Graphical Integration in Motion Analysis — Question 2

Section 2-9 · Physics pages 294–295

Question 2 An acceleration area needs an initial velocity A cart has x(0) = 2 m and v(0) = −1 m/s on an east-positive track. Its acceleration is +2 m/s2 during 0–2 s, −1 m/s2 during 2–5 s, and zero during 5–7 s. Ideal finite jumps in acceleration take no time; velocity remains continuous. Use v(t) = v(0) + ∫t 0 a(u) du and then signed velocity areas to obtain position changes. t (s) a (m/s2) 2 5 7 −1 2 Horizontal segments give acceleration; dashed jumps have zero duration. (a) Find the velocities at 2, 5 and 7 s and describe the velocity graph between them. Find all zero-velocity times or intervals. (b) Find the smallest position reached, the final position and the total distance traveled. (c) What does the total acceleration area over 0–7 s represent? Why is it neither final velocity by itself nor displacement? (d) Suppose the same acceleration record instead starts with v(0) = 0, keeping x(0) = 2 m. How do the final velocity and position change? Can an acceleration graph alone establish rest on its zero portion?
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Question 2 - Solution An acceleration area needs an initial velocity t (s) a (m/s2) 2 5 7 −1 2 (a) Carry the velocity forward through each area. The acceleration areas are +4, −3, 0 m/s. Therefore v(2) = 3, v(5) = 0, v(7) = 0 (m/s) . The velocity graph rises linearly from −1 to 3, falls linearly to zero and remains zero. On the first stage v = −1 + 2t in SI numerical values, so the reversal occurs at t = 0.5 s . The cart is then at rest throughout 5 ≤t ≤7 s. (b) Integrate velocity, splitting distance at the reversal. The initial negative triangle has area −1 2(0.5)(1) = −0.25 m. Hence xmin = 1.75 m at 0.5 s. The signed area during 0–2 s is the trapezoid 2(−1 + 3)/2 = 2 m. The next stage contributes 3(3 + 0)/2 = 4.5 m. The final stage contributes zero: x(7) = 2 + 2 + 4.5 = 8.5 m . Displacement is 6.5 m. Restoring the canceled backward length gives D = 6.5 + 2(0.25) = 7.0 m . (c) Check the units and the integration constant. Total acceleration area is ∆v = 1 m/s . Adding v(0) = −1 m/s gives final velocity zero. Position change requires integrating velocity, whose area has units of metres. (d) A constant shift in velocity accumulates throughout the run. vnew(t) −v(t) = 1 m/s, xnew(t) −x(t) = (1 m/s)t. Raising the initial velocity by 1 m/s raises the entire velocity graph by that amount. The new final velocity is 1 m/s and displacement increases by 1(7) = 7 m. Thus x(7) = 15.5 m . Zero acceleration only fixes velocity at its already attained value; it does not force that value to be zero.

Question 2

An acceleration area needs an initial velocity

A cart has x(0)=2mx(0)=2\ \mathrm{m} and v(0)=−1m/sv(0)=-1\ \mathrm{m/s} on an east-positive track. Its acceleration is +2m/s2+2\ \mathrm{m/s^2} during 0–2 s, −1m/s2-1\ \mathrm{m/s^2} during 2–5 s, and zero during 5–7 s. Ideal finite jumps in acceleration take no time; velocity remains continuous.

Use v(t)=v(0)+∫0ta(u)duv(t)=v(0)+\int_0^t a(u)\,du and then signed velocity areas to obtain position changes.

Diagram shown in the original SVG worksheet.

  1. Find the velocities at 2, 5 and 7 s and describe the velocity graph between them. Find all zero-velocity times or intervals.

  2. Find the smallest position reached, the final position and the total distance traveled.

  3. What does the total acceleration area over 0–7 s represent? Why is it neither final velocity by itself nor displacement?

  4. Suppose the same acceleration record instead starts with v(0)=0v(0)=0, keeping x(0)=2mx(0)=2\ \mathrm{m}. How do the final velocity and position change? Can an acceleration graph alone establish rest on its zero portion?

Question 2 - Solution

An acceleration area needs an initial velocity

Diagram shown in the original SVG worksheet.

(a) Carry the velocity forward through each area.

The acceleration areas are +4,−3,0m/s+4,-3,0\ \mathrm{m/s}. Therefore v(2)=3,v(5)=0,v(7)=0(m/s).\boxed{v(2)=3,\quad v(5)=0,\quad v(7)=0\quad(\mathrm{m/s})}. The velocity graph rises linearly from −1-1 to 3, falls linearly to zero and remains zero. On the first stage v=−1+2tv=-1+2t in SI numerical values, so the reversal occurs at t=0.5s\boxed{t=0.5\ \mathrm{s}}. The cart is then at rest throughout 5≤t≤7s5\leq t\leq7\ \mathrm{s}.

(b) Integrate velocity, splitting distance at the reversal.

The initial negative triangle has area −12(0.5)(1)=−0.25m-\tfrac12(0.5)(1)=-0.25\ \mathrm{m}. Hence xmin=1.75m\boxed{x_{\min}=1.75\ \mathrm{m}} at 0.5 s. The signed area during 0–2 s is the trapezoid 2(−1+3)/2=2m2(-1+3)/2=2\ \mathrm{m}. The next stage contributes 3(3+0)/2=4.5m3(3+0)/2=4.5\ \mathrm{m}. The final stage contributes zero: x(7)=2+2+4.5=8.5m.\boxed{x(7)=2+2+4.5=8.5\ \mathrm{m}}. Displacement is 6.5 m. Restoring the canceled backward length gives D=6.5+2(0.25)=7.0m.\boxed{D=6.5+2(0.25)=7.0\ \mathrm{m}}.

(c) Check the units and the integration constant.

Total acceleration area is Δv=1m/s\boxed{\Delta v=1\ \mathrm{m/s}}. Adding v(0)=−1m/sv(0)=-1\ \mathrm{m/s} gives final velocity zero. Position change requires integrating velocity, whose area has units of metres.

(d) A constant shift in velocity accumulates throughout the run.

vnew(t)−v(t)=1m/s,xnew(t)−x(t)=(1m/s)t.v_{\mathrm{new}}(t)-v(t)=1\ \mathrm{m/s},\qquad x_{\mathrm{new}}(t)-x(t)=(1\ \mathrm{m/s})t.

Raising the initial velocity by 1 m/s raises the entire velocity graph by that amount. The new final velocity is 1m/s\boxed{1\ \mathrm{m/s}} and displacement increases by 1(7)=7m1(7)=7\ \mathrm{m}. Thus x(7)=15.5m\boxed{x(7)=15.5\ \mathrm{m}}. Zero acceleration only fixes velocity at its already attained value; it does not force that value to be zero.