We started in Calculus I with integrals over an interval, then earlier in this course, we studied integrals over regions in the xy plane and over volumes. Now we'll see what we call line integrals, which are integrals along a path in three-dimensional space (later, we'll see integrals over surfaces).
Here's the idea: consider a surface in 3-D space, defined by z=f(x,y). Suppose there's a path along this surface, as shown below (pretend that there's a surface extending on both sides of the path). The curve C is the projection of this path onto the xy plane.
The line integral
∫Cf(x,y)ds
gives the area of this "curtain" under the curve.
To find ds, zoom in a segment of C in the xy plane:
Since ds=dx2+dy2,
dtds=(dtdx)2+(dtdy)2⟶ds=(dtdx)2+(dtdy)2dt.
If r(t)=⟨x(t),y(t)⟩, we can write this as ds=∣r⃗′(t)∣dt, so the line integral becomes
∫Cf(x,y)ds=∫Cf(x(t),y(t))∣r′(t)∣dt.
Examples
Evaluate the line integral ∫C2+x2yds, where C is the upper half of the unit circle x2+y2=1.
Solution
Since we evaluate a line integral in terms of t, we need to parametrize C. We can do it as follows:
xy=cost=1−x2=1−cos2t=sint
Since this is the upper half of the circle, 0≤t≤π.
Then r′(t)=⟨−sint,cost⟩, so ∣r′(t)∣=sin2t+cos2t=1. Therefore, the line integral becomes
∫0π2+cos2tsintdt=2t−31cos3t∣∣∣∣0π by u-substitution=2π+32
Alternate Solution
What if we parameterized the curve differently (recall that parameterization isn't unique)? It would be simpler to parameterize it as follows, but we'll find that the integral is tricker:
xy=t=1−t2
In this case, −1≤t≤1:
Then r′(t)=⟨1,1−t2−t⟩, so
∣r′(t)∣=1+(1−t2−t)2=1−t21.
Note that the magnitude of the velocity vector is 1300, meaning that the eagle traveled at 1300 ft/min for 10 minutes, for a total of 13,000 ft.
Find the length of the curve r(t)=⟨20sin4t,20cos4t,2t⟩ for 0≤t≤2.
101
Line Integrals in Vector Fields
A line integral arises when we describe the work done on an object moving along a path C in a force field.
At every point in this force field, the object feels a force, but only the tangential component of the force does any work:
∣FT∣=∣F∣cosθ,
where θ is the angle between F and FT.
FT=F⋅Tds=∣r′(t)∣dt: force (where T is the unit tangent vector): distance traveled along the curve
Recall that work is the product of force and distance, so
W=∫CF⋅Tds=∫abF⋅∣r′(t)∣r′(t)∣r′(t)∣dt
Simplifying:
W=∫abF⋅r′(t)dt
Note that work is a scalar.
Electric Force Field
An electric force field is described by
F=(x2+y2+z2)3/2k⟨x,y,z⟩,
where k is a constant. Suppose that k=1 and find the work done by this force field in moving a particle from (1,1,1) to (3,3,3).
Solution
Start by parameterizing the line segment C:
r(t)=⟨1+t,1+t,1+t⟩,0≤t≤2
Then r⃗′(t)=⟨1,1,1⟩ and the force is written in parametric form as
F=(3(1+t2))3/21⟨1+t,1+t,1+t⟩,
so
F⋅r′(t)=27(1+t)33(1+t)=3(1+t)21.
The work, therefore, is
W=∫abF⋅r′(t)dt=∫023(1+t)21dt=−3(1+t)1∣∣∣∣02=332=923
Find the work done by moving an object from (0,0) to (2,8) along the parabola y=2x2 if F=⟨y,x⟩.