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Experiment 8: Torques and Rotational Motion, Lab Reports of Physics

chemical formula of torque is τ = rF

Typology: Lab Reports

2020/2021

Uploaded on 05/12/2021

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Experiment 8: Torques and Rotational
Motion
Figure 8.1: The wood block provides necessary height for the hangers to not touch the table.
Figure 8.2: Clamp - The arrow indicates the correct
edge for position measurement.
EQUIPMENT
Fulcrum
Meter Stick
Vernier Caliper
(3) Mass Hangers
Masses
(3) Hanger Clamps (Clamps)
(1) Knife-Edge Clamp
Digital Balance
Triple-Beam Balance
Block of Wood
Unknown Mass (Marble or “Silver” Cube)
TA’s Table:
(1) Dial-O-Gram Balance
1
pf3
pf4
pf5

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Experiment 8: Torques and Rotational

Motion

Figure 8.1: The wood block provides necessary height for the hangers to not touch the table.

Figure 8.2: Clamp - The arrow indicates the correct edge for position measurement.

EQUIPMENT

Fulcrum Meter Stick Vernier Caliper (3) Mass Hangers Masses (3) Hanger Clamps (Clamps) (1) Knife-Edge Clamp Digital Balance Triple-Beam Balance Block of Wood Unknown Mass (Marble or “Silver” Cube)

TA’s Table: (1) Dial-O-Gram Balance

2 Experiment 8: Torques and Rotational Motion

Advance Reading

Text: Torque, center of mass, stable and unstable equi- librium, lever arm

Lab Manual: Appendix B

Objective

To measure torques on a rigid body, to determine the conditions necessary for equilibrium to occur, to per- form error analysis.

Theory

When a force F is applied to a rigid body at any point away from the center of mass, a torque is produced. Torque, τ (Greek letter, tau), can be defined as the tendency to cause rotation. The magnitude of the vec- tor is:

τ = rF sin θ (8.1)

where r is the distance from the point of rotation to the point at which the force is being applied (i.e., lever arm), and F sin θ is the component of the force per- pendicular to r. Note that the unit for torque is mN (meter × newton).

In this experiment, all forces will be acting normal (perpendicular) to the meter stick: θ = 90◦^ ; therefore, sin θ = 1. The equation for torque is simplified:

τ = rF (8.2)

Equilibrium, Latin for equal forces or balance, is reached when the net force and net torque on an object are zero. The first condition is that the vector sum of the forces must equal zero:

ΣF� = ΣF (^) x = ΣFy = ΣFz = 0.0 N (8.3)

The second condition that must be met is that the net torques about any axis of rotation must equal zero. We will use the standard convention for summing torques. Torques that tend to cause counterclockwise rotation, τ (^) cc , will be positive torques, while torques that tend to cause clockwise rotation, τc , will be negative torques.

Σ�τ = Σ�τ (^) cc − Σ�τ (^) c = 0.0 mN (8.4)

The system under consideration for this experiment will need to not only attain equilibrium, but also re- main in equilibrium. This will require that the object be in stable equilibrium, meaning if a slight displace- ment of the system occurs, the system will return to its original position (e.g., a pendulum). If the system were to move farther from its original position when given a slight displacement, it would be in unstable equilibrium (e.g., a ball on a hill).

Once stable equilibrium has been attained for each ex- perimental arrangement, measure the mass at each po- sition using the appropriate balance.

Figure 8.3: Required sketch for each experimental ar- rangement

Once stable equilibrium is attained, sketch each set-up:

x: position F : magnitude of force Arrow : direction of force r: lever arm cc: counterclockwise c: clockwise cm: center of mass f : fulcrum

Name: Section: Date:

Worksheet - Exp 8: Torques and Rotational Motion

Objective: This experiment investigates torque on a rigid body and determines the conditions necessary for static equilibrium.

Theory: When a force �F is applied to a rigid body at any point away from the center of mass, a torque is produced. Torque, τ , can be defined as the tendency to cause rotation. The magnitude of the vector is:

τ = rF sin θ

where r is the distance from the point of rotation to the point at which the force is being applied, and F sin θ is the component of the force perpendicular to r. Note that the unit for torque is the mN (m × Newton). In this experiment, all forces will be acting normal (perpendicular) to the meter stick: θ = 90◦^. Therefore sin θ = 1, and the equation for torque is simplified:

τ = rF.

Rotational equilibrium is obtained when the sum of torques about any axis is equal to zero.

� �τ (^) cc −

�τ (^) c = 0.0 mN

  1. Four hippopotamuses sit on one side of a scale as shown. How many hippos placed on the right side of the scale would balance the system? (5 pts)
  2. How much torque does a hubcap (4 kg) exert when mounted to the center of a wheel of a car (radius = 0.5 m)? (5 pts) mN

Procedure:

Part 1: Quantitative Analysis of Torque

  1. Measure the mass of the hanger clamps (m (^) hc ), record this data below. You will need it throughout the experiment.

mhc =

  1. Place the knife-edge clamp at the 50 cm position of the meter stick with the screw pointing down. Adjust the knife-edge clamp until the meter stick is balanced and horizontal (stable equilibrium). Record the position as x (^) cm (center of mass position), and x (^) f (fulcrum position).
  2. Place a clamp at the x (^) cc =15.0 cm position (position of counter-clockwise torque) and hang 200 g from it.
  3. Place another clamp an the x (^) c =75.0 cm position (position of clockwise torque). Add enough mass to attain equilibrium. If small fractional masses are not available to you, it may be necessary to adjust the position of the 75 cm clamp in order to balance the system.
  4. Measure the mass at each position; recall that the digital balance has a limit of 0.2 kg. Don’t forget to include the mass of the clamps!
  5. Determine the radius from the fulcrum, mass, force, and torque at each position.

(18 pts)

  1. : Calculate the sum of the torques. (Note that the torques are in opposite directions, if one is positive, the other must be negative.) (3 pts)

τ =

  1. Explain how a triple-beam balance works (5 pts). Would such a balance that functions properly on earth yield the correct mass of an object on the moon? Why or why not? (5 pts)

Part 3: Unknown Mass

  1. Determine the mass of a metal cube experimentally, using the torque apparatus however you choose. It is imperitive that you use the cube at your table. If you do not have one, ask your TA for help, do not simply get one from a different table.
  2. Record your table number:
  3. Make a torque-balance sketch of your experimental setup below. (6 pts) m (^) block = (2 pts)
  4. Determine the density of the metal cube by measur- ing its dimensions with the digital caliper and mass using your torque apparatus. (5 pts)

ρ (^) block =

Material: (4 pts)

Density %error: (3 pts)

Density Material (g/cm 3 )

Solids Metal: Aluminum 2. Stainless Steel 7. Brass 8.44 - 8. Bronze 8.74 - 8. Copper 8. Lead 11. Mercury 13. Rock: Granite 2.64 - 2. Slate 2.6 - 3. Diamond 3. Garnet 3.15 - 4. Corundum 3.9 - 4. Wood: Pine (Yellow) 0.37 - 0. Oak 0.60 - 0. Ebony 1.11 - 1. Misc.: Ice 0. Bone 1.7 - 2. Chalk 1.9 - 2. Glass (Lead) 3 - 4

Fluids Atmosphere (STP) 0. Water (20 ◦^ C) 0. Water (0 ◦^ C) 0. Mercury (20 ◦^ C) 13.