UNIVERSITI TUN HUSSEIN ONN MALAYSIA FINAL EXAMINATION SEMESTER I SESSION 2011/2012
COURSE NAME COURSE CODE PROGRAMME : : : ENGINEERING MATHEMATICS IV BWM 30603/BSM 3913 1 BEE 2 BDD/BEE/BFF 3 BDD/BEE/BFF 4 BDD/ BFF JANUARY 2012 3 HOURS ANSWER ALL QUESTIONS IN PART A AND TWO (2) QUESTIONS IN PART B. ALL CALCULATIONS AND ANSWERS MUST BE IN THREE (3) DECIMAL PLACES.
EXAMINATION DATE : DURATION INSTRUCTION : :
THIS EXAMINATION PAPER CONSISTS OF SEVEN (7) PAGES
CONFIDENTIAL
BWM 30603 /BSM 3913
PART A Q1 (a) Consider the heat conduction equation
2 T ( x, t ) 2 T ( x, t ), t x
0 x 10, t 0 ,
where is thermal diffusity 10, since c 2 . Given the boundary conditions,
T (0, t ) 0, T (10, t ) 100
and initial condition,
T ( x,0) x 2 .
By using explicit finite-difference method, find T ( x,0.055) and T ( x,0.11) with 5 grid intervals on the x coordinate. (10 marks) (b) Let y( x, t ) denotes displacement of a vibrating string. If T is the tension in the string, is the weight per unit length, and g is acceleration due to gravity, then y satisfies the equation
2 y Tg 2 y , 0 x 2, t 0. t 2 x 2
Suppose a particular string is 2 m long and is fixed at both ends. By taking T 1.5 N, 0.01 kg/m and g 10 m/s2, use the finite-difference method to solve for y up to level 2 only. The initial conditions are
x 0 x 1 2, y ( x , 0) 2 x , 1 x 2 2
and
y ( x , 0) x( x 2). t
Performed all calculations with x 0.5 m and t 0.01 s. (15 marks)
Q2
The steady state temperature distribution of heated rod follows the one-dimensional form of Poisson’s equation d 2T Q( x) 0 . dx 2 Solve the above equation for a 6 cm rod with boundary conditions of T (0, t ) 10 and T (6, t ) 50 and a uniform heat source Q( x) 40 with 3 equal-size elements of length by using finite-element method with linear approximation. (25 marks) 2
BWM 30603 /BSM 3913
PART B Q3 (a) Given f x 7e x sin x