End of Term One Examination (Year 3)

End of Term One Examination (Year 3)

<p>KENYA AERONAUTICAL COLLEGE</p><p>END OF TERM ONE EXAMINATION (YEAR 3)</p><p>MATHEMATICS (3 HOURS)</p><p>ANSWER ALL QUESTION:</p><p>Q1. (a) Evaluate ∫0 2x √5x + 1 dx (8 marks)</p><p>(b) The area bounded by the curve y = x² and the lines x = 4 and y = 0 is rotated about the x – axis through a complete revolution. Determine the x – coordinate of the centroid of the resulting solid of revolution. (12 marks) Q2. (a) If z = x2 - y2 and x = r cos θ and y = r sin θ, find</p><p>(i) ∂z</p><p>∂θ</p><p>(ii) ∂2 z</p><p>∂θ2 (6 marks) (b) Locate the stationary points of the function</p><p>Z = y² + xy + x² + 4y – 4x + 5 and determine their nature. (14 marks)</p><p>Q3. (a) Find the scalar product of the vectors</p><p>A = 3i - 2j + 4k and B = i + 5j – 2k. ~ ~ ~ ~ ~ ~ ~ ~</p><p>Hence determine the angle θ between the vectors. (5 marks) (b) Using De Moivre’s theorem, prove that </p><p>Tan 3 θ = 3t - t³ , where t = tan θ 1 -3t² Hence find the roots of the equation t³ - 3t² - 3t + 1 = 0, correct to three significant figures. (15 marks)</p><p>Q4. Given the equation</p><p>X4 - 8x³ + 17x² + 2x – 24 = 0, show that a better approximation of its root is</p><p>4 Xn+1 = 3Xn - 16Xn³ + 17Xn² + 24 4Xn³ - 24Xn² + 34Xn + 2</p><p>Using the Newton-Raphson iterative method. (8 marks)</p><p>(b) The equation x4 + 5x – 20 has a root approximately at x = 1.8</p><p>Determine the value of the root, correct to five significant figures. (8 marks)</p><p>Q5. The x - component of the acceleration of a particle of unit mass moving in a plane is equal to it’s y-component, and the y – component of the acceleration is equal to thrice it’s x – component. Find the equation of the path given that,</p><p>X = y =0, dx = 2, dy = 4</p><p> dt dt when t = 0 (20 marks) AN ABRIDGED TABLE OF LAPLACE TRANSFORMS</p><p>F(t) LTF (s)</p><p> k K (constant) /s Tn ( n + ve integer)_ n!/sn+1 ent . 1 . s – a Cos at s . S2 + a2 Sin at . a . s2 + a2 Cosh at . s . s2 - a2 Sinh at . a . s2 – a² te-at . 1 . (s + a)2 T cos at s 2 – a 2 (s2+ a2)2 T sin at . 2as . (s2 + a2)2 F’ (t) Sf(S) – f(0) n 2 F (t) S F (s) – SF(o) – F1 (0)</p>

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