Q4. A particle moves with r = (4 cos t)î + (4 sin t)ĵ m (t in s; the angle t is in radians). Show that its speed is constant and find the angle between v and a.
v = −4 sin t î + 4 cos t ĵ, so v = 4 m s always. a = −4 cos t î − 4 sin t ĵ m s, numerically −r, so it points to the origin. v·a = 16 sin t cos t − 16 sin t cos t = 0, so the angle is 90°: the particle moves on a circle of radius 4 m at constant speed.
Q5. Between t = 0 and t = 2 s a particle’s velocity changes from 4î m s to 4ĵ m s. Find its average acceleration.
Δv = −4î + 4ĵ, so the average acceleration is (−2î + 2ĵ) m s, magnitude 2√2 ≈ 2.83 m s, pointing north-west if î is east and ĵ north. The speed is 4 m s at both ends, yet the average acceleration is not zero: |Δv| is not Δ|v|.
Q6. For r = tî − 2tĵ m (t in s, t ≥ 0), is the velocity ever perpendicular to the acceleration?
v = 3tî − 4tĵ; a = 6tî − 4ĵ. v·a = 18t + 16t = 2t(9t + 8), which is zero only at t = 0, where v = 0 and there is no angle. For t > 0 both factors are positive, so v·a > 0: the angle stays below 90° and the particle keeps speeding up. They are never perpendicular.