Exam Details

Subject finite element method
Paper
Exam / Course m.tech
Department
Organization Institute Of Aeronautical Engineering
Position
Exam Date November, 2018
City, State telangana, hyderabad


Question Paper

Hall Ticket No Question Paper Code: AAE009
INSTITUTE OF AERONAUTICAL ENGINEERING
(Autonomous)
Four Year B.Tech V Semester End Examinations (Regular) November, 2018
Regulation: IARE R16
FINITE ELEMENT METHODS
Time: 3 Hours Max Marks: 70
Answer ONE Question from each Unit
All Questions Carry Equal Marks
All parts of the question must be answered in one place only
UNIT I
1. Discuss the finite element methodology to solve the structural problems.
Consider a bar as shown in Figure 1. An axial load of 200 kN is applied at a point p. Take
A1 2400 mm2, E1 70 x 109 A2 600 mm2, E2 200 x 109 N/m2. Calculate the
following: Nodal displacement at point P Stresses in each material.
Figure 1
2. Derive the stiffness matrix for Quadratic shape functions
A two-step bar subjected to loading condition as shown in Figure 2 is fixed at one end and the
free end is at a distance of 3.5mm from the support. Determine stresses in the element. Take
E=200X109 N/mm2.
Figure 2
UNIT II
3. Derive the transformation Matrix for a plane truss element.
For the truss in Figure 3 . a horizontal load of P 4000 lb is applied in the x direction at node
2.Write down the element stiffness matrix
Page 1 of 4
Figure 3
4. Derive shape function and stiffness matrix for 2D truss element.
For the cantilever beam subjected to the uniform load w as shown in Figure determine the vertical
displacement and rotation at the free end. Assume the beam to have constant EI throughout
its length.
Figure 4
UNIT III
5. Derive the stiffness matrix for beam element using potential energy approach.
For a thin plate subjected to in-plane loading a shown in Figure 5 determine the Global Stiffness
matrix. The plate thickness t=1cm, E 20 X 106 N/cm2 and moment of inertia I=2500cm4.
Consider it as a two elemental beam problem.
Figure 5
Page 2 of 4
6. For the triangular element shown in Figure 6. Obtain the strain-displacement relationship matrix
and determine the strains "y and
xy:
Figure 6
The nodal coordinates for an axisymmetric triangular element are given Table 1. Evaluate
matrix for that element.
Table 1
r1 10 mm z1 10 mm
r2 30 mm z2 10 mm
r3 30 mm z3 40 mm
UNIT IV
7. Derive the shape function and stiffness matrix for 1D heat conduction element.
Compute element matrices and vectors for the element shown in Figure when the edge kj
experiences convection heat loss.
Figure 7
8. Calculate the temperature distribution in a one dimension fin with physical properties given in
Figure 8. The fin is rectangular in shape and is 120 mm long. 40 mm wide and 10 mm thick.
Assume that convection heat loss occurs from the end of the fin. Use two elements. Take k
0.3 W/mmoC; h 1 x T1 20oC. Assume unit area.
Figure 8
Page 3 of 4
Find the temperature distribution in a square region with uniform heat generation as shown in
Figure 9. Assume that there is no temperature variation in the z-direction. Take 30W/cm0c,
h=10 watts/cm20k, l 10cm, T1 50oC, 100 W/cm3. Consider it a two elemental problem.

Figure 9
UNIT V
9. Consider a uniform cross-section bar as shown in Figure 10 of length L made up of material
whose Young's modulus and density is given by E and Estimate the natural frequencies of
axial vibration of the bar using lumped mass matrix. Consider the bar as one element.
For the one dimensional bar shown in Figure 10, determine natural frequencies of longitudinal
vibration using two elements of equal length. Take E 2 x 105 N/mm2, 0.8 x N/mm3,
and 400 mm.
Figure 10
10. Determine the natural frequencies of transverse vibration for a beam fixed at both ends. The
beam may be modeled by two elements, each of length density modulus of elasticity cross
sectional area A and moment of inertia I. Consider lumped mass approach.
Consider the simply supported beam shown in Figure 11. Let the length L 1 E 2 x 1011
area of cross section A 30 cm2, moment of inertia I 100 mm4, density 7800
kg/m3. Determine the natural frequency using lumped mass matrix approach.


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