Line Integral

Work in progress. This note is still being written and incomplete.

2 min read Last updated Tue Aug 18 2026 03:09:13 GMT+0000 (Coordinated Universal Time)

Let CC be a smooth curve with parametric equations x=x(t)x = x(t), y=y(t)y = y(t), z=z(t)z = z(t), atba \le t \le b, and ff defined on CC. Let P={t0,t1,,tn}P = \{t_0, t_1, \dots, t_n\}, a=t0<t1<<tn=ba = t_0 < t_1 < \dots < t_n = b, be a partition of [a,b][a,b], dividing CC into nn subarcs. Let Δsk\Delta s_k be the length of the kkth subarc, and (xk,yk,zk)(x_k^*, y_k^*, z_k^*) a sample point on the kkth subarc. The line integral of ff over CC with respect to arc length is

Cf(x,y,z)ds=limmax{Δsk}0k=1nf(xk,yk,zk)Δsk\int_C f(x,y,z)\,\text{d}s = \lim_{\max\{\Delta s_k\} \to 0} \sum_{k=1}^{n} f(x_k^*, y_k^*, z_k^*)\,\Delta s_k

provided the limit exists and does not depend on the choice of partition or sample points.

For r(t)=x(t)i^+y(t)j^+z(t)k^\boldsymbol{r}(t) = x(t)\hat{i} + y(t)\hat{j} + z(t)\hat{k}, atba \le t \le b,

ds=r(t)dt=(dxdt)2+(dydt)2+(dzdt)2dt\text{d}s = \lVert \boldsymbol{r}'(t) \rVert\,\text{d}t = \sqrt{\left(\frac{\text{d}x}{\text{d}t}\right)^2 + \left(\frac{\text{d}y}{\text{d}t}\right)^2 + \left(\frac{\text{d}z}{\text{d}t}\right)^2}\,\text{d}t

so

Cf(x,y,z)ds=abf(x(t),y(t),z(t))r(t)dt\int_C f(x,y,z)\,\text{d}s = \int_a^b f(x(t),y(t),z(t))\,\lVert \boldsymbol{r}'(t) \rVert\,\text{d}t

Line Integral of a Vector Field

Let F\boldsymbol{F} be a vector field and CC a piecewise smooth oriented curve parametrized by r(t)=x(t)i^+y(t)j^+z(t)k^\boldsymbol{r}(t) = x(t)\hat{i} + y(t)\hat{j} + z(t)\hat{k}, atba \le t \le b. The line integral of F\boldsymbol{F} along CC is

CFdr=abF(r(t))r(t)dt\int_C \boldsymbol{F} \cdot \text{d}\boldsymbol{r} = \int_a^b \boldsymbol{F}(\boldsymbol{r}(t)) \cdot \boldsymbol{r}'(t)\,\text{d}t

For F=Pi^+Qj^+Rk^\boldsymbol{F} = P\hat{i} + Q\hat{j} + R\hat{k},

CFdr=CPdx+Qdy+Rdz\int_C \boldsymbol{F} \cdot \text{d}\boldsymbol{r} = \int_C P\,\text{d}x + Q\,\text{d}y + R\,\text{d}z

Work

For a particle moving along a smooth curve CC, oriented in the direction of motion, under a continuous force field F\boldsymbol{F}, the work done by F\boldsymbol{F} on the particle is

W=CFdrW = \int_C \boldsymbol{F} \cdot \text{d}\boldsymbol{r}
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