{
  "aliases": [
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  "body": "\n## Statement\n\nLet $\\gamma \\colon [a, b] \\to \\mathbb{R}^n$ be a piecewise $C^1$ curve with image $C$, and let $\\gamma^- \\colon [a, b] \\to \\mathbb{R}^n$, $\\gamma^-(t) = \\gamma(a + b - t)$, be the reversed curve.\nFor each continuous vector field $F$ on $C$ and each continuous function $f$ on $C$,\n$$\\int_{\\gamma^-} F \\cdot d\\mathbf{r} = -\\int_\\gamma F \\cdot d\\mathbf{r}, \\qquad \\int_{\\gamma^-} f \\, ds = \\int_\\gamma f \\, ds.$$\n\n## Remarks\n\nProof: by the [[parametric formula|0W3W1VYWBP]], $(\\gamma^-)'(t) = -\\gamma'(a + b - t)$. The substitution $u = a + b - t$ then gives both identities.\nThe [[line integral of a vector field|0YS8RX87F4]] depends on the orientation of the curve. The [[line integral of a scalar field|0M50E4WYWJ]] does not, because it uses only $\\|\\gamma'\\|$.\nMore generally, under a $C^1$ change of parameter $\\varphi$ with $\\varphi' \u003e 0$, the vector line integral does not change. With $\\varphi' \u003c 0$ it changes sign.\n\n## Explanations\n\n### L1 human\n\nIf a force helps you along a path, it works against you on the way back.\nSo the work, a line integral of a vector field, changes sign when you reverse the path. The length of the path and the mass of a wire do not.\n",
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  "name": "Reversing a path changes the sign of a line integral",
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