1 / 23

Chapter 7

Chapter 7 . Section 4: Torque and simple machines. Objectives. Distinguish between torque and force. Calculate the magnitude of a torque on an object. Identify the six types of simple machines. Calculate the mechanical advantage of a simple machine. Rotational motion .

emile
Télécharger la présentation

Chapter 7

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Chapter 7 Section 4: Torque and simple machines

  2. Objectives • Distinguish between torque and force. • Calculate the magnitude of a torque on an object. • Identify the six types of simple machines. • Calculate the mechanical advantage of a simple machine.

  3. Rotational motion • In previous lessons we had studied various examples of uniform circular motion, such as a spinning Ferris wheel or an orbiting satellite. • In this section, we will examine a related type of motion: the motion of a rotating rigid object.

  4. Rotational motion • What is a rigid object? • Answer: In physics, a rigid body is an idealization of a solid body in which deformation is neglected. In other words, the distance between any two given points of a rigid body remains constant in time regardless of external forces exerted on it. Even though such an object cannot physically exist due to relativity, objects can normally be assumed to be perfectly rigid if they are not moving near the speed of light.

  5. Rotational motion • What is rotational motion? • Answer: rotational motion occurs if every particle in the body moves in a circle about a single line. This line is called the axis of rotation. Then the radius vectors from the axis to all particles undergo the same angular displacement in the same time. The axis of rotation need not be with the body. In general, any rotation can be specified completely by the three angular displacements with respect to the rectangular-coordinate axes x, y, and z. Any change in the position of the rigid body is thus completely described by three translational and three rotational coordinates.

  6. Rotational motion • Rotational and translational motion can be analyzed separately. • For example, when a bowling ball strikes the pins, the pins may spin in the air as they fly backward. • These pins have both rotational and translational motion. • More example???

  7. Torque • Torque is a quantity that measures the ability of a force to rotate an object around some axis. • Examples: • Imagine a cat trying to leave a house by pushing perpendicular on a cat-flap door.

  8. Example In each example, the cat is pushing on the door at the same distance from the axis. To produce the same torque, the cat must apply greater force for smaller angles.

  9. Torque • How easily an object rotates on both how much force is applied and on where the force is applied. • The perpendicular distance from the axis of rotation to a line drawn along the direction of the force is equal to d sin  and is called the lever arm.  = Fdsin  torque = force  lever arm

  10. Torque • The applied force may act at an angle. • However, the direction of the lever arm (d sin ) is always perpendicular to the direction of the applied force, as shown here.

  11. Sign of torque • Torque is a vector quantity. In this textbook, we will assign each torque a positive or negative sign, depending on the direction the force tends to rotate an object. • We will use the convention that the sign of the torque is positive if the rotation is counterclockwise and negative if the rotation is clockwise.

  12. Example#1 • A basketball is being pushed by two players during tip-off. One player exerts an upward force of 15 N at a perpendicular distance of 14 cm from the axis of rotation. The second player applies a downward force of 11 N at a distance of 7.0 cm from the axis of rotation. Find the net torque acting on the ball about its center of mass.

  13. solution 1. Define Given: F1 = 15 N F2 = 11 N d1 = 0.14 m d2 = 0.070 m • Unknown: • net = ?

  14. solution • Diagram:

  15. solution 2. Plan Choose an equation or situation: Apply the definition of torque to each force,and add up the individual torques. •  = Fd • net = 1 + 2 = F1d1 + F2d2

  16. solution • Calculate • 1 = F1d1 = (15 N)(–0.14 m) = –2.1 N•m • 2 = F2d2 = (–11 N)(0.070 m) = –0.77N•m net = 1 + 2 = –2.1 N•m – 0.77 N•m • net = –2.9 N•m

  17. Simple Machine • A machine is any device that transmits or modifies force, usually by changing the force applied to an object. • All machines are combinations or modifications of six fundamental types of machines, called simple machines. • These six simple machines are the lever, pulley, inclined plane, wheel and axle, wedge, and screw.

  18. Simple machine • Because the purpose of a simple machine is to change the direction or magnitude of an input force, a useful way of characterizing a simple machine is to compare the output and input force. • This ratio is called mechanical advantage. • If friction is disregarded, mechanical advantage can also be expressed in terms of input and output distance.

  19. Example#2 • The diagrams show two examples of a trunk being loaded onto a truck. • In the first example, a force (F1) of 360 N moves the trunk through a distance (d1) of 1.0 m. This requires 360 N•m of work. • In the second example, a lesser force (F2) of only 120 N would be needed (ignoring friction), but the trunk must be pushed a greater distance (d2) of 3.0 m. This also requires 360 N•m of work.

  20. Simple Machines • The simple machines we have considered so far are ideal, frictionless machines. • Real machines, however, are not frictionless. Some of the input energy is dissipated as sound or heat. • The efficiency of a machine is the ratio of useful work output to work input.

  21. Efficient machines • The efficiency of an ideal (frictionless) machine is 1, or 100 percent. • The efficiency of real machines is always less than 1.

  22. Homework • Do problems 1-3 in your book page 248

  23. Closure • Today we learned about torque and the different types of simple machines. • Next class we are going to have a lab about chapter 7

More Related