Back to Splitting the Acceleration Vector

Activity 10.7.2

Avg difficulty 2.5

In this activity, we will work to understand the sign of aT⃗a_{\vT} and aN⃗a_{\vN}.

  1. The tangential component of acceleration is defined as aT⃗=a⃗⋅T⃗a_{\vT} = \va \cdot \vT, while equation this equation establishes that aT⃗=d(speed)dta_{\vT} = \frac{d\text{(speed)}}{dt} is also true. Use these formulas to determine whether aT⃗a_{\vT} can be zero. Either explain why aT⃗a_{\vT} is always nonzero or describe scenarios in which aT⃗=0a_{\vT}=0.

  2. Determine whether aT⃗a_{\vT} can be negative. Either explain aT⃗a_{\vT} is never negative or describe scenarios in which aT⃗<0a_{\vT}\lt 0

  3. The normal component of acceleration is defined as aN⃗=a⃗⋅N⃗a_{\vN} = \va \cdot \vN, while equation this equation establishes that aN⃗=(speed)∥dT⃗dt∥a_{\vN} = (\text{speed}) \vecmag{\frac{d\vT}{dt}} is also true. Use these formulas to determine whether aN⃗a_{\vN} can be negative. Either explain why aN⃗a_{\vN} is negative or describe scenarios in which aN⃗<0a_{\vN}\lt 0.

  4. Determine whether aN⃗a_{\vN} can be zero. Either explain why aN⃗a_{\vN} is always nonzero or describe scenarios in which aN⃗=0a_{\vN}=0.

Long, Keller & Schlicker, Active Calculus Multivariable, §10.7 Splitting the Acceleration Vector, Activity 10.7.2

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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.