- (a)
- \(\vec {F}(x,y) = \vector {1,1}\)
- (b)
- \(\vec {G}(x,y) = \vector {x,y}\)
- (c)
- \(\vec {H}(x,y) = \vector {y,-x}\)
- (d)
- \(\vec {I}(x,y) = \vector {x,-y}\)
We work some examples of line integrals and vector fields.
Work in groups of 3–4, writing your answers on a separate sheet of paper.
Carefully sketch the following vector fields:
Let \(C\) be the circle of radius \(1\), centered at the origin, drawn once in a counterclockwise
direction. Using the fields above, compute:
- (a)
- \(\int _C \vec {F}\dotp \d \vec {p}\)
- (b)
- \(\int _C \vec {G}\dotp \d \vec {p}\)
- (c)
- \(\int _C \vec {H}\dotp \d \vec {p}\)
- (d)
- \(\int _C \vec {I}\dotp \d \vec {p}\)
Let \(T\) be the triangle with vertices at \((-2,-1)\), \((2,-1)\), and \((0,2)\) drawn once in a counterclockwise
direction. Using the fields above, compute:
- (a)
- \(\int _T \vec {F}\dotp \d \vec {p}\)
- (b)
- \(\int _T \vec {G}\dotp \d \vec {p}\)
- (c)
- \(\int _T \vec {H}\dotp \d \vec {p}\)
- (d)
- \(\int _T \vec {I}\dotp \d \vec {p}\)
Let \(A\) be the path connecting \((-2,-1)\) to \((2,-1)\) to \((0,2)\). Note, this is not a closed path. Using the
fields above, compute:
- (a)
- \(\int _A \vec {F}\dotp \d \vec {p}\)
- (b)
- \(\int _A \vec {G}\dotp \d \vec {p}\)
- (c)
- \(\int _A \vec {H}\dotp \d \vec {p}\)
- (d)
- \(\int _A \vec {I}\dotp \d \vec {p}\)
The work \(W\) done by a force \(\vec {F}\) on an object moving along a curve \(C\), parameterized by \(\vec {p}(t)\) is
given by:
\[ W = \int _C \vec {F}\dotp \d \vec {p} \]
A raindrop of mass \(0.001\unit {kg}\) slides from the top of a flat windshield to the bottom. If the
windshield is \(\frac {1}{2} \unit {m}\) high and \(\frac {1}{2}\unit {m}\) deep, how much work is done by gravity? (Assume that the
acceleration due to gravity is \(10 \unit {m}/\unit {s}^2\).)
A skateboarder of mass \(70\unit {kg}\) rolls from the left side of a circular half-pipe
of radius \(3\unit {m}\) to the right side. How much work is done by gravity?