The Center of Gravity — Question 7

Section 12-3 · Physics pages 1824–1825

Question 7 One orientation fixes the weight line but not a unique point on it A body has total downward weight 150 N and gravity torque −45 N m about the origin in a vertical plane. Its orientation is held fixed. x y 150 N .30 m Schematic; labels, not drawing lengths, specify the data. (a) Find the horizontal coordinate of the resultant weight line. (b) Can these two measurements determine the vertical coordinate of the center of gravity?
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Question 7 - Solution One orientation fixes the weight line but not a unique point on it x y 150 N .30 m (a) Derivation and calculation A downward resultant⃗W = −150ˆy N acting at (xG, yG) has moment τz = xG(−150) −yG(0) = −150xG. Hence −150xG = −45 =⇒ xG = .300 m . (b) Result and interpretation The measurement fixes the line x = .300 m , y arbitrary. Translation of the application point along this vertical line leaves the moment unchanged: ∆⃗r ×⃗W = (∆yˆy) × (−150ˆy) =⃗0. A second independent orientation or geometric constraint is needed to recover a particular height. Physical check The clockwise moment is consistent with a downward force to the right of the origin.

Question 7

One orientation fixes the weight line but not a unique point on it

A body has total downward weight 150N150\,\mathrm N and gravity torque −45Nm-45\,\mathrm{N\,m} about the origin in a vertical plane. Its orientation is held fixed.

Diagram shown in the original SVG worksheet.

  1. Find the horizontal coordinate of the resultant weight line.

  2. Can these two measurements determine the vertical coordinate of the center of gravity?

Question 7 - Solution

One orientation fixes the weight line but not a unique point on it

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

A downward resultant W→=−150ŷ\vec W=-150\hat y N acting at (xG,yG)(x_G,y_G) has moment τz=xG(−150)−yG(0)=−150xG.\tau_z=x_G(-150)-y_G(0)=-150x_G. Hence −150xG=−45⇒xG=.300m.-150x_G=-45\quad\Longrightarrow\quad\boxed{x_G=.300\ \mathrm m}.

(b) Result and interpretation

The measurement fixes the line x=.300m,yarbitrary.\boxed{x=.300\ \mathrm m},\qquad y\ \text{arbitrary}. Translation of the application point along this vertical line leaves the moment unchanged: Δr→×W→=(Δyŷ)×(−150ŷ)=0→.\Delta\vec r\times\vec W=(\Delta y\hat y)\times(-150\hat y)=\vec0. A second independent orientation or geometric constraint is needed to recover a particular height.

Physical check

The clockwise moment is consistent with a downward force to the right of the origin.