\( \newcommand{\sech}{\operatorname{sech}} \) \( \newcommand{\inverse}[1]{#1^\leftarrow} \) \( \newcommand{\<}{\langle} \) \( \newcommand{\>}{\rangle} \) \( \newcommand{\vect}{\mathbf} \) \( \newcommand{\veci}{\mathbf{\hat ı}} \) \( \newcommand{\vecj}{\mathbf{\hat ȷ}} \) \( \newcommand{\veck}{\mathbf{\hat k}} \) \( \newcommand{\curl}{\operatorname{curl}\,} \) \( \newcommand{\dv}{\operatorname{div}\,} \) \( \newcommand{\detThree}[9]{ \operatorname{det}\left( \begin{array}{c c c} #1 & #2 & #3 \\ #4 & #5 & #6 \\ #7 & #8 & #9 \end{array} \right) } \) \( \newcommand{\detTwo}[4]{ \operatorname{det}\left( \begin{array}{c c} #1 & #2 \\ #3 & #4 \end{array} \right) } \)

MA 227 Standard C12


Fundamental Theorem of Line Integrals

At the end of the course, each student should be able to…

  • C12: FundThmLine. Apply the Fundamental Theorem of Line Integrals.

C12. Fundamental Theorem of Line Integrals

  • Due to the Chain Rule \(\frac{df}{dt}=\nabla f(\vect r(t))\cdot\frac{d\vect r}{dt}\) and the Fundamental Theorem of Calculus \(\int_a^b\frac{df}{dt}\,dt=[f]_a^b=f(b)-f(a)\), the line integral of a gradient field may be computed simply by reversing the gradient.
    • If \(\vect F=\nabla f\), then \(f\) is called a potential function, and \(\vect F\) is called a conservative field.
    • The Fundamental Theorem of Line Integrals states that \(\int_C \nabla f\cdot d\vect{r}=[f]_A^B=f(B)-f(A)\) where \(A,B\) are the starting/ending points of the curve \(C\).
    • This theorem may be used to find \(\int_C \vect F\cdot d\vect{r}\) more quickly when \(\vect F\) is a conservative field (whenever a potential function \(f\) exists).
    • When \(\vect F\) is conservative and \(C\) is a closed loop (it begins and ends at the same point), then \(\int_C\vect F\cdot d\vect{r}=0\).
  • The curl of a vector field may be used to determine if a field is conservative.
    • The vector field \(\vect F\) is conservative if and only if \(\curl\vect F=\vect 0\).
    • Thus \(\int_C\vect F\cdot d\vect{r}=0\) when \(C\) is a closed loop and \(\curl\vect F=\vect 0\).

Textbook References

  • University Calculus: Early Transcendentals (3rd Ed)
    • 15.3 (exercises 1-12, 18-24)