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M2

Module-4

Vector integral calculus

 


The Line Integral

Let- F be vector function defined throughout some region of space and let C be any curve in that region. is the position vector of a point p (x,y,z) on C then the integral ƪ F .d is called the line integral of  F taken over

Now, since =xi+yi+zk

And if F͞ =F1i + F2 j+ F3  K

 

Q1. Evaluate where F= cos y.i-x siny j and C is the curve y= in the xy plae from (1,0) to (0,1)

Solution: The curve y= i.e x2+y2 =1. Is a circle with centre at the origin and radius unity.

=

=

=       =-1

 

Q2. Evaluate where = (2xy +z2) I +x2j +3xz2 k along the curve x=t, y=t2, z= t3 from (0,0,0) to (1,1,1).

 Solution:    F x dr =

 Put x=t, y=t2, z= t3

Dx=dt ,dy=2tdt,                dz=3t2dt.

F x dr =

=(3t4-6t8) dti  – ( 6t5+3t8 -3t7) dt j +( 4t4+2t7-t2)dt k

=t4-6t3)dti –(6t5+3t8-3t7)dt j+(4t4 + 2t7 – t2)dt k

=

=+

Example 3: Prove that   ͞͞͞F = [y2cos x +z3] i+(2y sin x – 4) j +(3xz2 + 2) k is a conservative field. Find (i) scalar potential for͞͞͞F  (ii) the work done in moving an object in this field from (0, 1, -1) to (/ 2,-1, 2)

Sol.: (a) The field is conservative if cur͞͞͞͞͞͞F = 0.

Now, curl͞͞͞ F = ̷̷ X                    / y            / z

                            Y2COS X +Z3        2y sin x-4     3xz2 + 2

; Cur = (0-0) – (3z2 – 3z2) j + (2y cos x- 2y cos x) k = 0

; F is conservative.

(b) Since F is conservative there exists a scalar potential ȸ such that

F = ȸ

(y2cos x=z3) i + (2y sin x-4) j + (3xz2 + 2) k =   i +   j + k

= y2cos x + z3, = 2y sin x – 4, = 3xz2 + 2

Now, = dx + dy + dz

= (y2cos x + z3) dx +(2y sin x – 4)dy + (3xz2 + 2)dz

= (y2cos x dx + 2y sin x dy) +(z3dx +3xz2dz) +(- 4 dy) + (2 dz)

=d(y2 sin x + z3x – 4y -2z)

ȸ = y2 sin x +z3x – 4y -2z

(c)  now, work done = .d   ͞r

=  dx + (2y sin x – 4) dy + ( 3xz2 + 2) dz

=   (y2 sin x + z3x – 4y + 2z)    (as shown above)

= [ y2 sin x + z3x – 4y + 2z ]( /2, -1, 2)

= [ 1 +8 + 4 + 4 ] – { - 4 – 2} =4 + 15

Sums Based on Line Integral

1. Evaluate where =yz i+zx  j+xy k and C is the position of the curve.

= (a cost)i+(b sint)j+ct k , from y=0 to t=π/4.

Sol.:  = (a cost)i+(b sint)j+ct k

 The parametric eqn. of the curve are x= a cost, y=b sint, z=ct              (i)

=

 Putting values of x,y,z from (i),

dx=-a sint

dy=b cost

dz=c dt

=

=

==

2. Find the circulation of around the curve C where =yi+zj+xk and C is circle .

Soln. Parametric eqn of circle are:

x=a cos

y=a sin

z=0

=xi+yj+zk = a cosi + b cos + 0 k

d=(-a sin i + a cos j)d

Circulation = =+zj+xk). d

=-a sin i + a cos j)d

= =

 

Key takeaways-

  • When the path of integration is closed curve then we use the notation for integration-
      in place of

  • Green’s theorem in a plane

    If C be a regular closed curve in the xy-plane and S is the region bounded by C then,

    Where P and Q are the continuously differentiable functions inside and on C.

     

    Green’s theorem in vector form-

     

    Example-1: Apply Green’s theorem to evaluate where C is the boundary of the area enclosed by the x-axis and the upper half of circle

     

    Sol. We know that by Green’s theorem-

    And it it given that-

    Now comparing the given integral-

    P =   and   Q =

    Now-

    and

    So that by Green’s theorem, we have the following integral-

     

    Example-2: Evaluate by using Green’s theorem, where C is a triangle formed by

    Sol. First we will draw the figure-

    Here the vertices of triangle OED are (0,0), (

    Now by using Green’s theorem-

    Here P = y – sinx, and Q  =cosx

    So that-

    and

    Now-

    =

    Which is the required answer.

     

    Example-3: Verify green’s theorem in xy-plane for where C is the boundary of the region enclosed by

    Sol.

    On comparing with green’s theorem,

    We get-

    P = and Q =

    and

    By using Green’s theorem-

      ………….. (1)

    And left hand side=

    ………….. (2)

    Now,

    Along

    Along

    Put these values in (2), we get-

                   L.H.S. = 1 – 1 = 0

    So that the Green’s theorem is verified.

     


    Surface integrals-

    An integral which we evaluate over a surface is called a surface integral.

                       Surface integral =

     

    Volume integrals-

    The volume integral is denoted by

    And defined as-

    If  , then

     

    Note-

    If in a conservative field 

    Then this is the condition for independence of path.

     

    Example: Evaluate , where S is the surface of the sphere in the first octant.

    Sol. Here-

     

    Which becomes-

     

    Example: Evaluate , where and V is the closed reason bounded by the planes 4x + 2y + z = 8, x = 0, y = 0, z = 0.

    Sol.

    Here-   4x + 2y + z = 8

    Put y = 0 and z = 0 in this, we get

    4x = 8 or x = 2

    Limit of x varies from 0 to 2 and y varies from 0 to 4 – 2x

    And z varies from 0 to 8 – 4x – 2y

    So that-

    So that-

     

    Example: Evaluate if V is the region in the first octant bounded by and the plane x = 2 and .

    Sol.

    x varies from 0 to 2

    The volume will be-

     

    Key takeaways-

  • Surface integral =
  • The volume integral is denoted by
  • 3.     If in a conservative field 

    Then this is the condition for independence of path

     


    Stoke’s theorem (without proofs) and their verification-

    If is any continuously differentiable vector point function and S is a surface bounded by a curve C, then-

     

    Example-1: Verify stoke’s theorem when and surface S is the part of sphere , above the xy-plane.

    Sol.

    We know that by stoke’s theorem,


     

     

    Here C is the unit circle-

    So that-

    Now again on the unit circle C, z = 0

    dz = 0

    Suppose, 

    And           

    Now

      ……………… (1)

    Now-

    Curl

     

    Using spherical polar coordinates-

      ………………… (2)

    From equation (1) and (2), stoke’s theorem is verified.

     

    Example-2: If and C is the boundary of the triangle with vertices at (0, 0, 0), (1, 0, 0) and (1, 1, 0), then evaluate by using Stoke’s theorem.

     

    Sol. here we see that z-coordinates of each vertex of the triangle is zero, so that the triangle lies in the xy-plane and

    Now,

    Curl

    Curl

     

    The equation of the line OB is y = x

    Now by stoke’s theorem,


     

     

    Example-3: Verify Stoke’s theorem for the given function-

    Where C is the unit circle in the xy-plane.

     

    Sol. Suppose-

    Here

    We know that unit circle in xy-plane-

    Or

    So that,

    Now

    Curl

     

    Now,

    Hence the Stoke’s theorem is verified.

     

    Gauss divergence theorem

    If V is the volume bounded by a closed surface S and is a vector point function with continuous derivative-

    Then it can be written as-

    where unit vector to the surface S.

     

    Example-1: Prove the following by using Gauss divergence theorem-

    1.

    2.

    Where S is any closed surface having volume V and

     

    Sol. Here we have by Gauss divergence theorem-

    Where V is the volume enclose by the surface S.

    We know that-

    = 3V

    2.

    Because 

     

    Example – 2 Show that 

    Sol

    By divergence theorem,  ..…(1)

    Comparing  this  with  the  given  problem  let 

    Hence, by (1)

                                        ………….(2)

    Now ,

    Hence, from (2), We get,

     

    Example Based on Gauss Divergence Theorem

  • Show that
  • Soln.  We have Gauss Divergence Theorem

     By data, F=  

    =(n+3)

     

    2 Prove that  =

    Soln. By Gauss Divergence Theorem,

    =

    = =

    .[

    =

    References

     

  • E. Kreyszig, “Advanced Engineering Mathematics”, John Wiley & Sons, 2006.
  • P. G. Hoel, S. C. Port And C. J. Stone, “Introduction To Probability Theory”, Universal Book Stall, 2003.
  • S. Ross, “A First Course in Probability”, Pearson Education India, 2002.
  • W. Feller, “An Introduction To Probability Theory and Its Applications”, Vol. 1, Wiley, 1968.
  • N.P. Bali and M. Goyal, “A Text Book of Engineering Mathematics”, Laxmi Publications, 2010.
  • B.S. Grewal, “Higher Engineering Mathematics”, Khanna Publishers, 2000.
  • T. Veerarajan, “Engineering Mathematics”, Tata Mcgraw-Hill, New Delhi, 2010
  • Higher engineering mathematics, HK Dass
  • BV ramana, higher engineering mathematics
  •  

     

     

     


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