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# Torque

## A force acting on an object that causes the object to rotate.

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Practice Torque
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Estimated12 minsto complete
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Torque

Students will learn to calculate Torque in various situations.

### Key Equations

$\vec{\tau} = \vec{r} \times \vec{F} = r _\perp F = rF _\perp$

Individual torques are determined by multiplying the force applied by the perpendicular component of the moment arm

Guidance
Torque is equal to the cross product as stated above. In general, one can simplify by saying that the torque is equal to the force acting on the object multiplied by the perpendicular distance from the application of the force to the rotational axis. Say you had a seesaw. It is easier to exert torque, get the seesaw to move, if you pushed on the board near the end rather than near the middle. It is the rotational version of Force.

#### Example 2

A 1 m long 2 kg rod is attached to the side of a building with a hinge one one end. The rod is held level by a cable that makes an angle of 45 degrees with the rod and is also attached to the building above the rod. What is the tension in the cable? The situation is illustrated in a diagram below.

##### Solution

There will be multiple steps to this problem. First we'll make a free body diagram for the rod; making free body diagrams in torque problems is just as important as in Newton's Laws problems. In the diagram, the force of tension from the cable, the rod's weight, and the forces from the hinge are shown. For the purposes of calculating torque, an object's weight acts from it's center of mass (half way along the rod in this case). In the diagram below, the force on the rod from the hinge is already broken into it's components to make it easier to visualize.

Now, in order to find the tension in the cable, we'll sum the torques on the rod with the hinge as the axis of rotation. Notice that the sign of the torque due to tension in the cable and the torque due to the rod's weight will be opposite signs because they would cause the rod to rotate in opposite directions.

$\Sigma\tau&=0\\mg\frac{r}{2} - T\sin(\theta)r&=0\\T&=\frac{mgr}{2\sin(\theta)r}\\T&=\frac{mg}{2\sin(\theta)}\\T&=\frac{2\;\text{kg} * 9.8\;\text{m/s}^2}{2\sin(45)}\\T&=13.85\;\text{N}\\$

### Time for Practice

1. Consider hitting someone with a Wiffle ball bat. Will it hurt them more if you grab the end or the middle of the bat when you swing it? Explain your thinking, but do so using the vocabulary of moment of inertia (treat the bat as a rod) and torque (in this case, torques caused by the contact forces the other person’s head and the bat are exerting on each other).
2. A wooden plank is balanced on a pivot, as shown below. Weights are placed at various places on the plank. Consider the torque on the plank caused by weight $A$ .
1. What force, precisely, is responsible for this torque?
2. What is the magnitude (value) of this force, in Newtons?
3. What is the moment arm of the torque produced by weight $A$ ?
4. What is the magnitude of this torque, in $N \cdot m$ ?
5. Repeat parts (a – d) for weights $B$ and $C$ .
6. Calculate the net torque. Is the plank balanced? Explain.

1. At End  -- Moment of inertia at the end $1/3 \;\mathrm{ML}^2$ at the center $1/12 \;\mathrm{ML}^2$ and torque, $\tau = I\alpha$ change the in the same way
2. a. weight b. $19.6 \;\mathrm{N}$ c. plank’s length $(0.8\mathrm{m})$ left of the pivot d. $15.7 \;\mathrm{N \ m}$ , e. Ba. weight, Bb. $14.7 \;\mathrm{N}$ , Bc. plank’s length $(0.3\mathrm{m})$ left of the pivot, Bd. $4.4 \;\mathrm{N \ m}$ , Ca. weight, Cb. $13.6\;\mathrm{N}$ , Cc. plank’s length $(1.00 \;\mathrm{m})$ right of the pivot, Cd. $13.6 \;\mathrm{N \ m}$ , f) $6.5 \;\mathrm{N \ m \ CC}$ , g) no, net torque doesn’t equal zero

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