Equilibrium — Question 10

Section 12-1 · Physics pages 1790–1791

Question 10 Equilibrium depends on which motions a constraint allows A bead is constrained to move horizontally along y = h in a potential U(x, y) = kx2/2 −mgy, with k, m, g > 0. The support is ideal and holds the bead at fixed height. mg support y = h The specified potential produces an upward force; the guide supplies the opposing reaction. (a) Find its constrained equilibrium and the vertical support force. (b) What happens if the vertical constraint is removed at that configuration?
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Question 10 - Solution Equilibrium depends on which motions a constraint allows mg support y = h (a) Derivation and calculation The specified potential produces⃗ F = −∇U = −kxˆx + mgˆy. The allowed horizontal coordinate satisfies Fx = 0 =⇒ x = 0 . Vertical constraint balance requires Fy + Ry = 0,⃗ R = −mgˆy . (b) Result and interpretation Removing the vertical constraint makes Ry = 0. At the former constrained equilibrium, ¨x = −kx/m = 0, ¨y = g . For small allowed horizontal displacements, ∆U y=h = 1 2kx2 > 0, so horizontal stability remains a valid constrained statement, but does not establish full two-dimensional equilibrium. Physical check The upward force follows the minus sign in the given −mgy potential; it must not be replaced by conventional downward gravity.

Question 10

Equilibrium depends on which motions a constraint allows

A bead is constrained to move horizontally along y=hy=h in a potential U(x,y)=kx2/2−mgyU(x,y)=kx^2/2-mgy, with k,m,g>0k,m,g>0. The support is ideal and holds the bead at fixed height.

Diagram shown in the original SVG worksheet.

  1. Find its constrained equilibrium and the vertical support force.

  2. What happens if the vertical constraint is removed at that configuration?

Question 10 - Solution

Equilibrium depends on which motions a constraint allows

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

The specified potential produces F→=−𝜵U=−kxx̂+mgŷ.\vec F=-\boldsymbol\nabla U=-kx\hat x+mg\hat y. The allowed horizontal coordinate satisfies Fx=0⇒x=0.F_x=0\quad\Longrightarrow\quad\boxed{x=0}. Vertical constraint balance requires Fy+Ry=0,R→=−mgŷ.F_y+R_y=0,\qquad\boxed{\vec R=-mg\hat y}.

(b) Result and interpretation

Removing the vertical constraint makes Ry=0R_y=0. At the former constrained equilibrium, ẍ=−kx/m=0,ÿ=g.\ddot x=-kx/m=0,\qquad\boxed{\ddot y=g}. For small allowed horizontal displacements, ΔU|y=h=12kx2>0,\Delta U\big|_{y=h}=\tfrac12kx^2>0, so horizontal stability remains a valid constrained statement, but does not establish full two-dimensional equilibrium.

Physical check

The upward force follows the minus sign in the given −mgy-mgy potential; it must not be replaced by conventional downward gravity.