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Experimental Verification of Principle of Superposition For An Indeterminate Structure

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AE451A

Experimental Verification of Principle of Superposition


for an Indeterminate Structure

Prepared by: Rupinder Singh (160593)


Group: S9
OBJECTIVES:

(i) To compare the experimentally obtained beam deflection values


from dial gauge with theoretical values calculated from principle of
superposition for a given indeterminate beam which is transversely
loaded at two points.

(ii) To verify the principle of superposition by the strain values


obtained from strain gauges mounted on indeterminate beam which
is transversely loaded at two points.

INTRODUCTION:

(i)Definitions

• Indeterminacy: The aim of structural analysis is to evaluate the


external reactions, the deformed shape and internal stresses in the
structure. If this can be accomplished by equations of equilibrium,
then such structures are known as determinate structures. If no. of
unknown reactions were more than no. of equilibrium equation, then
it is known as Indeterminacy.

• Redundancy: Redundancy means the structure's forces and stresses


cannot be determined by just the basic equilibrium equations. A truss
having more than (2j – 3) members is statically indeterminate or
redundant, the degree of indeterminacy or redundancy being equal
to the number of extra members.

• Basics of principle of superposition and its validity: The Principle


of Superposition Theorem states that in any linear network
containing two or more sources, the response in any element is equal
to the algebraic sum of the responses caused by individual sources
acting alone, while the other sources are non-operative.
EXPERIMENTAL SETUP:

FIGURE 1:
Free Body Diagram of beam-

CALCULATIONS:
E (Aluminium) = 69GPa

Moment of Inertia (I) = (1/12) bh3 = (1/12)*25*(12)3 = 36*10-10 m4

In similar for the other two cases:


Now for deformation at each point:--

TABLE 1: Deflection Reading on Dial Gauge.

Gauge Position Zero Load Reading (mm) P1= 5N P1= 5N P1= 0N


no. (mm) P2 = 0N P2 = 5N P2 = 5N

Initial Final Avg. Actual Raw Actual Raw Actual Raw Actual
Data Data Data Data Data Data
(mm) (mm) (mm) (mm) (mm) (mm)

1 45 0 0 0 0.00 -0.01 -0.01 -0.01 -0.01 -0.01 -0.01

2 225 0 0 0 0.00 -0.05 -0.05 -0.12 -0.12 -0.06 -0.06

3 360 0 -0.01 -0.005 0.00 -0.07 -0.065 -0.19 -0.185 -0.11 -0.105

4 495 -0.01 0 -0.005 0.00 -0.07 -0.065 -0.21 -0.205 -0.13 -0.125

5 685 -0.01 0 -0.005 0.00 -0.04 -0.035 -0.11 -0.105 -0.08 -0.075
TABLE 2: Dial Gauge Deflection value for the four loading cases and their
Theoretical deflection.

Theoretical Deflection vs Dial Gauge Deflection

P1 = 0 N P1= 5N P1= 5N P1= 0N


Gauge Position P2 = 0N P2 = 0N P2 = 5N P2 = 5N
no. (mm)
Theory Dial Theory Dial Theory Dial Theory Dial
Gauge Gauge Gauge Gauge

1 45 0.00 0.00 -0.00052 -0.01 -0.00097 -0.01 -0.00043 -0.01

2 225 0.00 0.00 -0.00816 -0.05 -0.01612 -0.12 -0.00795 -0.06

3 360 0.00 0.00 -0.01205 -0.065 -0.02714 -0.185 -0.01510 -0.105

4 495 0.00 0.00 -0.01144 -0.065 -0.03004 -0.205 -0.01861 -0.125

5 685 0.00 0.00 -0.00550 -0.035 -0.01622 -0.105 -0.01074 -0.075

FIGURE 2:

Deflection vs position
0
0 100 200 300 400 500 600 700 800
-0.05
Deflection (mm)

-0.1
Theory
-0.15 Dial Gauge

-0.2

-0.25
Position (mm)
TABLE 3: Data records for the strain gauges in all 4 loading conditions. And
strain values obtained from the principle of superposition.

Strain Distance Loading Condition and corresponding strain values(in 10-6) Error (in %)
Gauge (in cm)
Number
P1 = 0 N P1 = 5 N P1 = 0 N P1 = 5 N P1 = 5 N
P2 = 0N P2 = 0 N P2 = 5 N P2 = 5 N P2 = 5 N
(P1+ P2) Exp.

3 76 -1.9445 -2.9504 -6.3943 -9.3447 -8.6787 7.6739

4 70 -1.9250 -4.0208 -10.5656 -14.5864 -14.2646 2.2559

5 64 -1.6379 -5.1371 -14.6713 -19.8084 -19.5865 1.1329

6 58 -1.5356 -6.1297 -19.0981 -25.2278 -25.2559 0.1112

7 52 -1.6388 -7.2719 -22.0456 -29.3175 -29.5757 0.8730

8 46 -1.6418 -9.1819 -17.6623 -26.8442 -26.9582 0.4310

9 40 -1.5673 -10.8647 -13.6829 -24.5476 -25.1760 2.4960

10 34 -1.9824 -13.0532 -10.0146 -23.0678 -23.2595 0.8241

11 28 -1.7013 -14.6048 -5.2305 -19.8353 -19.6705 0.8378

12 22 -2.1416 -8.8017 -1.5248 -10.3265 -9.5581 0.0803

13 16 -1.9276 -2.0421 3.0094 0.9673 1.5993 39.5172

14 10 -2.1252 4.2464 6.7036 10.9502 12.2331 10.4887

15 4 -2.1110 10.5594 22.5478


10.4874 21.0468 6.6592
FIGURE 3:

SOURCES OF ERROR:

1. Error can come while taking the reading from the dial gauges.
2. Effect of air can disturb the values as well.
3. Temperature conditions can alter the results as well.
4. There could be a permanent deflection in beam after a long use

Conclusion:

• The dial gauges provided a fair idea of the distribution of deflection


throughout the beam, but the readings of the deflections were
inaccurate with respect to the theoretical data.

• Principle of Superposition can be applied to analyse with


indeterminate structure with fair accuracy. But it is observed that the
error is higher towards the ends of the beam and accurate with
(|error|<5%) towards the centre of the beam.

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