5. Integration Over Curves and Surfaces Flashcards
Curve
Definition
-a curve is a path through space described parametrically by writing the position vector as a function of a parameter t that varies along the curve
Equations of Curves
General Form of a Straight Line
|r (t) = |a + t |b
-where |a and |b are constant
Equations of Curves
General Form of a Parabola
|r(t) = (at, bt² ,0)
Equations of Curves
Helix of Radius 1
|r(t) = (cos t , sin t , t)
Line Integral
Description
- the domain of a one dimensional definite integral does not have to lie on the x axis
- instead we can integrate along any one dimensional curve embedded in three dimensional space
- an integral of this kind is called a line integral
Line Integral
Arc Length Equation
arc length = ∫ ds
-where ds measures the distance moved in an infinitesimal step from |r to |r+d|r , ds = | d|r |
Line Integrals
|r)(t) in parametric form
|r(t) = ( x(t) , y(t) , z(t) )
Line Integrals
d|r
d|r = d|r/dt * dt
= ( dx/dt dt , dy/dt dt , dz/dt dt)
= (dx\dt , dy/dt , dz/dt) dt
Line Integrals
ds
ds = | d|r |
ds² = ((dx/dt)² , (dy/dt)² , (dz/dt)²) dt²
so:
ds = [ (dx/dt)² + (dy/dt)² + (dz/dt)² ]^(1/2) * dt
Properties of Line Integrals and Closed Curves
Addition
-if Q is an intermediate point on curve C between points P and R then:
the integral of the line between P and Q plus the integral of the line between Q and R, is equal to the integral of the line between P and R
Properties of Line Integrals and Closed Curves
Closed Curves
-if C is a simple closed curve (ie is made of one non-intersecting loop), then the line integral around the curve is written:
∮ f(|r)
and is independent of the starting point
The Vector Line Integral
-suppose we have a curve C given by |r(t) and a vector field F defined on the curve C
-we can integrate |F(|r) along the curve with respect to arc length giving:
∫ |F(|r) ds = (∫F1 ds , ∫F2 ds , ∫F3 ds)
The Scalar Line Integral
-suppose we have a curve C given by |r(t) and a vector field F defined on the curve C
-formed by integrating the component of |F in the direction of unit tangent vector ^T, which points in the direction of d|r
∫|F . ^T
-and since ^T ds = d|r (as ^T is the direction of d|r and ds is the magnitude of ds
-so the scalar line integral is usually written:
∫|F . d|r
Work
-if |F is a force field acting on a particle moving along the curve C from A to B,
-then the work done in displacing the particle an infinitesimal distance d|x along the curve is |F.d|x
-thus the total work done in moving the particle from A to B is given by:
W = A,B ∫ |F . d|x
(d|x = d|r)
Circulation
-the circulation of a vector field |F around a closed curve C is defined as:
∮ |F . d|x
-note that circulation changes sign under reversal of direction