Skip to main content \(\newcommand{\N}{\mathbb N}
\newcommand{\Z}{\mathbb Z}
\newcommand{\Q}{\mathbb Q}
\newcommand{\R}{\mathbb R}
\newcommand{\lt}{<}
\newcommand{\gt}{>}
\newcommand{\amp}{&}
\definecolor{fillinmathshade}{gray}{0.9}
\newcommand{\fillinmath}[1]{\mathchoice{\colorbox{fillinmathshade}{$\displaystyle \phantom{\,#1\,}$}}{\colorbox{fillinmathshade}{$\textstyle \phantom{\,#1\,}$}}{\colorbox{fillinmathshade}{$\scriptstyle \phantom{\,#1\,}$}}{\colorbox{fillinmathshade}{$\scriptscriptstyle\phantom{\,#1\,}$}}}
\)
Section 11.3 Centripetal Acceleration
When an object moves along a curved path, the instantaneous velocity always points tangent to the curve.
Exercises Model Application - Acceleration Direction
The figure below shows four different instants (A-D) for a car moving clockwise along a curved path at constant speed.
Figure 11.3.1. 1.
Sketch vectors for the instantaneous velocity at each instant.
2.
Sketch vectors for the change in velocity for each case.
3.
Use the definition of instantaneous acceleration to determine the direction of the car’s acceleration at instant A.
Exercises Model Application - Acceleration Magnitude
The figure below shows three identical cars, each moving around a circular track. Cars A and B move at different constant speeds around tracks with the same radius. Cars A and C move at the same speed around tracks with different radii.
Figure 11.3.2. 1.
Predict which of the three cars has an acceleration with the largest magnitude. Explain your reasoning
The figure below shows several instants for the cars described above. In each case, the two points are separated by the same distance along the path.
Figure 11.3.3. 2.
Sketch vectors for the instantaneous velocity for each point.
3.
Sketch vectors for the change in velocity for each case.
4.
Use the definition of instantaneous acceleration to rank the magnitudes of the cars’ accelerations.
Definition 11.3.4 . Centripetal Acceleration.
An object moving along a curved path experiences a
centripetal acceleration that points perpendicular to the path (inward) with magnitude
\(a_{c} = \frac{v^2}{r}\text{,}\) where
\(r\) is the local radius of curvature. If the object is moving at constant speed, the acceleration is entirely centripetal.