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<document xmlns="http://cnx.rice.edu/cnxml" xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:bib="http://bibtexml.sf.net/" id="Module.2004-05-19.2729">
  <name>Simple Machine Elements</name>
  <metadata>
  <md:version>1.1</md:version>
  <md:created>2004/05/19 14:27:29.144 GMT-5</md:created>
  <md:revised>2006/04/25 15:33:16.714 GMT-5</md:revised>
  <md:authorlist>
      <md:author id="young">
      <md:firstname>James</md:firstname>
      <md:othername>F.</md:othername>
      <md:surname>Young</md:surname>
      <md:email>young@rice.edu</md:email>
    </md:author>
  </md:authorlist>

  <md:maintainerlist>
    <md:maintainer id="young">
      <md:firstname>James</md:firstname>
      <md:othername>F.</md:othername>
      <md:surname>Young</md:surname>
      <md:email>young@rice.edu</md:email>
    </md:maintainer>
    <md:maintainer id="ahlfing">
      <md:firstname>Robert</md:firstname>
      
      <md:surname>Ahlfinger</md:surname>
      <md:email>ahlfing@rice.edu</md:email>
    </md:maintainer>
  </md:maintainerlist>
  
  <md:keywordlist>
    <md:keyword>Basic Mechanics</md:keyword>
    <md:keyword>Gears</md:keyword>
    <md:keyword>Inclined Plane</md:keyword>
    <md:keyword>Lever</md:keyword>
    <md:keyword>Screw</md:keyword>
  </md:keywordlist>

  <md:abstract>The simple mechanical elements that comprise complex machines, like robots, are described.</md:abstract>
</metadata>

  <content>

    <!-- intro to simple machines --> 
    <para id="para1">Complex machines are made up of moving parts such
      as levers, gears, cams, cranks, springs, belts, and
      wheels. Machines deliver a certain type of movement to a desired
      location from an input force applied somewhere else. Some
      machines simply convert one type of motion to another type, such as
      rotary to linear.  While there is a seemingly endless variety
      of machines, they are all based upon simple machine elements. The elements
discussed here include inclined planes, levers, wheels and axles,
      pulleys, and screws.</para>

    <para id="para2">It is important to remember that all machines are
      limited in their efficiency by friction. No machine is 100 percent efficient
      in its efforts, so the mechanical advantage gained will require additional
       energy to accomplish the task.  For more information on friction, see this <cnxn document="m11106" strength="7">module</cnxn>
	</para>

    <section id="ip">
      <name>The Inclined Plane</name>

      <para id="para3">An <term>inclined plane</term> decreases the force
	required to raise an object a given height by
	increasing the distance over which that force must be
	applied, see <cnxn target="fig1"/>.  Imagine lifting something twice your weight to a 4
	foot high shelf. Now imagine rolling the same mass up a gently
	sloping surface.  The latter would be much easier. Inclined
	planes are commonly put to use in cutting devices and often
	two inclined planes are put back to back to form a wedge. In a
	wedge, forward movement is converted into a parting movement
	acting perpendicular to the face of the blade. A zipper is simply a combination of two
	lower wedges for closing and an upper wedge for opening, as shown in <cnxn target="fig2"/>.</para>

      <figure id="fig1">
	<media type="image/gif" src="img70.gif"/>
	<caption>Inclined Plane</caption>
      </figure>
      
      <figure id="fig2"> 
	<media type="image/gif" src="img71.gif"/>
	<caption>The Inclined Plane at Work</caption>
      </figure>
    <!-- section for The Screw under inclined plane -->
    <section id="scr">
      <name>The Screw</name>

      <figure id="fig8">
	<media type="image/gif" src="screw.gif"/>
	<caption>The Screw</caption>
      </figure>

      <para id="para15">The <term>screw</term> is basically an
	inclined plane (see <cnxn target="fig8"/>) wrapped around a
	cylinder. In an inclined plane, a linear force in the
	horizontal plane is converted to a vertical "lifting"
	force. With a screw, a rotary force in the horizontal plane is
	converted to a vertical "lifting" force.</para>

      <para id="para16">When a wood screw is turned, the threads of
	the screw push up on the wood. A reaction force from the wood
	pushes back down on the screw threads and in this way the
	screw moves down even though the force of turning the screw is
	in the horizontal plane. Screws are known for high friction,
	which is why they are used to hold things together. A worm gear is sometimes used in machines, but they also have high friction that can waste considerable power. </para>
    </section>
    </section>

    <!-- section for levers under simple machines -->
    <section id="levers">
      <name>Levers</name>

      <para id="para4">A <term>lever</term> has three points of
	interest: the fulcrum, the load, and the effort applied to the lever. The
	<term>fulcrum</term> is the point around which the lever
	pivots rotationally. The <term>load</term> is what we wish to
	manipulate with the lever, and the load is described by its position relative to the fulcrum, and the force (magnitude and direction) it exerts at that point. 
	The <term>effort</term> is also a force that has a magnitude and
	a direction, and a position with respect to the fulcrum. A lever
	is used to change the direction of movement, and to
	trade the magnitude of the effort for the distance over which
	the effort is applied.</para>
      
      <figure id="fig3"> 
	<media type="image/gif" src="levers.gif"/>
	<caption>Classes of Levers</caption>
      </figure>

      <para id="para5">As shown in <cnxn target="fig3"/>, there are
	three different classes of levers defined by the relative
	positions of the fulcrum, effort, and load. A <term>first
	class lever</term> has the fulcrum positioned between the
	effort and the load. Examples of first class levers include: a
	balance, a crow bar, and scissors. In a <term>second class
	lever</term> the load is placed between the fulcrum and the
	effort. Examples of second class levers include: a
	wheelbarrow, a bottle opener, and a nutcracker.  <term>Third
	class levers</term> place the effort between the fulcrum and
	the load. Examples of a third class lever are a hammer, a
	fishing rod, and tweezers. Most machines that employ levers
	use a combination of several levers, often of different
	classes.</para>
    </section>

    <!-- section for The Wheel and Axle under simple machines -->
    <section id="wheelandaxle">
      <name>The Wheel and Axle</name>

      <para id="para6">Both levers and the inclined plane lower the force required for a task at the price of having to apply that force over a longer distance. 
	With wheels and
	axles the same is true: a poweful force and movement of the axle is converted
	to a greater movement, but less force, at the circumference of the wheel. In a circular geometry, <term>torque</term> is a more useful concept than force and distance.  You can learn more about torque <cnxn document="m11106" strength="7">here</cnxn>. The
	<term>wheel and axle</term> can be thought of as simply a
	circular lever, as shown in <cnxn target="fig4"/>. Many common
	items rely on the wheel and axle such as the screwdriver, the
	steering wheel, the wrench, and the faucet.</para>

      <figure id="fig4"> 
	<media type="image/gif" src="img73.gif"/>
	<caption>The Wheel and Axle</caption>
      </figure>
      
      <!-- subsection for Gears and Belts under The Wheel and Axle in
      simple machines -->
      <section id="gearsbelts">
	<name> Gears and Belts</name>
	
	<para id="para7">A wheel and axle assembly becomes especially
	  useful when combined with gears and belts. <term>Gears</term> can be used to change the
	  direction or speed of movement, but changing the speed of
	  rotation inversely affects the force transmitted. A small
	  gear meshed with a larger gear will turn faster, but with
	  less force. There are four basic types of gears: spur gears,
	  rack and pinion gears, bevel gears, and worm gears.
	  <term>Spur gears</term> are probably the type of gear that
	  most people picture when they hear the word. The two wheels
	  are in the same plane (the axles are parallel). With
	  <term>rack and pinion gears</term> there is one wheel and
	  one rack, a flat toothed bar that converts the rotary motion
	  into linear motion.  <term>Bevel gears</term> are also known
	  as pinion and crown or pinion and ring gears. In bevel
	  gears, two wheels intermesh at an angle changing the
	  direction of rotation (the axles are not parallel); the
	  speed and force may also be modified, if desired.
	  <term>Worm gears</term> involve one wheel gear (a pinion)
	  and one shaft with a screw thread wrapped around it. Worm
	  gears change the direction of motion as well as the speed
	  and force.  <term>Belts</term> work in the same manner as
	  spur gears except that they do not change the direction of
	  motion.</para>

	<para id="para8">In both gears and belts, the speed and force is altered
	  by the size of the two interacting
	  wheels. In any pair, the bigger wheel always rotates more
	  slowly, but with more force.  On both the big and the small gear, the linear
	  velocity at the point of contact for the wheels is equal. If
	  it was unequal and one gear were spinning faster than the
	  other at the point of contact then it would rip the teeth
	  right off of the other gear. As the circumference of the
	  larger gear is greater, a point on the outside of the larger
	  gear must cover a greater distance than a point on the
	  smaller gear to complete a revolution. Therefore the smaller
	  gear must complete more revolutions than the larger gear in
	  the same time span. (It's rotating more quickly.) </para> 

	<para id="para8a">The force
	  applied to the outer surface of each wheel must also be
	  equal otherwise one of them would be accelerating more
	  rapidly than the other, and again the teeth of the other
	  wheel would break. However, the forces 
	  the forces applied to 
	  the axles are not equal. Returning to the
	  concept of levers, we know that the distance from the fulcrum at which the
	  force is applied effects the force applied at another point, and a wheel and
	  axle works like a lever. Equal forces are being applied to
	  each wheel, but on the larger wheel that force is being
	  applied at a greater distance from the axle. Thus, for the larger wheel,
	  the force on the axle is greater than the force on the axle
	  of the smaller wheel.</para>
      </section>
    </section>

    <!-- section for Cams and Cranks under simple machines -->
    <section id="cac">
      <name>Cams and Cranks </name>

      <para id="para9">Both cams and cranks are useful when a
	repetitive motion is desired. <term>Cams</term> make rotary
	motion a little more interesting by essentially moving the
	axle off-center. Cams are often used in conjunction with a
	rod. One end of the rod is held flush against the cam by a
	spring. As the cam rotates the rod remains stationary until
	the "bump" of the cam pushes the rod away from the cam's
	axle.  Cams can be used to
	create either a linear repetitive motion such as the one
	illustrated in <cnxn target="fig5"/>, or a repetitive
	rotational motion such as <cnxn document="m" target="use_rubberband2.gif">using a cam and a rubber
	band</cnxn>.</para>

      <figure id="fig5">
	<media type="image/gif" src="img74.gif"/>
	<caption>Cams and Cranks</caption>
      </figure>

      <para id="para10"><term>Cranks</term> convert rotary motion into
	a piston-like linear motion. The best examples of cranks in
	action are the drive mechanism for a steam locomotive and the
	automobile engine crankshaft. In a crank, the wheel rotates
	about a centered axle, while an arm is attached to the wheel
	with an off-centered peg. This arm is attached to a rod fixed
	in a linear path. A crank will cause the rod to move back and
	forth.  If instead the rod is pushed back and forth, it will cause
	the crank to turn. On the other hand, cams can move their
	rods, but rods cannot move the cams. </para>

    </section>
    <!-- section for Pulleys under simple machines -->
    <section id="pull">
      <name>Pulleys </name>

      <figure id="fig6">
	<media type="image/gif" src="pulley.gif"/>
	<caption>Pulleys</caption>
      </figure>

      <para id="para11"><term>Pulleys</term> can be used to simply
	change the direction of an applied force or to provide a
	force/distance tradeoff in addition to a directional change,
	as shown in <cnxn target="fig6"/>. Pulleys are very flexible
	because they use ropes or chain to transfer force rather than a rigid
	object such as a rod. Ropes can be routed through
	virtually any path. They are able to abruptly change
	directions in three-dimensions without consequence, except, of 
course, additional friction. Ropes can
	be wrapped around a motor's shaft and either wound up or let
	out as the motor turns.</para>

      <figure id="fig7">
	<media type="image/gif" src="compound_pulley.gif"/>
	<caption>How Compound Pulleys Work</caption>
      </figure>
     
      <para id="para13"> <cnxn target="fig7"/> illustrates how a
	compound pulley 'trades' force for distance through an
	action/reaction force pair. In a double pulley, as the rope
	passes over the pulley the force is transmitted entirely but
	the direction has changed. The effort is now pulling up on the
	left side of the bottom pulley. Now, for a moment forget that
	the end of the rope is tied to the bottom of the top
	pulley. The mechanics are the same if the rope is fixed to the
	ceiling. The important thing is that the end of the rope is
	immobile. The effort is once again transmitted entirely as the
	rope passes over the bottom pulley and there is a direction
	change. The end of the rope is attached to the ceiling so the
	rope is pulling down on the ceiling with the force of the
	effort (and half of the force of the load). We assume that the
	ceiling holds up, so this must mean that there is a force
	balancing out this downward force. The ceiling pulls up on the
	rope as a reaction force. This upward force is equal to the
	effort and now there is an upward force on the right side of
	the bottom pulley. From the perspective of a free-body diagram
	the compound pulley system could be replaced by tying two
	ropes to the load and pulling up on each with a force equal to
	the effort.</para>

      <para id="para14">The disadvantages of pulleys, in contrast to
	machines that use rigid objects to transfer force, are
	slipping and stretching. A rope will permanently stretch under
	tension, which may affect the future performance of a
	device. If a line becomes slack, then the operation of a
	machine may change entirely. Also, ropes will slip and stick
	along pulley wheels just like belts. One solution to the
	problems associated with rope is to use chain. Chain is
	pliable like rope, and is able to transfer force through many
	direction changes, but the chain links are inflexible in
	tension, so that the chain will not stretch. Chains may also
	be made to fit on gears so that slipping is avoided.
      </para>
    </section>

  </content>
	  
</document>
