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Curvature

Measuring how sharply a path turns independently of its parameterization, and the radius of the best-fitting circle at each point.

Active Calculus Multivariable, Curvature

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7 exercises

Activity 10.6.2

In this activity we will use our previous work in finding unit speed parameterizations of lines and circles to make sense of the definition of curvature.

  1. Recall that in this example we found that the unit speed parameterization of a line through the points (1,2,3)(1,2,3) and (2,0,5)(2,0,5) to be r⃗1(s)=⟨1,2,3⟩+s3⟨1,−2,2⟩\vr_1(s)= \langle 1,2,3\rangle + \frac{s}{3} \langle 1,-2,2 \rangle. Calculate T⃗(s)\vT(s), dT⃗ds\frac{d\vT}{ds}, and ∥dT⃗ds∥\vecmag{ \frac{d\vT}{ds} } for the unit speed parameterization of this line. Note that because we are using the unit speed parameter…

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Activity 10.6.4

In this activity we will look at the measurement of curvature and determine if curvature is a property of the driver or a property of the road. This is a continuation of this activity. As a reminder, a measurement is a property of the driver if the value(s) of that measurement can be different for different drivers (when measured at the same location on the racetrack). A measurement is a property…

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Exercise 11

Let y=f(x)y = f(x) define a curve in the plane. We can consider this curve as a curve in three-space with zz-coordinate 0.

  1. Find a parameterization of the form r⃗(t)=⟨x(t),y(t),z(t)⟩\vr(t) = \langle x(t), y(t), z(t) \rangle of the curve y=f(x)y=f(x) in three-space.

  2. Use the formula to show that

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Exercise 12

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Exercise 13

In this exercise we verify the curvature formula

  1. Explain why

  2. Use the fact that T⃗(t)=r⃗′(t)∥r⃗′(t)∥\vT(t) = \frac{\vr'(t)}{\vecmag{\vr'(t)}} and ∥r⃗′(t)∥=dsdt\vecmag{\vr'(t)} = \frac{ds}{dt} to explain why

  3. The Product Rule shows that Explain why

  4. In Key Idea on T⃗\vT and N⃗\vN we showed that ∥T⃗(t)∥=1\vecmag{\vT(t)} = 1 implies that T⃗(t)\vT(t) is orthogonal to T⃗′(t)\vT'(t) for every value of tt. Explain what this tells us about ∥T⃗(t)×T⃗′(t)∥\vecmag{\vT(t) \times \vT'(t)} and conclude that

  5. Finally, use the fact that κ=∥T⃗′(t)∥∥r⃗′(t)∥\kappa = \frac{\vecmag{\vT'(t)} }{\vecmag{\vr'(t)}} to verify that

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Exercise 15

In this activity, you verified for a specific line that the curvature is 00. The generalization of this is that the unit speed parameterization of a line through (x0,y0,z0)(x_0,y_0,z_0) with direction vector ⟨a,b,c⟩\langle a,b,c\rangle can be given by .

  1. Compute the speed of this parameterization to verify that this has unit speed. This will also show that r⃗ ′(s)=v⃗(s)=T⃗(s)\vr\, '(s)=\vv(s)=\vT(s) (which is not true in general).

  2. Calculate T⃗(s)\vT(s), dT⃗ds\frac{d\vT}{ds}, and ∥dT⃗ds∥\vecmag{ \frac{d\vT}{ds} } for this unit speed parameterization…

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Exercise 16

  1. If u⃗×w⃗=0⃗\vu \times \vw = \vzero, what does this say about the direction of u⃗\vu and w⃗\vw?

  2. Remember that the vector v⃗\vv has magnitude and direction, so the derivative dv⃗dt=a⃗\frac{d\vv}{dt} = \va will measure the change in both the magnitude and direction of of v⃗\vv. Write a few sentences to describe how if v⃗\vv and a⃗=dv⃗dt\va= \frac{d\vv}{dt} are in parallel directions, then the unit normal vector will be undefined at that point.

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Adapted from Active Calculus Multivariable © 2013–2026 Nicholas Long, Mitchel T. Keller, and Steven Schlicker. Licensed under CC BY-SA 4.0. Source: Active Calculus Multivariable. Imported at revision 692c03c.