Some Particular Forces — Question 10

Section 5-6 · Physics pages 730–731

Question 10 A spring force has a signed displacement law A horizontal spring exerts Fx = −kx on a 2 kg slider, with k = 50 N/m and x measured from the relaxed position. The track is frictionless and vertical forces balance. x relaxed Fx For positive extension the given spring force points back toward x=0. (a) Find force and acceleration at x = +0.10 m and x = −0.06 m. (b) At x = 0, must the slider be at rest? (c) Explain why the spring is not interchangeable with a tension-only cord.
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Question 10 - Solution A spring force has a signed displacement law x relaxed Fx (a) Apply the restoring sign. Fx = −kx, ax = −k mx : (F, a).10 = (−5, −2.5), (F, a)−.06 = (3, 1.5) (SI) At +0.10 m, Fx = −5 N and ax = −2.5 m/s2. At -0.06 m, Fx = +3 N and ax = +1.5 m/s2. (b) Distinguish force from velocity. x = 0 ⇒Fx = 0, ax = 0, vx unrestricted by this instantaneous condition The spring force and horizontal acceleration vanish at x=0, but the slider may pass through with nonzero velocity. The instantaneous force law does not specify the motion’s initial conditions. (c) Compare physical models. Fxx = −kx2 ≤0, Fx changes sign at x = 0; Tcord ≥0 The supplied spring law allows both pulling and pushing relative to the relaxed position. A flexible cord can sustain tension but not a compressive push. No full oscillation solution is needed to distinguish these models.

Question 10

A spring force has a signed displacement law

A horizontal spring exerts Fx=−kxF_x=-kx on a 2 kg slider, with k=50k=50 N/m and x measured from the relaxed position. The track is frictionless and vertical forces balance.

Diagram shown in the original SVG worksheet.

  1. Find force and acceleration at x=+0.10x=+0.10 m and x=−0.06x=-0.06 m.

  2. At x=0x=0, must the slider be at rest?

  3. Explain why the spring is not interchangeable with a tension-only cord.

Question 10 - Solution

A spring force has a signed displacement law

Diagram shown in the original SVG worksheet.

(a) Apply the restoring sign.

Fx=−kx,ax=−kmx:(F,a).10=(−5,−2.5),(F,a)−.06=(3,1.5)(SI)F_x=-kx,\quad a_x=-\frac{k}{m}x:\quad\boxed{(F,a)_{.10}=(-5,-2.5),\quad(F,a)_{-.06}=(3,1.5)}\ \text{(SI)} At +0.10 m, Fx=−5F_x=-5 N and ax=−2.5a_x=-2.5 m/s2^2. At -0.06 m, Fx=+3F_x=+3 N and ax=+1.5a_x=+1.5 m/s2^2.

(b) Distinguish force from velocity.

x=0⇒Fx=0,ax=0,vx unrestricted by this instantaneous conditionx=0\ \Rightarrow\ F_x=0,\ a_x=0,\quad v_x\text{ unrestricted by this instantaneous condition} The spring force and horizontal acceleration vanish at x=0, but the slider may pass through with nonzero velocity. The instantaneous force law does not specify the motion’s initial conditions.

(c) Compare physical models.

Fxx=−kx2≤0,Fx changes sign at x=0;Tcord≥0F_xx=-kx^2\le0,\quad F_x\text{ changes sign at }x=0;\qquad T_{\mathrm{cord}}\ge0 The supplied spring law allows both pulling and pushing relative to the relaxed position. A flexible cord can sustain tension but not a compressive push. No full oscillation solution is needed to distinguish these models.