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39-245

Rapid Design through Virtual and Physical Prototyping

Carnegie Mellon University

Course Index
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Introduction to Mechanisms

Yi Zhang
with
Susan Finger
Stephannie Behrens

Table of Contents

2 Mechanisms and Simple Machines

Mechanism: the fundamental physical or chemical processes involved in or responsible for an action, reaction or other natural phenomenon.

Machine: an assemblage of parts that transmit forces, motion and energy in a predetermined manner.

Simple Machine: any of various elementary mechanisms having the elements of which all machines are composed.  Included in this category are the lever, wheel and axle, pulley, inclined plane, wedge and the screw.

The word mechanism has many meanings. In kinematics, a mechanism is a means of transmitting, controlling, or constraining relative movement (Hunt 78). Movements which are electrically, magnetically, pneumatically operated are excluded from the concept of mechanism. The central theme for mechanisms is rigid bodies connected together by joints.

A machine is a combination of rigid or resistant bodies, formed and connected do that they move with definite relative motions and transmit force from the source of power to the resistance to be overcome. A machine has two functions: transmitting definite relative motion and transmitting force.  These functions require strength and rigidity to transmit the forces.

The term mechanism is applied to the combination of geometrical bodies which constitute a machine or part of a machine. A mechanism may therefore be defined as a combination of rigid or resistant bodies, formed and connected so that they move with definite relative motions with respect to one another (Ham et al. 58).

Although a truly rigid body does not exist, many engineering components are rigid because their deformations and distortions are negligible in comparison with their relative movements.

The similarity between machines and mechanisms is that

  • they are both combinations of rigid bodies
  • the relative motion among the rigid bodies are definite.

The difference between machine and mechanism is that machines transform energy to do work, while mechanisms so not necessarily perform this function. The term machinery generally means machines and mechanisms. Figure 2-1 shows a picture of the main part of a diesel engine. The mechanism of its cylinder-link-crank parts is a slider-crank mechanism, as shown in Figure 2-2.

Figure 2-1 Cross section of a power cylinder in a diesel engine

Figure 2-2 Skeleton outline

2.1 The Inclined Plane

Figure 2-3a shows an inclined plane, AB is the base, BC is the height and AC the inclined plane. With the use of the inclined plane a given resistance can be overcome with a smaller force than if the plane is not used. For example, in Figure 2-3b, suppose we wish to raise a weight of 1000 lb. through the vertical distance BC = 2 ft. If this weight were raised vertically and without the use of the inclined plane the force 1000 lb. would have to be exerted through the distance BC. If, however, the inclined plane is used and the weight is moved over its inclined plane AC, a force of only 2/3 of 1000 lb. or 667 lb. is necessary, although this force is exerted through a distance AC which is greater than distance BC.

Figure 2-3 Inclined plane

Using an inclined plane requires a smaller force exerted through a greater distance to do a certain amount of work.

Letting F represent the force required to raise a given weight on the inclined plane, and W the weight to be raised, we have the proportion:

(2-1)

2.1.1 Screw Jack

One of the most common application of the principle of the inclined plane is in the screw jack which is used to overcome a heavy pressure or raise a heavy weight of W by a much smaller force F applied at the handle. R represents the length of the handle and P the pitch of the screw, or the distance advances in one complete turn.

Figure 2-4 The screw jack

Neglecting the friction the following rule is used: The force F multiplied by the distance through which it moves in one complete turn is equal to the weight lifted times the distance through which it is lifted in the same time. In one complete turn the end of the handle describes a circle of circumference 2R. This is the distance through which the force F is exerted.

Therefore from the rule above

(2-2)

and

(2-3)

Suppose R equals 18 in., P equals 1/8 in. and the weight to be lifted equals 100,000 lb., then the force required at F is then 110 lb. This means that, neglecting friction, 110 lb. at F will raise 100,000 lb. at W, but the weight lifted moves much slower than the force applied at F.

2.2 Gears

A gear, or toothed wheel, when in operation, may actually be considered as a lever with the additional feature that it can be rotated continuously, instead of rocking back and forth through a short distance. One of the basic relationships for a gear is the number of teeth, the diameter, and the rotary velocity of gears. Figure 2-5 shows the ends of two shafts A and B connected by 2 gears of 24 and 48 teeth respectively. Notice that the larger gear will make only one-half turn while the smaller makes a complete turn. That is, the ratio of speeds (velocity ratio) of the large to the smaller is as 1 to 2.

Figure 2-5 Gears

The gear that is closer to the source of power is called the driver, and the gear that receives power from the driver is called the driven gear.

2.2.1 Gear Trains

A gear train may have several drivers and several driven gears.

Figure 2-6 Gear train

When gear A turns once clockwise, gear B turns 4 times counter-clockwise and gear C turns once clockwise. Hence gear B does not change the speed of C from what it would have been if geared directly to gear A, but it changes its direction from counterclockwise to clockwise.

The velocity ratio of the first and last gears in a train of simple gears dose not changed by putting any number of gears between them.

Figure 2-7 shows compound gears in which two gears are on the middle shaft. Gears B and D rotate at the same speed since they are keyed (fixed) to the same shaft. The number of teeth on each gear is given in the figure. Given these numbers, if gear A rotates at 100 r.p.m. clockwise, gear B turns 400 r.p.m. (rotations per minute) counterclockwise and gear C turns 1200 r.p.m. clockwise.

Figure 2-7 Compound gears

2.2.2 Gear Ratios

It is important when working with gears to know what number of teeth the gears should have so that they can mesh properly in a gear train. The size of the teeth for connecting gears must be match properly.

2.3 Belts and Pulleys

Belts and pulleys are an important part of most machines. Pulleys are nothing but gears without teeth and instead of running together directly they are made to drive one another by cords, ropes, cables, or belting of some kinds.

As with gears, the velocities of pulleys are inversely proportional to their diameters.

Figure 2-8 Belts and pulleys

Pulleys can also be arranged as a block and tackle.

2.4 Lever

2.5 Wheel and Axle

2.6 Wedge

2.7 Efficiency of Machines

In working out the problems on levers, belts and pulleys, inclined planes and so forth, we have not taken account of friction or other sources of energy loss. In other words, we have supposed them to be perfect, when in fact they are not. To measure the performance of a machine, we often find its efficiency, which is defined as

(2-4)

where

= the efficiency of a machine,
Win = the input work to a machine, and
Wout = the output work of a machine.

Table of Contents

   Complete Table of Contents
1 Introduction to Mechanisms
2 Mechanisms and Simple Machines
2.1 The Inclined Plane
2.1.1 Screw Jack
2.2 Gears
2.2.1 Gear Trains
2.2.2 Gear Ratios
2.3 Belts and Pulleys
2.4 Lever
2.5 Lever
2.6 Wedge
2.7 Efficiency of Machines
3 More on Machines and Mechanisms
4 Basic Kinematics of Constrained Rigid Bodies
5 Planar Linkages
6 Cams
7 Gears
8 Other Mechanisms
Index
References


             

sfinger@ri.cmu.edu