lab span deflection - copy
DESCRIPTION
EXPERIMENTTRANSCRIPT
SPAN DEFLECTION (DOUBLE INTEGRATION METHOD)GROUP 3 SECTION 3
1.0 OBJECTIVE
To determine the relationship between span and deflection.
2.0 INTRODUCTION
A beam must possess sufficient stiffness so that excessive deflections do not
have an adverse effect on adjacent structural members. In many cases, maximum
allowable deflections are specified by Code of Practice in terms of the dimensions of
the beam, particularly the span. The actual deflections of a beam must be limited to the
elastic range of the beam, otherwise permanent distortion result. Thus in determining
the deflections of beam under load, elastic theory is used. In this experiment double
integrations method is used to give the complete deflected shape of the beam.
3.0 THEORY
M x-x = EI d²y = P L dx² 2 2
SPAN DEFLECTION (DOUBLE INTEGRATION METHOD)GROUP 3 SECTION 3
v x-x = EI dy = PLx _ Px² + Adx 4 4
y x-x = EIy = PLx² _ Px³ + Ax + B 8 12
When x = 0 ; dy = 0 hence A = 0
When x = L / 2 ; y = 0; hence 0 = PL³ _ PL³ + B32 96
B = - PL³48
When x = 0 ; Y mak = - PL³ ( mid span ; c )48EI
x = L / 2 ; v mak = PL² ( at support )16 EI
Where E can be obtained from the backboard
I = bd³12
b
d
4.0 APPARATUS
SPAN DEFLECTION (DOUBLE INTEGRATION METHOD)GROUP 3 SECTION 3
1. Deflection of Beam and Cantilever Appratus
2. Digital Dail Test Indicator
3. Hanger and Masses
SPAN DEFLECTION (DOUBLE INTEGRATION METHOD)GROUP 3 SECTION 3
4. Specimen Beam
5.0 PROCEDURES
SPAN DEFLECTION (DOUBLE INTEGRATION METHOD)GROUP 3 SECTION 3
1. The moveable knife-edge supports were positioned so that they are
400mm apart. The chosen beam was place on the support.
3. The hanger and the digital dial test indicator placed at mid span. The
digital reading zeroed.
4. An incremental load was apply and the deflection recorded for each
SPAN DEFLECTION (DOUBLE INTEGRATION METHOD)GROUP 3 SECTION 3
increment in the table below.
5. Repeated the above using span of 300mm and 500mm and another beam.
6.0 RESULT
SPAN DEFLECTION (DOUBLE INTEGRATION METHOD)GROUP 3 SECTION 3
Experiment 1: Span = 500mm
No. Mass (N) Deflection
(experimental)
Theoretical Def.
(Ymax)
% Different
1 2.453 - 2.01 - 0.00374 98.14 %
2 2.453 - 0.68 - 0.00072 99.89 %
3 2.453 - 1.49 - 0.0015 99.90 %
Table 1
Experiment 2: Span = 400mm
No. Mass (N) Deflection
(experimental)
Theoretical Def.
(Ymax)
% Different
1 2.453 - 1.02 - 0.00192 99.81 %
2 2.453 - 0.37 - 0.00031 99.92 %
3 2.453 - 0.80 - 0.00077 99.90 %
Table 2
Experiment 3: Span = 300mm
No. Mass (N) Deflection
(experimental)
Theoretical Def.
(Ymax)
% Different
1 2.453 - 0.44 - 0.00082 99.81 %
2 2.453 - 0.16 - 0.00016 99.90 %
3 2.453 - 0.34 - 0.00032 99.91 %
Table 3
7.0 DATA ANALYSIS
SPAN DEFLECTION (DOUBLE INTEGRATION METHOD)GROUP 3 SECTION 3
Experiment 1, number 1;
When x = 0; Y mak = - PL³ (mid span ; c )
48EI
I aluminium = bd³12
b = 19mmd = 2.5mm
I = (19) ( 2.5 ) 3 12
= 24.740 mm4
= 2.474 x 10-11m4
E = 207GNm-2
Ymak = - ( 2.453 )(0.5) 3 48(69G)(2.474 x10-11) = - 0.00374 mm
% different = theo – exp x 100% exp = - 2.01 – (- 0.00374 ) x 100%
- 2.01 = 98.14 %
When x = 0;
SPAN DEFLECTION (DOUBLE INTEGRATION METHOD)GROUP 3 SECTION 3
Y mak = - PL³ (mid span ; c )48EI
I tembaga = bd³12
b = 18mmd = 3mm
I = (1 8 ) ( 3.0 ) 3 12
= 40.50 mm4
= 4.05 x 10-11m4
E = 105GNm-2
Ymak = - ( 2.453 )(0. 5 ) 3 48(105G)(4.05 x10-11) = - 0.0015 mm
% different = theo – exp x 100% exp = - 1.49 – (- 0.0015 ) x 100%
- 1.49 = 99.90 %
When x = 0;
SPAN DEFLECTION (DOUBLE INTEGRATION METHOD)GROUP 3 SECTION 3
Y mak = - PL³ (mid span ; c )48EI
I steel = bd³12
b = 19mmd = 3.0mm
I = (19) ( 3.0 ) 3 12
= 42.75 mm4
= 4.275 x 10-11m4
E = 207GNm-2
Ymak = - ( 2.453 )(0. 5 ) 3 48(207G)(2.474 x10-11) = - 0.00072 mm
% different = theo – exp x 100% exp = - 0.68 – (- 0.00072 ) x 100%
- 0.68 = 99.89 %
8.0 DISCUSSION
SPAN DEFLECTION (DOUBLE INTEGRATION METHOD)GROUP 3 SECTION 3
Comment on the different between the theoretical and experimental result.
The range of percentage of the different between the theoretical and experimental
result was 99.14% to 99.92%. Therefore, there might have some errors occur during
this experiment. The surrounding environment might be effect the reading of the result
of deflection. The errors also can occur when the hanger was hang at a wrong place or
the masses was not accurate.
9.0 EXTRA QUESTIONS
1. Calculate the deflection when x = L / 3 (experiment 1, no 3). Check the result by
placing the digital dial at this position.
y x-x = EIy = PLx² _ Px³ + - PL³ 8 12 48EI
P = 2.453N
x = 0.5/3 = 0.167m
L =0.5m
E = 105GNm-2
I = 40.50 mm4
= 4.050 x 10-11m4
- PL³ = - ( 2.453 )(0.5) 3 48EI 48(105G)(4.05 x10-11) = - 0.0015 mm
y x-x = ( 2.453 x 0.5 x 0.167 2 ) – ( 2.453 x 0.167 3 ) – 0.0015 x 10-3
8 12 = 3.32 x 10-3 m
= 3.32 mm
2. Calculate V max in experiment 2, no. 2.
x = L / 2 ;
SPAN DEFLECTION (DOUBLE INTEGRATION METHOD)GROUP 3 SECTION 3
v mak = -PL² ( at support )16 EI
P = 2.453N
L =0.4m
E = 207GNm-2
I = 42.75 mm4
= 4.275 x 10-11m4
v mak = ( 2.453 )(0.4) 2 16(207G)( 4.275 x 10-11)
= 1.109 x 10-3
10.0 CONCLUSION
Macaulay’s method (the double integration method) is a technique used in
structural analysis to determine the deflection of Euler-Bernoulli beams. Use of
Macaulay’s technique is very convenient for cases of discontinuous and/or discrete
loading. Typically partial uniformly distributed loads (u.d.l.) and uniformly varying
loads (u.v.l.) over the span and a number of concentrated loads are conveniently
handled using this technique.
The first English language description of the method was by Macaulay. The
actual approach appears to have been developed by Clebsh in 1862 Macaulay's method
has been generalized for Euler-Bernoulli beams with axial compression, to
Timoshenko beams, to elastic foundations, and to problems in which the bending and
shear stiffness changes discontinuously in a beam.
From this experiment, we can concluded that we were achieve the objective that
to determine the relationship between span and deflection. We also can conclude that
the deflection will be increase when the mass or forces are increase. Beside that, the
span or the length of the beam will also affect the value of deflection. The shorter beam
SPAN DEFLECTION (DOUBLE INTEGRATION METHOD)GROUP 3 SECTION 3
will have a smaller value of deflection
11.0 REFERENCES
Labsheet Lab Structure Span Defelection (Double Intergration Method)
www.wikipedia.com.my
Mechanics Of Materials Second Edition Universiti Tun Hussein Onn
Malaysia.
CONTENT
SPAN DEFLECTION (DOUBLE INTEGRATION METHOD)GROUP 3 SECTION 3
OBJECTIVE…………………… 1
INTRODUCTION………........... 1
THEORY………………………. 1
APPARATUS………………….. 3
PROCEDURE………………..... 5
RESULT……………………...... 7
DATA ANALYSIS……………... 8
DISCUSSION………………….. 11
EXTRA QUESTION…………... 11
CONCLUSION………………... 12
REFERENCES………………… 13