Detailed Solutions        Mathematics - II         D-23/DC-23       December 2004


 

Q1(a)

z1 = r1 (Cos q1 + i Sin q1)

z2 = r2 (Cos q2 + i Sin q2)

z1 z2 = r1 r2 (Cos q1 + i Sin q1) (Cos q2 + i Sin q2)

= r1 r2 [(Cos q1 Cos q2 - Sin q1 Sin q2) + i (Cos q1 Sin q2 +Cos q2 Sin q1)]

= r1 r2 [Cos (q1 +q2 ) + i Sin (q1 +q2)]                                                           Ans. B

 

Q1(b)   If w is cube root of unity then we know that 1+w+w2=0                            Ans. A

 

Q1(c)   Given  x2-x-12=0  Þ (x-4) (x+3) = 0   Þ x=4,-3                                         Ans. C

 

Q1(d)  Given

   Þ                                  Ans. A

 

Q1(e) Given

A-1A = I,  B-1B = I

Now (AB) (B-1 A-1)  = AIA-1 = AA-1 = I --......................---------------(1)

Also (B-1 A-1) (AB) = B-1 (A-1A) B  = B-1 IB = B-1 B=I-----------------(2)

from 1 and 2, we get    (AB)-1 = B-1 A-1                                                         Ans. C

 

Q1(f)    Given   A ( 3,4,5) and   B (6,8,9)

                              Ans. A

 

 

Q1(g)   We know that the function ¦(x) = Sin x is periodic and period is 2p            Ans. C

 

Q1(h)   By definition

=

                                           Ans. B

 

Q2(a)  

 

Also |z|2 =  ----------(2)

 

From (1) and (2),

 

Q2(b)   ,  

 and

 = 9+16 = 25

from (1) and (3) x2=4, y2=1

from (2) xy is positive so if x=2, y=1 and x=-2, y=-1

Hence

 

Q3(a)   Given z=Cos q +i Sin qÞ zn = Cos n q + i Sin n q,
z-n =Cosnq-iSinnqTherefore zn+z-n= 2 Cos n q.

 

Q3(b)  Given

.................

Now

        = Cos p + i Sin p = -1

 

Q4(a)   Since A is invertible matrix, therefore |A| ¹0 Þ|AT|¹0

Þ AT is also invertible

Now AA-1 = I = A-1Þ (AA-1)T = I = (A-1A)T  Þ (A-1)T AT= I = AT(A-1)T

Þ (AT)-1 = (A-1)T

 

Q4(b)

  and

      ,

,

 ,

 , ,

 

 

Q.5(a)   = 0, Since

 

Q5(b) 

C2 à C2+C3

= (x+y+z) 0         [C1 and C2 are identical]

 

= 0

 

Q6(a)   Let the position vectors of points A and B are  and  respectively. Let P be the point which divides the line joining A and B in the ratio m:n and let be the position vector of P. Then  where O is origin

 
Given

Now ,

From (i) we get

 

Q6(b)   ,

Þ sides represented by   are at right angles

Also

\vectors  form the sides of right angled triangle

 

Q7(a)   Cayley Hamilton Theorem

Every square matrix satisfies its own characteristic equation

Characteristic matrix is

Characteristic equation is

|A-lI| = 0  Þl3-7l2+11l-5 = 0 . By Cayley Hamilton theorem

 

A3-7A2+11A-5I = 0

 

Now

 =

 

A3-7A2+11A-5I

 

            +

 

 

Q7(b)   System of equations is 2x - 3y + z = 0, x +2y – 3z = 0 and 4x – y –2z = 0

This is system of homogeneous equations can be written as

or AX = O, where

A=

Now |A| =

Thus |A| ¹ 0, So, the given system has only the trivial solution given by x=y=z=0

           

Q8.      The Fourier series of ¦(x) is ¦(x) =

Where ,

Now   

 

Fourier series is

Q9(a)   Even function:

A function ¦(x) is said to be even function if  ¦(-x) = ¦(x)

Odd Function:

A function ¦(x) is said to be odd function if  ¦(-x) = -¦(x)

Example:

Cos x, x2 are even functions and Sin x, x are odd functions

Q9(b)   Let  be the resultant of the three forces,*     == 3i + 4j + 5k

Vector moment of  at P about Q

=

=(2i+4j-k)  (3i+4j+5k)

= i [20+4]-j [10+3] +k [8-12]  =24i-13j-4k

Q10(a) , where function f(t) is defined for t ³ 0 and  s>0 is a        parameteparameter.

 

= =

====

 

Q10(b) =

=

=  =

=

Q11(a) Differential equation is

 

Let y = emx is the solution of given differential equation.

The auxiliary equation is m2-7m+12 = 0  Þ(m-4) (m-3) = 0 Þm=3,4

solution is  y=C1e3x + C2e4x

 

Q11(b) Given

Taking Laplace transform of both sides, we have

 

Þ

But y(0) = 1, y¢(0) = 0Þ