The Center of Gravity — Question 2

Section 12-3 · Physics pages 1814–1815

Question 2 The center of gravity of an L-shaped plate lies in empty space A uniform thin plate is the union of rectangles 0 ≤x ≤4, 0 ≤y ≤1 and 0 ≤x ≤1, 1 ≤y ≤4, with coordinates in metres. Gravity is uniform. x y 1 1 Uniform plate; the two rectangles meet without overlapping area. (a) Locate its center of gravity. (b) Is a material point required at that location? Explain how a rigid extension could balance the plate there.
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Question 2 - Solution The center of gravity of an L-shaped plate lies in empty space x y 1 1 (a) Derivation and calculation For the two nonoverlapping rectangles, use area weights: A1 = 4, (x1, y1) = (2, .5), A2 = 3, (x2, y2) = (.5, 2.5). xG = 4(2) + 3(.5) 7 = 19 14 m , yG = 4(.5) + 3(2.5) 7 = 19 14 m . (b) Result and interpretation Both coordinates exceed 1 m, so G lies in the missing upper-right region. A massless rigid extension can transmit the supporting force through this point:⃗ R = Mgˆy,⃗ τG =⃗0. The center of gravity is a weighted position and need not lie in material. Physical check The plate is symmetric under interchange of x and y, consistent with xG = yG.

Question 2

The center of gravity of an L-shaped plate lies in empty space

A uniform thin plate is the union of rectangles 0≤x≤40\le x\le4, 0≤y≤10\le y\le1 and 0≤x≤10\le x\le1, 1≤y≤41\le y\le4, with coordinates in metres. Gravity is uniform.

Diagram shown in the original SVG worksheet.

  1. Locate its center of gravity.

  2. Is a material point required at that location? Explain how a rigid extension could balance the plate there.

Question 2 - Solution

The center of gravity of an L-shaped plate lies in empty space

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

For the two nonoverlapping rectangles, use area weights: A1=4,(x1,y1)=(2,.5),A2=3,(x2,y2)=(.5,2.5).A_1=4,\quad(x_1,y_1)=(2,.5),\qquad A_2=3,\quad(x_2,y_2)=(.5,2.5). xG=4(2)+3(.5)7=1914m,x_G=\frac{4(2)+3(.5)}7=\boxed{\frac{19}{14}\ \mathrm m}, yG=4(.5)+3(2.5)7=1914m.y_G=\frac{4(.5)+3(2.5)}7=\boxed{\frac{19}{14}\ \mathrm m}.

(b) Result and interpretation

Both coordinates exceed 11 m, so GG lies in the missing upper-right region. A massless rigid extension can transmit the supporting force through this point: R→=Mgŷ,τ→G=0→.\vec R=Mg\hat y,\qquad \vec\tau_G=\vec0. The center of gravity is a weighted position and need not lie in material.

Physical check

The plate is symmetric under interchange of xx and yy, consistent with xG=yGx_G=y_G.