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File: Vector Calculus Book Pdf 171119 | Chap 16
math214 chapter 16 vector calculus 0 1 line integrals consider a smooth plane curve c in the space given by the parametric equations x x t y y t z ...

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               MATH214
               Chapter 16: Vector Calculus
               0.1     Line Integrals
               Consider a smooth plane curve C in the space given by the parametric equations
                                      x=x(t),     y = y(t),   z = z(t),     a ≤ t ≤ b                    (1)
                                                                             ′
               or r(t) = x(t)i + y(t)j + z(t)k. Then, r’ is continuous and r (t) 6= 0.
               Construct a uniform partition of [a,b] into n subintervals [t      , t ] with a point t∗ in it.
                                                                               i−1  i                i
               Show Fig 1 book for corresponding partition along arc length parameter s.
               0.2     Definition 0.1: Line integral of Scalar Function f along C
               - f is defined on smooth curve C given by equations (1)
               Then,                    Z
                                                                 n
                                           f(x,y,z)ds = lim Xf(x∗,y∗,z∗)∆s
                                                          n→∞          i  i  i     i
                                          C                     i=1
               is the line integral of f along C, if this limit exists.
               0.3     Theorem 0.1: Evaluation of Line Integral of a Scalar Func-
                       tion f along C
               Discuss: Evaluation of arc length of curve C between a and b.
                   The line integral of f along C can be evaluated as
                         Z f(x,y,z)ds = Z bf(x(t),y(t),z(t))sµdx¶2 +µdy¶2 +µdz¶2dt
                           C                 a                        dt        dt        dt
              0.4    Theorem 0.2: Line Integral of a Scalar Function f along C
                     with respect to x, y, and z
                                    Z                Z b                   ′
                                       f(x,y,z)dx =      f(x(t),y(t),z(t))x (t)dt
                                     C                 a
                                    Z f(x,y,z)dy = Z bf(x(t),y(t),z(t))y′(t)dt
                                      C                a
                                    Z f(x,y,z)dz = Z bf(x(t),y(t),z(t))z′(t)dt
                                      C                a
              0.5    Definition 0.2: Vector Field
              If E ⊆ R3, then a vector field on R3 is a function F that assigns to each point (x,y,z) in
              E a three-dimensional vector F(x,y,z). It ca be expressed as
                                  F(x,y,z) = P(x,y,z)i+Q(x,y,z)j+R(x,y,z)k
              0.6    Definition 0.3: Flow Lines or Streamlines
              The flow lines of a vector field F are the curves C in the space (or plane) such that the
              vectors in the vector field are tangents to these curves.
              Alternative Definition:
              The flow lines or streamlines of a vector field are the paths followed by particles whose
              velocity field is the given vector field.
                  More precisely, if
                                  F(x,y,z) = P(x,y,z)i+Q(x,y,z)j+R(x,y,z)k
              and a flow line curve C has the parametric representation r(t) = (x(t),y(t),z(t)) then the
              components of r satisfy the differential equation
                   dx(t) = P(x(t),y(t),z(t))  dy(t) = Q(x(t),y(t),z(t))  dz(t) = R(x(t),y(t),z(t))
                   dt                         dt                          dt
              0.7    Definition 0.4: Work Done to Move Particle with Force F
                     along C
                                    W=Z F(x,y,z)·T(x,y,z)ds=Z F·Tds
                                           C                           C
              where, T(x,y,z) is the unit tangent vector at the point (x,y,z) on C.
               0.8     Theorem 0.3: Work Done to Move Particle with Force F
                       along C, Using a parametric Representation of C
                                            Z b                      ′        Z
                                       W= a F(x(t),y(t),z(t))·r(t)dt = CF·dr
                   Show Why?
               0.9     Definition 0.5: Line Integral of a Vector Field F along C
               - F is a continuous vector field defined on C
               - C is a smooth curve given by r(t), a ≤ t ≤ b
               Then, the line integral of the vector field F along C is given by
                                        Z           Z b           ′        Z
                                         C F · dr =  a F(r(t)) · r (t)dt =  C F · Tds
               0.10      Alternative Representation of a Line Integral of a Vector
                         Field F along C
               - If F(x,y,z) = hP(x,y,z),Q(x,y,z),R(x,y,z)i
               - r(t) = hx(t),y(t),z(t)i
               Then,
                         Z b           ′        Z                  Z                 Z
                          a F(r(t))·r(t)dt = CP(x,y,z)dx+ CQ(x,y,z)dy+ CR(x,y,z)dz
                   Show Why?
               0.11      Theorem 1: Integration of Conservative Vector Fields
               – C is a smooth curve given by r(t) where a ≤ t ≤ b,
               .     r(a) = hx ,y ,z i, and r(b) = hx ,y ,z i
                               1  1  1                 2  2  2
               – f is defined on a domain D containing C,
               – f is differentiable and its gradient vector ∇f is continuous on C. Then,
                               Z ∇f ·dr = f(r(b))−f(r(a)) = f(x ,y ,z )−f(x ,y ,z )
                                                                       2  2  2        1  1  1
                                 C
                   Work on proof.
               0.12     Alternative for Theorem 1: Integration of Conservative
                        Vector Fields
               – F is continuous on D ⊆ R3,
               – D contains a smooth curve C given by r(t) where a ≤ t ≤ b,
               .    r(a) = hx ,y ,z i, and r(b) = hx ,y ,z i
                              1  1  1                 2  2  2
               – F is a conservative vector field in the domain D. It means there is f such that F = ∇f.
               Then,
                         ZCF·dr=ZC∇f·dr=f(r(b))−f(r(a))=f(x2,y2,z2)−f(x1,y1,z1)
                   Work on proof and discuss examples
               0.13     Definition 1: Independence of Path
               – F continuous vector field on D.
               – C and C two curves or paths contained in D.
                   1       2
               – C and C have the same initial and terminal point.
                   1       2           R
               Then, the line integral C F · dr is independent of path if
                                                  Z F·dr=Z F·dr
                                                   C            C
                                                     1           2
               0.14     Theorem 2:
               R F·dris independent of path in D if and only if R F·dr = 0 for every piecewise-smooth
                C                                                   C
               closed path C in D.
               Discuss proof.
               Aclosed path is one for which its terminal point coincides with its initial point.
               0.15     Corollary:
               If F is a conservative vector field defined on D then, the line integral R F·dr is independent
                                                                                     C
               of path in D.
               Is the reciprocal statement true?
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