong steel, powder coated for increased corrosion resistance.
Stainless Steel Hardware - resists corrosion (the type of material)
Matching, slip-resistant sand tread - for maximum safety
Weight limit: 113 kg (maximum load)
Various Length of diving broad: 1.83m, 2.44m, 3.05m (maximum length)
All diving board and diving stand equipment is supplied with a comprehensive
instruction manual
Installation of all board and stand apparatus can be carried out without special skills
or materials by any home handyman
BDA 3033 - Solid Project
2.0 Problem Statement
A springboard or diving board is used for diving and is a board that is itself a
spring, i.e. a linear flex-spring, of the cantilever type. Springboards are commonly fixed by a
hinge at one end (so they can be flipped up when not in use), and the other end usually hangs
over a swimming pool, with a point midway between the hinge and the end resting on an
adjustable fulcrum.
Diving board is used in Olympic Games or other diving game. This study analyses
which diving board is have more deflection when 113 kg/1108.53 N loads applied. This study
also analyses the principle strain in the plane of rosette and the maximum in plane shearing
strain.
3.0 Objective
The main objective of this project study is to analyze the Frontier III - Cantilever Diving
Board using solid mechanics principles. The solid mechanic method use is stress & strain rosette to
find out the principle strain in the plane of rosette and the maximum in plane shearing strain.
By using Macaulay’s methods the maximum deflection in various length of diving board also
can calculate.
4.0 Scope
The analysis on air plane wing is carried out using the following basic concepts of solid
mechanics only
(i) Deflection of Beam
(ii) Principle strain in the plane of rosette
(iii) Maximum in plane shearing strain
The following assumptions are made in this study with respect to Frontier III - Cantilever
Diving Board
• The board is assumed to be horizontal
• The self weight of board is neglected
• The cross section is assumed as rectangular instead of air foil geometry
• Material is assumed to be Stainless steel with high strength
BDA 3033 - Solid Project
5.0 Analysis of method are use
Deflection of Beams (first method)
The deflection of a spring beam depends on its length, its cross-sectional shape, the
material, where the deflecting force is applied, and how the beam is supported. The equations
given here are for homogenous, linearly elastic materials, and where the rotations of a beam
are small. In the following examples, only loads applying at a single point or single points are
considered - the application point of force F in the diagrams is intended to denote a model
locomotive horn block (or vehicle axle box) able to move vertically in a horn guide, and
acting against the force of the spring beam fixed to or carried by the locomotive or vehicle
mainframes. The proportion of the total weight acting on each axle of a loco or vehicle will
depend on the position of its centre of gravity in relation to the axle (or the chassis fixing
points of equalizing beams where these are used).
5.1 Choosing a deflection value
For reasonable 4mm scale fine scale track, a recommended value for horn block
deflection, δ, under the final load of a locomotive, is 0.5mm.The above recommendation is
known to be an over simplistic and possibly incorrect assumption on what the design value
for the deflection should be, and has given rise to considerable debate. Any experience on
applying this recommendation to real chassis modeling practice is welcomed - the purpose of
this article is a starter for discussion rather than a conclusion of it.
BDA 3033 - Solid Project
5.3 Example: A Cantilever beam is subjected to a bending moment M at the force
end.
2
2
dx
ydEI = Ma…………….(1)
By Integrating of equation 1 (first integration)
dx
dy=
2
2
dx
ydEI
EI dy/dx = Max + C1…………….(2) (slope equation)
At X = 0; dx
dy= 0
Which is C1 = 0
By Integrating of equation 2 (second integration)
y = dx
dyEI = C1 +Max
EI
1
EI y = 2
2Max+ C1x + C2 …………….(2) (max. deflection equation)
Since the value of C1= 0
At X = 0; y = 0
So the maximum deflection equation will be:
y = EI
Max
2
2
……………….(3) (maximum elastic curve equation)
BDA 3033 - Solid Project
Strain gauge and rosette (second method)
The strain gauge has been in use for many years and is the fundamental
sensing element for many types of sensors, including pressure sensors, load cells,
torque sensors, position sensors, etc. The majority of strain gauges are foil types,
available in a wide choice of shapes and sizes to suit a variety of applications. They
consist of a pattern of resistive foil which is mounted on a backing material. They
operate on the principle that as the foil is subjected to stress, the resistance of the foil
changes in a defined way.
The strain gauge is connected into a Wheatstone Bridge circuit with a
combination of four active gauges (full bridge), two gauges (half bridge), or, less
commonly, a single gauge (quarter bridge). In the half and quarter circuits, the bridge
is completed with precision resistors.
BDA 3033 - Solid Project
1. Transformation equation:
1 = x cos2
1 + x sin
2
1 +
xysin
1.cos
1
2 = x cos2
2 + x sin
2
2 + xy sin
2.cos
2
3 = x cos2
3 + x sin2
3 + xy sin1.cos 3
2. Principal strain equation
2,1 = 2
+ yx))
2()
2
-(( 22y xyx
3. Max Shear Strain
2
max = ))2
()2
-(( 22y xyx
4. Principal planes
pTan2yx
xy
BDA 3033 - Solid Project
5.3 Data of Frontier III - Cantilever Diving Board
Figure: Data of Frontier III - Cantilever Diving Board from website:
(http://www.interfab.com/userfiles/2009_U-Stand.pdf)
5.4 specification of Frontier III - Cantilever Diving Board
Table: specification of Frontier III - Cantilever Diving Board in three various lengths
(Website: http://divingboard.net/info/selection_chart.asp)
Raw data which is use in calculation method
BDA 3033 - Solid Project
5.5 Material
Stainless steels resistance to corrosion and staining, low maintenance, relatively low
cost, and familiar luster make it an ideal base material for a host of commercial applicat ions.
There are over 150 grades of stainless steel, of which fifteen are most common. The alloy is
milled into coils, sheets, plates, bars, wire, and tubing to be used in cookware, cutlery,
hardware, surgical instruments, major appliances, industrial equipment, and as an automotive
and aerospace structural alloy and construction material in large buildings. Storage tanks and
tankers used to transport orange juice and other food are often made of stainless steel, due to
its corrosion resistance and antibacterial properties. This also influences its use in commercial
kitchens and food processing plants, as it can be steam-cleaned, sterilized, and does not need
painting or application of other surface finishes. The material is uses for Frontier III -
Cantilever Diving Board are the stainless steel High strength which is Modulus of elastic is
200GPa.
BDA 3033 - Solid Project
Max. Deflection
5.6 Loading
Frontier III - Cantilever Diving Board is used to dive when having swimming
activities. The maximum load can applied is 1108.53 N/ 113 KG. So by using three different
lengths, we can determine the maximum deflection. To determine the maximum deflection,
we are using Macaulay’s method which is just sectioning the last section of beam (Frontier
III - Cantilever Diving Board).
5.7 Case 1: Maximum deflection
5.7.1 Analysis of case:
Case 1: deflection of beam
Figure: before the swimmer stand on the diving plate
Figure: After the swimmer stand on the diving plat
Max. Load =
113 kg/1108.53 N
BDA 3033 - Solid Project
1108.53 N
Ray
M
Rax
0.8 m
0.44 m
L = 1.83m
x = 0 x = L
1108.53 N
X
V M
x = 0
Solution for deflection of beam
When x = L
I = 12
3bd(moment inertia) 0
dx
dy
y = 0
I = 12
)44.0)(8.0( 3
= 5.679 x 10-3 m4
Find out support reaction
Rax = 0
yF = yF
Ray = 1108.53 N / 1.109 KN
Find out slope of beam
0Ma
Ma = (1.109 KN) (1.83m) - M
= 2029.47 Nm + M
M = - 2029.47Nm
• Sectioning method
2
2
dx
ydEI -1108.53 N(X)
2
2
dx
ydEI -1108.53 N(X) ----------- (first Integrating)
BDA 3033 - Solid Project
The Slope equation , Ө
dx
dy = -
EI2
)N(X 1108.53 2
+ C1
When X = L, 0dx
dy..……… (Applying boundary condition)
C1 = EI2
)N(L 1108.53 2
The maximum deflection, y
dx
dy = -
EI2
)N(X 1108.53 2
+ C1…………….. (From slope equation)
y = 1
2
2
)(53.1108C
EI
X
y = - 21
3
6
)(53.1108CXC
EI
X
When X = L, y = 0.
C2 = EI
XL
EI
L
2
)()(53.1108
6
)(53.1108 23
= EI
L
EI
L
2
)(53.1108
6
)(53.1108 33
= EI
L
3
53.1108 3
The specific deflection equation:
y = -EI
X
6
)(53.1108 3
+EI2
)(X)N(L 1108.53 2
EI
L
3
53.1108 3
BDA 3033 - Solid Project
When X = 0, y = Maximum.
y = -EI
X
6
)(53.1108 3
+EI2
)(X)N(L 1108.53 2
EI
L
3
53.1108 3
y = EI
L
3
53.1108 3
By using, I = 5.679 x 10-3 m4 & E = 200 GPa
The Slope
dx
dy =
EI2
)N(X 1108.53 2
When X = 1.83 m
dx
dy =
)10679.5)(200(2
)N(1.83 1108.533
2
xG
dx
dymm00163.0
The maximum deflection, y
y = EI
L
3
53.1108 3
= )10679.5)(200(3
)83.1(53.11083
3
xG
= mm00199.0
BDA 3033 - Solid Project
Case 2: Strain rosette
Solution for Strain rosette
400 = x cos20 + y sin
20 + xy sin0 .cos0 ……….. (1)
200 = x cos245 + y sin
245 + xy sin45 .cos45 ……… (2)
350 = x cos290 + y sin
290 + xy sin90 .cos90 ……… (3)
From equation (1):
400x mm …………..(4)
From equation (2):
xyy )5.0()5.0()5.0)(400(200 ……………… (5)
From equation (3):
350y mm……………(6)
1 = 400 x 10-6 mm
2 = 200 x 10-6 mm
3 = 350 x 10-6 mm
BDA 3033 - Solid Project
From equation 4 & 5, substitute 350ymm & 400x mm to equation 4
xy)5.0()5.0)(350()5.0)(400(200
xy)5.0()1075.1()102(200 44
5.0
375200xy
350xy mm
Principal strain equation
2,1 = 2
350+400))
2
350()
2
350400(( 22
2,1 37522 )175()25(
Ans:
78.5511 mm
22.1982 mm
Max. Shear Strain
2
max = ))2
350()
2
350-400(( 22
2
max 22 )175()25(
2
max78.176
mm
max 55.353mm
BDA 3033 - Solid Project
Principal planes
pTan2
350400
55.353
pTan2 7.071
95.812 p
1
40.97°
2
130.98°
6.0 Results
Methods
Type of calculation Results
Macaulay’s method
Reaction of force, Ray 1.109 KN
Slope of beam 0.00163 mm
Max. deflection of beam 0.00199 mm
Strain rosette
Principal strain
ξ1 = 551.78µ mm
ξ 2 = 198.22 µ mm
Max Shear Strain γmax = 353.55 µ mm
Principal planes 1 40.97°
2 130.98°
BDA 3033 - Solid Project
1.7 Conclusion
The analysis gives out the maximum defection by using Macaulay’s method and the
Principal strain, Max Shear Strain, Principal Planes by using Strain rosette of Frontier III -
Cantilever Diving Board. The specification of Frontier III - Cantilever Diving Board is found
from the trusted website because they are one of the diving board deliver for big game event
such as Olympic Games. So the specification follows the original length and width of
Frontier III - Cantilever Diving Board. This diving board use Stainless steels material with
200G (this is I assume own).
Along I did this solid project; I was able to calculate the deflection of beam (Frontier
III - Cantilever Diving Board) by Macaulay’s method and strain rosette to find the strain in
the beam (Frontier III - Cantilever Diving Board). I also learn how to apply the concept I
learn in class, in the real world or our daily life such as deflection occur in bridge by loads
(cars).
So this project is really worth it if a student applying the concepts are learn in the
class such as buckling of strut, strain energy, Euler theory and many more to apply in our real
life.
BDA 3033 - Solid Project
Referents:
1. Ferdinand P. Beer,E Russell Johnston, John T. DeWolf. "Third Edition:
Mechanics of Materials”
2. http://en.wikipedia.org/wiki/Strain_gauge
3. http://divingboard.net/info/selection_chart.asp
4. http://diving.about.com/od/divingglossary/g/fulcrumDef.ht
5. http://www.interfab.com/userfiles/2009_U-Stand.pdf
6. http://www.aquanet.net/pool-diving-boards- fibredive.htm
7. http://www.poolwarehouse.net/Catalogs/catDivingBoards/fibreDiveDivingBoa
rds.asp