Newton's Second Law for a System of Particles — Question 4

Section 9-2 · Physics pages 1178–1179

Question 4 Following an object after it breaks apart A projectile breaks into fragments in midair at (x, y) = (0, 20) m. Just before breakup its velocity is (6, 4) m/s. Afterward, all fragments remain airborne for 1.0 s. Air resistance is negligible and g = 9.8 m/s2. x y breakup Schematic fragment directions; the center follows a gravity-only trajectory. (a) Find the system center position and velocity 1.0 s after breakup. (b) Explain why knowing the energy released is unnecessary, and state when the stated trajectory would cease to apply.
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Question 4 - Solution Following an object after it breaks apart x y breakup (a) Derivation and calculation For all airborne fragments together, M⃗aC = (0, −Mg) ⇒⃗aC = (0, −g).⃗ RC(t) = (6t, 20 + 4t −4.9t2),⃗ VC(t) = (6, 4 −9.8t).⃗ RC(1) = (6, 19.1) m ,⃗ VC(1) = (6, −5.8) m/s . (b) Result and interpretation The breakup impulses obey ∑ i⃗ Ji,internal =⃗0, so released internal energy is unnecessary for the center trajectory. Ground contact or appreciable drag adds external force and invalidates the gravity-only equation. Physical check The center follows the trajectory of the unbroken projectile while gravity is the only external force.

Question 4

Following an object after it breaks apart

A projectile breaks into fragments in midair at (x,y)=(0,20)m(x,y)=(0,20)\,\mathrm m. Just before breakup its velocity is (6,4)m/s(6,4)\,\mathrm{m/s}. Afterward, all fragments remain airborne for 1.0s1.0\,\mathrm s. Air resistance is negligible and g=9.8m/s2g=9.8\,\mathrm{m/s^2}.

Diagram shown in the original SVG worksheet.

  1. Find the system center position and velocity 1.0s1.0\,\mathrm s after breakup.

  2. Explain why knowing the energy released is unnecessary, and state when the stated trajectory would cease to apply.

Question 4 - Solution

Following an object after it breaks apart

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

For all airborne fragments together, Ma→C=(0,−Mg)⇒a→C=(0,−g).M\vec a_C=(0,-Mg)\Rightarrow\vec a_C=(0,-g). R→C(t)=(6t,20+4t−4.9t2),V→C(t)=(6,4−9.8t).\vec R_C(t)=(6t,20+4t-4.9t^2),\qquad\vec V_C(t)=(6,4-9.8t). R→C(1)=(6,19.1)m,V→C(1)=(6,−5.8)m/s.\boxed{\vec R_C(1)=(6,19.1)\ \mathrm m},\qquad \boxed{\vec V_C(1)=(6,-5.8)\ \mathrm{m/s}}.

(b) Result and interpretation

The breakup impulses obey ∑iJ→i,internal=0→,\sum_i\vec J_{i,\mathrm{internal}}=\vec0, so released internal energy is unnecessary for the center trajectory. Ground contact or appreciable drag adds external force and invalidates the gravity-only equation.

Physical check

The center follows the trajectory of the unbroken projectile while gravity is the only external force.