Newton's Second Law for a System of Particles — Question 10

Section 9-2 · Physics pages 1190–1191

Question 10 When a measured center curve fails a force model Two point masses, 2.0 and 3.0 kg, are claimed to form a horizontally isolated system. For t in seconds their measured positions in meters are x1 = t2 and x2 = 4 −1 2t2. Masses remain constant. t XC 2.4 The measured center trajectory curves upward; isolation would require a straight position-time graph. (a) Test the isolation claim from the center trajectory. (b) If x1 is correct and x2 = 4 + bt2, find the value of b required by horizontal isolation.
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Question 10 - Solution When a measured center curve fails a force model t XC 2.4 (a) Derivation and calculation Form the measured center trajectory: XC = 2t2 + 3(4 −1 2t2) 5 = 2.4 + 0.10t2. aC = 0.20 m/s2 ⇒Fext,x = 5(0.20) = 1.0 N . The claimed horizontal isolation is inconsistent with these trajectories. (b) Result and interpretation With the proposed corrected second trajectory, XC = 12 + (2 + 3b)t2 5 . aC = 2(2 + 3b) 5 = 0 ⇒b = −2 3 m/s2 . Internal forces cannot account for a nonzero acceleration of an otherwise isolated center. Physical check The corrected weighted accelerations cancel: 2(2) + 3(−4/3) = 0.

Question 10

When a measured center curve fails a force model

Two point masses, 2.02.0 and 3.0kg3.0\,\mathrm{kg}, are claimed to form a horizontally isolated system. For tt in seconds their measured positions in meters are x1=t2x_1=t^2 and x2=4−12t2x_2=4-\tfrac12t^2. Masses remain constant.

Diagram shown in the original SVG worksheet.

  1. Test the isolation claim from the center trajectory.

  2. If x1x_1 is correct and x2=4+bt2x_2=4+bt^2, find the value of bb required by horizontal isolation.

Question 10 - Solution

When a measured center curve fails a force model

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Form the measured center trajectory: XC=2t2+3(4−12t2)5=2.4+0.10t2.X_C=\frac{2t^2+3(4-\tfrac12t^2)}5=2.4+0.10t^2. aC=0.20m/s2⇒Fext,x=5(0.20)=1.0N.a_C=0.20\ \mathrm{m/s^2}\Rightarrow\boxed{F_{{\mathrm{ext}},x}=5(0.20)=1.0\ \mathrm N}. The claimed horizontal isolation is inconsistent with these trajectories.

(b) Result and interpretation

With the proposed corrected second trajectory, XC=12+(2+3b)t25.X_C=\frac{12+(2+3b)t^2}{5}. aC=2(2+3b)5=0⇒b=−23m/s2.a_C=\frac{2(2+3b)}5=0\Rightarrow\boxed{b=-\frac23\ \mathrm{m/s^2}}. Internal forces cannot account for a nonzero acceleration of an otherwise isolated center.

Physical check

The corrected weighted accelerations cancel: 2(2)+3(−4/3)=02(2)+3(-4/3)=0.