The Drag Force and Terminal Speed — Question 6

Section 6-3 · Physics pages 822–823

Question 6 Wind changes ground velocity without changing the terminal slip balance Take g = 10 m/s2 and neglect buoyancy unless explicitly specified. A 1 kg particle moves through a uniform horizontal wind⃗u = 6ˆi m/s. Take right and downward as positive x and y. Its only forces are gravity and linear drag⃗Fd = −b(⃗v −⃗u), with b = 2 kg/s. x y wind gravity downward The coordinate y is defined positive downward; drag uses velocity relative to the wind. (a) Find the terminal ground-frame velocity vector. (b) Find its ground speed and angle below horizontal. (c) At an instant when⃗v = 0, find acceleration and explain why drag is then nonzero.
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Question 6 - Solution Wind changes ground velocity without changing the terminal slip balance x y wind gravity downward (a) Balance the two components. Use right and downward positive. The terminal component equations are 0 = −b(vx,t −ux), 0 = mg −bvy,t.⃗ vt = 6ˆi + 5ˆj m/s ,⃗ vt −⃗u = 5ˆj m/s. The terminal motion relative to the air is vertically downward. (b) Combine the ground components. The ground-frame magnitude and direction are |⃗vt| = √ 62 + 52 = √ 61 = 7.810 m/s , θ = tan−1 (5 6 ) = 39.806◦below horizontal . (c) Evaluate the actual relative velocity. At ground-frame rest,⃗v −⃗u = −6ˆi m/s. Therefore⃗ Fd = −2(−6ˆi) = 12ˆi N,⃗ a =⃗Fd + mgˆj m = 12ˆi + 10ˆj m/s2 . Zero ground speed does not eliminate drag when the surrounding air moves.

Question 6

Wind changes ground velocity without changing the terminal slip balance

Take g=10g=10 m/s2^2 and neglect buoyancy unless explicitly specified. A 1 kg particle moves through a uniform horizontal wind u→=6𝒊̂\vec u=6\hat{\mathbf i} m/s. Take right and downward as positive x and y. Its only forces are gravity and linear drag F→d=−b(v→−u→)\vec F_d=-b(\vec v-\vec u), with b=2b=2 kg/s.

Diagram shown in the original SVG worksheet.

  1. Find the terminal ground-frame velocity vector.

  2. Find its ground speed and angle below horizontal.

  3. At an instant when v→=0\vec v=0, find acceleration and explain why drag is then nonzero.

Question 6 - Solution

Wind changes ground velocity without changing the terminal slip balance

Diagram shown in the original SVG worksheet.

(a) Balance the two components.

Use right and downward positive. The terminal component equations are 0=−b(vx,t−ux),0=mg−bvy,t.0=-b(v_{x,t}-u_x),\qquad0=mg-bv_{y,t}. v→t=6𝒊̂+5𝒋̂m/s,v→t−u→=5𝒋̂m/s.\boxed{\vec v_t=6\hat{\mathbf i}+5\hat{\mathbf j}\ \mathrm{m/s}},\qquad \vec v_t-\vec u=5\hat{\mathbf j}\ \mathrm{m/s}. The terminal motion relative to the air is vertically downward.

(b) Combine the ground components.

The ground-frame magnitude and direction are |v→t|=62+52=61=7.810m/s,\boxed{|\vec v_t|=\sqrt{6^2+5^2}=\sqrt{61}=7.810\ \mathrm{m/s}}, θ=tan⁡−1(56)=39.806∘ below horizontal.\boxed{\theta=\tan^{-1}\!\left(\frac56\right)=39.806^\circ\text{ below horizontal}}.

(c) Evaluate the actual relative velocity.

At ground-frame rest, v→−u→=−6𝒊̂\vec v-\vec u=-6\hat{\mathbf i} m/s. Therefore F→d=−2(−6𝒊̂)=12𝒊̂N,\vec F_d=-2(-6\hat{\mathbf i})=12\hat{\mathbf i}\ \mathrm N, a→=F→d+mg𝒋̂m=12𝒊̂+10𝒋̂m/s2.\boxed{\vec a=\frac{\vec F_d+mg\hat{\mathbf j}}m=12\hat{\mathbf i}+10\hat{\mathbf j}\ \mathrm{m/s^2}}. Zero ground speed does not eliminate drag when the surrounding air moves.