Question
The torque about the origin $O$ due to a force $\mathbf{F}$ acting on an object with position vector $\mathbf{r}$ is the vector quantity $\mathbf{\tau}=\mathbf{r} \times \mathbf{F}$. If several forces $\mathbf{F}_{j}$ act at positions $\mathbf{r}_{j},$ then the net torque (units: $N-m$ or $\left.l b-f t\right)$ is the sum $$ \boldsymbol{\tau}=\sum \mathbf{r}_{j} \times \mathbf{F}_{j} $$Calculate the net torque about $O$ at $P$, assuming that a $30-\mathrm{kg}$ mass is attached at $P$ [Figure $21(\mathrm{~B})]$. The force $\mathbf{F}_{g}$ due to gravity on a mass $m$ has magnitude $9.8 m \mathrm{~m} / \mathrm{s}^{2}$ in the downward direction.
Step 1
The vectors are given as $\mathbf{U} = (1,1,1)$ and $\mathbf{V} = (0,2,0)$. The cross product is given by $\mathbf{U} \times \mathbf{V} = (2,0,-2)$. Show more…
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In Exercises $67-70,$ the torque about the origin $O$ due to a force $\mathbf{F}$ acting on an object with position vector $\mathbf{r}$ is the vector quantity $\boldsymbol{\tau}=\mathbf{r} \times \mathbf{F}$. If several forces $\mathbf{F}_{j}$ act at positions $\mathbf{r}_{j},$ then the net torque (units: $N-m$ or $\left.l b-f t\right)$ is the sum $$ \boldsymbol{\tau}=\sum \mathbf{r}_{j} \times \mathbf{F}_{j} $$ Calculate the torque $\tau$ about $O$ acting at the point $P$ on the mechanical arm in Figure $21(\mathrm{~A})$, assuming that a 25 -newton force acts as indicated.
Vector Geometry
The Cross Product
The torque about the origin $O$ due to a force F acting on an object with position vector $\mathbf{r}$ is the vector quantity $\tau=\mathbf{r} \times \mathbf{F}.$ If several forces $\mathbf{F}_{j}$ act at positions $\mathbf{r}_{j},$ then the net torque (units: $N-m$ or $l b-f t )$ is the sum $$\tau=\sum \mathbf{r}_{j} \times \mathbf{F}_{j}$$ Torque measures how much the force causes the object to rotate. By Newton's Laws, $\tau$ is equal to the rate of change of angular momentum. \begin{equation}\begin{array}{l}{\text { Calculate the torque } \tau \text { about } O \text { acting at the point } P \text { on the mechanical }} \\ {\text { arm in Figure } 22(\mathrm{A}), \text { assuming that a } 25 \text { -newton force acts as }} \\ {\text { indicated. Ignore the weight of the arm itself. }}\end{array}\end{equation}
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