{"id":461,"date":"2020-04-19T15:59:31","date_gmt":"2020-04-19T19:59:31","guid":{"rendered":"https:\/\/pressbooks.bccampus.ca\/humanbiomechanics\/chapter\/9-5-simple-machines-2\/"},"modified":"2020-09-03T14:38:59","modified_gmt":"2020-09-03T18:38:59","slug":"9-5-simple-machines-2","status":"publish","type":"chapter","link":"https:\/\/pressbooks.bccampus.ca\/humanbiomechanics\/chapter\/9-5-simple-machines-2\/","title":{"raw":"8.5 Mechanical Advantage","rendered":"8.5 Mechanical Advantage"},"content":{"raw":"<div>\r\n<div class=\"bcc-box bcc-highlight\">\r\n<h3>Summary<\/h3>\r\n<div>\r\n<ul>\r\n \t<li>Calculate the mechanical advantage.<\/li>\r\n<\/ul>\r\n<\/div>\r\n<\/div>\r\n<\/div>\r\n<p id=\"import-auto-id1426082\">Simple machines are devices that can be used to multiply or augment a force that we apply \u2013 often at the expense of a distance through which we apply the force. The human body can be compared to simple machines depending on muscle attachment and weight of the limb. The word for \u201cmachine\u201d comes from the Greek word meaning \u201cto help make things easier.\u201d Levers, gears, pulleys, wedges, and screws are some examples of machines. The ratio of output to input force magnitudes for any simple machine is called its <strong>mechanical advantage<\/strong> (MA).<\/p>\r\n\r\n<div class=\"equation\" style=\"text-align: center\">\u00a0 MA = (F <sub>output<\/sub>) \/ ( F <sub>input<\/sub> )<\/div>\r\n<p id=\"import-auto-id2973037\">One of the simplest machines is the lever, which is a rigid bar pivoted at a fixed place called the fulcrum. Torques are involved in levers, since there is rotation about a pivot point. Distances from the physical pivot of the lever are crucial, and we can obtain a useful expression for the MA in terms of these distances.<\/p>\r\n\r\n<figure id=\"import-auto-id2670210\">\r\n\r\n[caption id=\"\" align=\"aligncenter\" width=\"250\"]<img src=\"https:\/\/pressbooks.bccampus.ca\/humanbiomechanics\/wp-content\/uploads\/sites\/972\/2020\/04\/Figure_10_05_01a-1-1.jpg\" alt=\"There is a nail in a wooden plank. A nail puller is being used to pull the nail out of the plank. A hand is applying force F sub I downward on the handle of the nail puller. The top of the nail exerts a force F sub N downward on the puller. At the point where the nail puller touches the plank, the reaction of the surface force N is applied. At the top of the figure, a free body diagram is shown.\" width=\"250\" height=\"670\" \/> <strong>Figure 1.<\/strong> A nail puller is a lever with a large mechanical advantage. The external forces on the nail puller are represented by solid arrows. The force that the nail puller applies to the nail (<strong>F<sub>o<\/sub><\/strong>) is not a force on the nail puller. The reaction force the nail exerts back on the puller (<strong>F<sub>n<\/sub><\/strong>) is an external force and is equal and opposite to <strong>F<sub>o<\/sub><\/strong>. The perpendicular lever arms of the input and output forces are<strong><em> l<\/em><sub>i<\/sub><\/strong> and<strong><em> l<\/em><sub>0<\/sub><\/strong>.[\/caption]<\/figure>\r\n<a class=\"autogenerated-content\" href=\"#import-auto-id2670210\">Figure 1<\/a> shows a lever type that is used as a nail puller. Crowbars, seesaws, and other such levers are all analogous to this one. [latex]\\boldsymbol{\\vec{\\textbf{F}}_{\\textbf{i}}}[\/latex] is the input force and [latex]\\boldsymbol{\\vec{\\textbf{F}}_{\\textbf{o}}}[\/latex] is the output force. There are three vertical forces acting on the nail puller (the system of interest) \u2013 these are [latex]\\boldsymbol{\\vec{\\textbf{F}}_{\\textbf{i}},\\: \\vec{\\textbf{F}}_{\\textbf{o}}}[\/latex] and [latex]\\vec{\\textbf{N}}.[\/latex] [latex]\\boldsymbol{\\vec{\\textbf{F}}_{\\textbf{n}}}[\/latex] is the reaction force back on the system, equal and opposite to [latex]\\boldsymbol{\\vec{\\textbf{F}}_{\\textbf{o}}}.[\/latex] (Note that [latex]\\boldsymbol{\\vec{\\textbf{F}}_{\\textbf{o}}}[\/latex] is not a force on the system.) [latex]\\vec{\\textbf{N}}[\/latex] is the normal force upon the lever, and its torque is zero since it is exerted at the pivot. The torques due to [latex]\\boldsymbol{\\vec{\\textbf{F}}_{\\textbf{i}}}[\/latex] and [latex]\\boldsymbol{\\vec{\\textbf{F}}_{\\textbf{n}}}[\/latex] must be equal to each other if the nail is not moving, to satisfy the second condition for equilibrium (<strong>net \u03c4 = 0<\/strong>). (In order for the nail to actually move, the torque due to [latex]\\boldsymbol{\\vec{\\textbf{F}}_{\\textbf{i}}}[\/latex] must be ever-so-slightly greater than torque due to [latex]\\boldsymbol{\\vec{\\textbf{F}}_{\\textbf{n}}}[\/latex].) Hence,\r\n<div id=\"eip-158\" class=\"equation\" style=\"text-align: center\">[latex]\\boldsymbol{l_{\\textbf{i}}F_{\\textbf{i}}=l_{\\textbf{o}}F_{\\textbf{o}}}[\/latex]<\/div>\r\n<p id=\"import-auto-id3592966\">where <strong><em>l<\/em><sub>i<\/sub><\/strong> and <strong><em>l<\/em><sub>o<\/sub><\/strong> are the distances from where the input and output forces are applied to the pivot, as shown in the figure. Rearranging the last equation gives<\/p>\r\n\r\n<div class=\"equation\" style=\"text-align: center\">[latex]\\boldsymbol{\\frac{F_{\\textbf{o}}}{F_{\\textbf{i}}}}\\boldsymbol{=}\\boldsymbol{\\frac{l_{\\textbf{i}}}{l_{\\textbf{o}}}}.[\/latex]<\/div>\r\n<p id=\"import-auto-id1451106\">What interests us most here is that the magnitude of the force exerted by the nail puller, <strong><em>F<\/em><sub>o<\/sub><\/strong>, is much greater than the magnitude of the input force applied to the puller at the other end, <strong><em>F<\/em><sub>i<\/sub><\/strong>. For the nail puller,<\/p>\r\n\r\n<div class=\"equation\" style=\"text-align: center\">[latex]\\boldsymbol{\\textbf{MA}\\:=}\\boldsymbol{\\frac{F_{\\textbf{o}}}{F_{\\textbf{i}}}}\\boldsymbol{=}\\boldsymbol{\\frac{l_{\\textbf{i}}}{l_{\\textbf{o}}}}.[\/latex]<\/div>\r\n<p id=\"import-auto-id1201292\">This equation is true for levers in general. For the nail puller, the MA is certainly greater than one. The longer the handle on the nail puller, the greater the force you can exert with it.<\/p>\r\n<p id=\"import-auto-id2575661\">Two other types of levers that differ slightly from the nail puller are a wheelbarrow and a shovel, shown in <a class=\"autogenerated-content\" href=\"#import-auto-id2664028\">Figure 2<\/a>. All these lever types are similar in that only three forces are involved \u2013 the input force, the output force, and the force on the pivot \u2013 and thus their MAs are given by [latex]\\boldsymbol{\\textbf{MA}=\\frac{F_{\\textbf{o}}}{F_{\\textbf{i}}}}[\/latex] and [latex]\\boldsymbol{\\textbf{MA}=\\frac{d_1}{d_2}},[\/latex] with distances being measured relative to the physical pivot. The wheelbarrow and shovel differ from the nail puller because both the input and output forces are on the same side of the pivot.<\/p>\r\n<p id=\"import-auto-id2596612\">In the case of the wheelbarrow, the output force or load is between the pivot (the wheel\u2019s axle) and the input or applied force. In the case of the shovel, the input force is between the pivot (at the end of the handle) and the load, but the input lever arm is shorter than the output lever arm. In this case, the MA is less than one.<\/p>\r\n\r\n<figure id=\"import-auto-id2664028\">\r\n\r\n[caption id=\"\" align=\"aligncenter\" width=\"359\"]<img class=\"\" src=\"https:\/\/pressbooks.bccampus.ca\/humanbiomechanics\/wp-content\/uploads\/sites\/972\/2020\/04\/Figure_10_05_02a-1-1.jpg\" alt=\"A wheelbarrow is shown in which the input force F sub I is shown as a vector in vertically upward direction below the handle of wheelbarrow. The weight of the wheelbarrow is downward at the center of gravity. The normal reaction of the ground is acting at the wheel in upward direction. The perpendicular distance between the normal reaction and the input force F sub I is labeled as R sub I and the distance between output force F sub O and normal reaction is labeled as R sub O. In figure b, a man is holding a shovel in his hands. One hand is at one end of the handle and the other hand is holding the shovel at the middle. The center of gravity of the shovel is at its flat end. The weight of the shovel is acting at the center of gravity. The input force is acting at the hand in the middle in upward direction and the end of the shovel is acting as pivot. A free body diagram is also shown at the right side of the figure.\" width=\"359\" height=\"503\" \/> <strong>Figure 2.<\/strong> (a) In the case of the wheelbarrow, the output force or load is between the pivot and the input force. The pivot is the wheel\u2019s axle. Here, the output force is greater than the input force. Thus, a wheelbarrow enables you to lift much heavier loads than you could with your body alone. (b) In the case of the shovel, the input force is between the pivot and the load, but the input lever arm is shorter than the output lever arm. The pivot is at the handle held by the right hand. Here, the output force (supporting the shovel\u2019s load) is less than the input force (from the hand nearest the load), because the input is exerted closer to the pivot than is the output.[\/caption]<\/figure>\r\n<div class=\"textbox shaded\">\r\n<div id=\"fs-id3597397\" class=\"example\">\r\n<h3 id=\"import-auto-id1286140\">Example 1: What is the Advantage for the Wheelbarrow?<\/h3>\r\nIn the wheelbarrow of <a class=\"autogenerated-content\" href=\"#import-auto-id2664028\">Figure 2<\/a>, the load has a perpendicular lever arm of 7.50 cm, while the hands have a perpendicular lever arm of 1.02 m. (a) What upward force must you exert to support the wheelbarrow and its load if their combined mass is 45.0 kg? (b) What force does the wheelbarrow exert on the ground?\r\n<p id=\"import-auto-id2583956\"><strong>Strategy<\/strong><\/p>\r\n<p id=\"fs-id2877509\">Here, we use the concept of mechanical advantage.<\/p>\r\n<p id=\"import-auto-id3048099\"><strong>Solution<\/strong><\/p>\r\n<p id=\"fs-id1394216\">(a) In this case, [latex]\\boldsymbol{\\frac{F_{\\textbf{o}}}{F_{\\textbf{i}}}=\\frac{l_{\\textbf{i}}}{l_{\\textbf{o}}}}[\/latex] becomes<\/p>\r\n\r\n<div id=\"eip-501\" class=\"equation\" style=\"text-align: center\">[latex]\\boldsymbol{F_{\\textbf{i}}=F_{\\textbf{o}}}\\boldsymbol{\\frac{l_{\\textbf{o}}}{l_{\\textbf{i}}}}.[\/latex]<\/div>\r\n<p id=\"import-auto-id2702678\">Adding values into this equation yields<\/p>\r\n\r\n<div id=\"eip-453\" class=\"equation\" style=\"text-align: center\">[latex]\\boldsymbol{F_{\\textbf{i}}=(45.0\\textbf{ kg})(9.80\\textbf{ m\/s}^2)}\\boldsymbol{\\frac{0.075\\textbf{ m}}{1.02\\textbf{ m}}}\\boldsymbol{=\\:32.4\\textbf{ N}}.[\/latex]<\/div>\r\nThe free-body diagram (see <a class=\"autogenerated-content\" href=\"#import-auto-id2664028\">Figure 2<\/a>) gives the following normal force: <strong><em>F<\/em><sub>i<\/sub> + <em>N <\/em>= <em>W<\/em><\/strong>. Therefore, <strong><em>N<\/em> = (45.0 kg)(9.80 m\/s<sup>2<\/sup>) -32.4 N = 409 N<\/strong>. <em><strong>N<\/strong><\/em> is the normal force acting on the wheel; by Newton\u2019s third law, the force the wheel exerts on the ground is <strong>409 N<\/strong>.\r\n<p id=\"import-auto-id1254753\"><strong>Discussion<\/strong><\/p>\r\n<p id=\"fs-id720675\">An even longer handle would reduce the force needed to lift the load. The MA here is <strong>MA=1.02\/0.0750=13.6<\/strong>.<\/p>\r\n\r\n<\/div>\r\n<\/div>\r\n<p id=\"import-auto-id1323114\">Another very simple machine is the inclined plane. Pushing a cart up a plane is easier than lifting the same cart straight up to the top using a ladder, because the applied force is less. However, the work done in both cases (assuming the work done by friction is negligible) is the same.<\/p>\r\nA crank is a lever that can be rotated <strong>360\u00b0<\/strong> about its pivot, as shown in <a class=\"autogenerated-content\" href=\"#import-auto-id2741043\">Figure 3<\/a>. Such a machine may not look like a lever, but the physics of its actions remain the same. The MA for a crank is simply the ratio of the radii <strong><em>r<\/em><sub>i<\/sub>\/<em>r<\/em><sub>0<\/sub><\/strong>. Wheels and gears have this simple expression for their MAs too. The MA can be greater than 1, as it is for the crank, or less than 1, as it is for the simplified car axle driving the wheels, as shown. If the axle\u2019s radius is <strong>2.0 cm<\/strong> and the wheel\u2019s radius is <strong>24.0 cm<\/strong>, then <strong>MA=2.0\/24.0=0.083<\/strong> and the axle would have to exert a force of<strong> 12,000 N<\/strong> on the wheel to enable it to exert a force of <strong>1000 N<\/strong> on the ground.\r\n<figure id=\"import-auto-id2741043\">\r\n\r\n[caption id=\"\" align=\"aligncenter\" width=\"200\"]<img src=\"https:\/\/pressbooks.bccampus.ca\/humanbiomechanics\/wp-content\/uploads\/sites\/972\/2020\/04\/Figure_10_05_03-1-1.jpg\" alt=\"In figure a, a crank lever is shown in which a hand is at the handle of the crank lever. The output force F sub O is at the base of the lever and the input force F sub I is at the handle of the lever. The distance between input force and output force is labeled as R sub I. In figure b, a simplified axle of the car is shown. The input force is shown as a vector F sub I on the axle toward right. The output force is shown at the point of contact of the wheel with the ground toward left. The distance between the output force and the pivot point is labeled as R sub O. In figure c, rope over the pulley is shown. The input force is shown as a downward arrow at the left part of rope. The output force is acting on the right part of the rope. The center of the pulley is the pivot point. The distances of the two forces from the pivot are R sub I and R sub O respectively.\" width=\"200\" height=\"1150\" \/> <strong>Figure 3.<\/strong> (a) A crank is a type of lever that can be rotated<strong> 360\u00ba<\/strong> about its pivot. Cranks are usually designed to have a large MA. (b) A simplified automobile axle drives a wheel, which has a much larger diameter than the axle. The MA is less than 1. (c) An ordinary pulley is used to lift a heavy load. The pulley changes the direction of the force <em><strong>T<\/strong><\/em> exerted by the cord without changing its magnitude. Hence, this machine has an MA of 1.[\/caption]<\/figure>\r\n<section id=\"fs-id2588505\" class=\"section-summary\">\r\n<h1>Section Summary<\/h1>\r\n<ul id=\"fs-id1167981\">\r\n \t<li id=\"import-auto-id1238080\">Simple machines are devices that can be used to multiply or augment a force that we apply \u2013 often at the expense of a distance through which we have to apply the force.<\/li>\r\n \t<li id=\"import-auto-id2697990\">The ratio of output to input forces for any simple machine is called its mechanical advantage<\/li>\r\n \t<li id=\"import-auto-id1279635\">A few simple machines are the lever, nail puller, wheelbarrow, crank, etc.<\/li>\r\n<\/ul>\r\n<\/section><section id=\"fs-id3028918\" class=\"conceptual-questions\">\r\n<div class=\"bcc-box bcc-info\">\r\n<h3>Conceptual Questions<\/h3>\r\n<div id=\"fs-id2730066\" class=\"exercise\">\r\n<div id=\"fs-id2696305\" class=\"problem\">\r\n\r\n<strong>1: <\/strong>Why are the forces exerted on the outside world by the limbs of our bodies usually much smaller than the forces exerted by muscles inside the body?\r\n\r\n<\/div>\r\n<\/div>\r\n<div id=\"fs-id1428982\" class=\"exercise\">\r\n<div id=\"fs-id1398239\" class=\"problem\">\r\n<p id=\"import-auto-id2738965\"><strong>2: <\/strong>Explain why the forces in our joints are several times larger than the forces we exert on the outside world with our limbs. Can these forces be even greater than muscle forces (see previous Question)?<\/p>\r\n\r\n<\/div>\r\n<\/div>\r\n<\/div>\r\n<\/section>\r\n<div>\r\n<h2>Glossary<\/h2>\r\n<dl id=\"import-auto-id3034634\" class=\"definition\">\r\n \t<dt>mechanical advantage<\/dt>\r\n \t<dd id=\"fs-id1370336\">the ratio of output to input forces for any simple machine<\/dd>\r\n<\/dl>\r\n<\/div>","rendered":"<div>\n<div class=\"bcc-box bcc-highlight\">\n<h3>Summary<\/h3>\n<div>\n<ul>\n<li>Calculate the mechanical advantage.<\/li>\n<\/ul>\n<\/div>\n<\/div>\n<\/div>\n<p id=\"import-auto-id1426082\">Simple machines are devices that can be used to multiply or augment a force that we apply \u2013 often at the expense of a distance through which we apply the force. The human body can be compared to simple machines depending on muscle attachment and weight of the limb. The word for \u201cmachine\u201d comes from the Greek word meaning \u201cto help make things easier.\u201d Levers, gears, pulleys, wedges, and screws are some examples of machines. The ratio of output to input force magnitudes for any simple machine is called its <strong>mechanical advantage<\/strong> (MA).<\/p>\n<div class=\"equation\" style=\"text-align: center\">\u00a0 MA = (F <sub>output<\/sub>) \/ ( F <sub>input<\/sub> )<\/div>\n<p id=\"import-auto-id2973037\">One of the simplest machines is the lever, which is a rigid bar pivoted at a fixed place called the fulcrum. Torques are involved in levers, since there is rotation about a pivot point. Distances from the physical pivot of the lever are crucial, and we can obtain a useful expression for the MA in terms of these distances.<\/p>\n<figure id=\"import-auto-id2670210\">\n<figure style=\"width: 250px\" class=\"wp-caption aligncenter\"><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/pressbooks.bccampus.ca\/humanbiomechanics\/wp-content\/uploads\/sites\/972\/2020\/04\/Figure_10_05_01a-1-1.jpg\" alt=\"There is a nail in a wooden plank. A nail puller is being used to pull the nail out of the plank. A hand is applying force F sub I downward on the handle of the nail puller. The top of the nail exerts a force F sub N downward on the puller. At the point where the nail puller touches the plank, the reaction of the surface force N is applied. At the top of the figure, a free body diagram is shown.\" width=\"250\" height=\"670\" \/><figcaption class=\"wp-caption-text\"><strong>Figure 1.<\/strong> A nail puller is a lever with a large mechanical advantage. The external forces on the nail puller are represented by solid arrows. The force that the nail puller applies to the nail (<strong>F<sub>o<\/sub><\/strong>) is not a force on the nail puller. The reaction force the nail exerts back on the puller (<strong>F<sub>n<\/sub><\/strong>) is an external force and is equal and opposite to <strong>F<sub>o<\/sub><\/strong>. The perpendicular lever arms of the input and output forces are<strong><em> l<\/em><sub>i<\/sub><\/strong> and<strong><em> l<\/em><sub>0<\/sub><\/strong>.<\/figcaption><\/figure>\n<\/figure>\n<p><a class=\"autogenerated-content\" href=\"#import-auto-id2670210\">Figure 1<\/a> shows a lever type that is used as a nail puller. Crowbars, seesaws, and other such levers are all analogous to this one. [latex]\\boldsymbol{\\vec{\\textbf{F}}_{\\textbf{i}}}[\/latex] is the input force and [latex]\\boldsymbol{\\vec{\\textbf{F}}_{\\textbf{o}}}[\/latex] is the output force. There are three vertical forces acting on the nail puller (the system of interest) \u2013 these are [latex]\\boldsymbol{\\vec{\\textbf{F}}_{\\textbf{i}},\\: \\vec{\\textbf{F}}_{\\textbf{o}}}[\/latex] and [latex]\\vec{\\textbf{N}}.[\/latex] [latex]\\boldsymbol{\\vec{\\textbf{F}}_{\\textbf{n}}}[\/latex] is the reaction force back on the system, equal and opposite to [latex]\\boldsymbol{\\vec{\\textbf{F}}_{\\textbf{o}}}.[\/latex] (Note that [latex]\\boldsymbol{\\vec{\\textbf{F}}_{\\textbf{o}}}[\/latex] is not a force on the system.) [latex]\\vec{\\textbf{N}}[\/latex] is the normal force upon the lever, and its torque is zero since it is exerted at the pivot. The torques due to [latex]\\boldsymbol{\\vec{\\textbf{F}}_{\\textbf{i}}}[\/latex] and [latex]\\boldsymbol{\\vec{\\textbf{F}}_{\\textbf{n}}}[\/latex] must be equal to each other if the nail is not moving, to satisfy the second condition for equilibrium (<strong>net \u03c4 = 0<\/strong>). (In order for the nail to actually move, the torque due to [latex]\\boldsymbol{\\vec{\\textbf{F}}_{\\textbf{i}}}[\/latex] must be ever-so-slightly greater than torque due to [latex]\\boldsymbol{\\vec{\\textbf{F}}_{\\textbf{n}}}[\/latex].) Hence,<\/p>\n<div id=\"eip-158\" class=\"equation\" style=\"text-align: center\">[latex]\\boldsymbol{l_{\\textbf{i}}F_{\\textbf{i}}=l_{\\textbf{o}}F_{\\textbf{o}}}[\/latex]<\/div>\n<p id=\"import-auto-id3592966\">where <strong><em>l<\/em><sub>i<\/sub><\/strong> and <strong><em>l<\/em><sub>o<\/sub><\/strong> are the distances from where the input and output forces are applied to the pivot, as shown in the figure. Rearranging the last equation gives<\/p>\n<div class=\"equation\" style=\"text-align: center\">[latex]\\boldsymbol{\\frac{F_{\\textbf{o}}}{F_{\\textbf{i}}}}\\boldsymbol{=}\\boldsymbol{\\frac{l_{\\textbf{i}}}{l_{\\textbf{o}}}}.[\/latex]<\/div>\n<p id=\"import-auto-id1451106\">What interests us most here is that the magnitude of the force exerted by the nail puller, <strong><em>F<\/em><sub>o<\/sub><\/strong>, is much greater than the magnitude of the input force applied to the puller at the other end, <strong><em>F<\/em><sub>i<\/sub><\/strong>. For the nail puller,<\/p>\n<div class=\"equation\" style=\"text-align: center\">[latex]\\boldsymbol{\\textbf{MA}\\:=}\\boldsymbol{\\frac{F_{\\textbf{o}}}{F_{\\textbf{i}}}}\\boldsymbol{=}\\boldsymbol{\\frac{l_{\\textbf{i}}}{l_{\\textbf{o}}}}.[\/latex]<\/div>\n<p id=\"import-auto-id1201292\">This equation is true for levers in general. For the nail puller, the MA is certainly greater than one. The longer the handle on the nail puller, the greater the force you can exert with it.<\/p>\n<p id=\"import-auto-id2575661\">Two other types of levers that differ slightly from the nail puller are a wheelbarrow and a shovel, shown in <a class=\"autogenerated-content\" href=\"#import-auto-id2664028\">Figure 2<\/a>. All these lever types are similar in that only three forces are involved \u2013 the input force, the output force, and the force on the pivot \u2013 and thus their MAs are given by [latex]\\boldsymbol{\\textbf{MA}=\\frac{F_{\\textbf{o}}}{F_{\\textbf{i}}}}[\/latex] and [latex]\\boldsymbol{\\textbf{MA}=\\frac{d_1}{d_2}},[\/latex] with distances being measured relative to the physical pivot. The wheelbarrow and shovel differ from the nail puller because both the input and output forces are on the same side of the pivot.<\/p>\n<p id=\"import-auto-id2596612\">In the case of the wheelbarrow, the output force or load is between the pivot (the wheel\u2019s axle) and the input or applied force. In the case of the shovel, the input force is between the pivot (at the end of the handle) and the load, but the input lever arm is shorter than the output lever arm. In this case, the MA is less than one.<\/p>\n<figure id=\"import-auto-id2664028\">\n<figure style=\"width: 359px\" class=\"wp-caption aligncenter\"><img loading=\"lazy\" decoding=\"async\" class=\"\" src=\"https:\/\/pressbooks.bccampus.ca\/humanbiomechanics\/wp-content\/uploads\/sites\/972\/2020\/04\/Figure_10_05_02a-1-1.jpg\" alt=\"A wheelbarrow is shown in which the input force F sub I is shown as a vector in vertically upward direction below the handle of wheelbarrow. The weight of the wheelbarrow is downward at the center of gravity. The normal reaction of the ground is acting at the wheel in upward direction. The perpendicular distance between the normal reaction and the input force F sub I is labeled as R sub I and the distance between output force F sub O and normal reaction is labeled as R sub O. In figure b, a man is holding a shovel in his hands. One hand is at one end of the handle and the other hand is holding the shovel at the middle. The center of gravity of the shovel is at its flat end. The weight of the shovel is acting at the center of gravity. The input force is acting at the hand in the middle in upward direction and the end of the shovel is acting as pivot. A free body diagram is also shown at the right side of the figure.\" width=\"359\" height=\"503\" \/><figcaption class=\"wp-caption-text\"><strong>Figure 2.<\/strong> (a) In the case of the wheelbarrow, the output force or load is between the pivot and the input force. The pivot is the wheel\u2019s axle. Here, the output force is greater than the input force. Thus, a wheelbarrow enables you to lift much heavier loads than you could with your body alone. (b) In the case of the shovel, the input force is between the pivot and the load, but the input lever arm is shorter than the output lever arm. The pivot is at the handle held by the right hand. Here, the output force (supporting the shovel\u2019s load) is less than the input force (from the hand nearest the load), because the input is exerted closer to the pivot than is the output.<\/figcaption><\/figure>\n<\/figure>\n<div class=\"textbox shaded\">\n<div id=\"fs-id3597397\" class=\"example\">\n<h3 id=\"import-auto-id1286140\">Example 1: What is the Advantage for the Wheelbarrow?<\/h3>\n<p>In the wheelbarrow of <a class=\"autogenerated-content\" href=\"#import-auto-id2664028\">Figure 2<\/a>, the load has a perpendicular lever arm of 7.50 cm, while the hands have a perpendicular lever arm of 1.02 m. (a) What upward force must you exert to support the wheelbarrow and its load if their combined mass is 45.0 kg? (b) What force does the wheelbarrow exert on the ground?<\/p>\n<p id=\"import-auto-id2583956\"><strong>Strategy<\/strong><\/p>\n<p id=\"fs-id2877509\">Here, we use the concept of mechanical advantage.<\/p>\n<p id=\"import-auto-id3048099\"><strong>Solution<\/strong><\/p>\n<p id=\"fs-id1394216\">(a) In this case, [latex]\\boldsymbol{\\frac{F_{\\textbf{o}}}{F_{\\textbf{i}}}=\\frac{l_{\\textbf{i}}}{l_{\\textbf{o}}}}[\/latex] becomes<\/p>\n<div id=\"eip-501\" class=\"equation\" style=\"text-align: center\">[latex]\\boldsymbol{F_{\\textbf{i}}=F_{\\textbf{o}}}\\boldsymbol{\\frac{l_{\\textbf{o}}}{l_{\\textbf{i}}}}.[\/latex]<\/div>\n<p id=\"import-auto-id2702678\">Adding values into this equation yields<\/p>\n<div id=\"eip-453\" class=\"equation\" style=\"text-align: center\">[latex]\\boldsymbol{F_{\\textbf{i}}=(45.0\\textbf{ kg})(9.80\\textbf{ m\/s}^2)}\\boldsymbol{\\frac{0.075\\textbf{ m}}{1.02\\textbf{ m}}}\\boldsymbol{=\\:32.4\\textbf{ N}}.[\/latex]<\/div>\n<p>The free-body diagram (see <a class=\"autogenerated-content\" href=\"#import-auto-id2664028\">Figure 2<\/a>) gives the following normal force: <strong><em>F<\/em><sub>i<\/sub> + <em>N <\/em>= <em>W<\/em><\/strong>. Therefore, <strong><em>N<\/em> = (45.0 kg)(9.80 m\/s<sup>2<\/sup>) -32.4 N = 409 N<\/strong>. <em><strong>N<\/strong><\/em> is the normal force acting on the wheel; by Newton\u2019s third law, the force the wheel exerts on the ground is <strong>409 N<\/strong>.<\/p>\n<p id=\"import-auto-id1254753\"><strong>Discussion<\/strong><\/p>\n<p id=\"fs-id720675\">An even longer handle would reduce the force needed to lift the load. The MA here is <strong>MA=1.02\/0.0750=13.6<\/strong>.<\/p>\n<\/div>\n<\/div>\n<p id=\"import-auto-id1323114\">Another very simple machine is the inclined plane. Pushing a cart up a plane is easier than lifting the same cart straight up to the top using a ladder, because the applied force is less. However, the work done in both cases (assuming the work done by friction is negligible) is the same.<\/p>\n<p>A crank is a lever that can be rotated <strong>360\u00b0<\/strong> about its pivot, as shown in <a class=\"autogenerated-content\" href=\"#import-auto-id2741043\">Figure 3<\/a>. Such a machine may not look like a lever, but the physics of its actions remain the same. The MA for a crank is simply the ratio of the radii <strong><em>r<\/em><sub>i<\/sub>\/<em>r<\/em><sub>0<\/sub><\/strong>. Wheels and gears have this simple expression for their MAs too. The MA can be greater than 1, as it is for the crank, or less than 1, as it is for the simplified car axle driving the wheels, as shown. If the axle\u2019s radius is <strong>2.0 cm<\/strong> and the wheel\u2019s radius is <strong>24.0 cm<\/strong>, then <strong>MA=2.0\/24.0=0.083<\/strong> and the axle would have to exert a force of<strong> 12,000 N<\/strong> on the wheel to enable it to exert a force of <strong>1000 N<\/strong> on the ground.<\/p>\n<figure id=\"import-auto-id2741043\">\n<figure style=\"width: 200px\" class=\"wp-caption aligncenter\"><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/pressbooks.bccampus.ca\/humanbiomechanics\/wp-content\/uploads\/sites\/972\/2020\/04\/Figure_10_05_03-1-1.jpg\" alt=\"In figure a, a crank lever is shown in which a hand is at the handle of the crank lever. The output force F sub O is at the base of the lever and the input force F sub I is at the handle of the lever. The distance between input force and output force is labeled as R sub I. In figure b, a simplified axle of the car is shown. The input force is shown as a vector F sub I on the axle toward right. The output force is shown at the point of contact of the wheel with the ground toward left. The distance between the output force and the pivot point is labeled as R sub O. In figure c, rope over the pulley is shown. The input force is shown as a downward arrow at the left part of rope. The output force is acting on the right part of the rope. The center of the pulley is the pivot point. The distances of the two forces from the pivot are R sub I and R sub O respectively.\" width=\"200\" height=\"1150\" \/><figcaption class=\"wp-caption-text\"><strong>Figure 3.<\/strong> (a) A crank is a type of lever that can be rotated<strong> 360\u00ba<\/strong> about its pivot. Cranks are usually designed to have a large MA. (b) A simplified automobile axle drives a wheel, which has a much larger diameter than the axle. The MA is less than 1. (c) An ordinary pulley is used to lift a heavy load. The pulley changes the direction of the force <em><strong>T<\/strong><\/em> exerted by the cord without changing its magnitude. Hence, this machine has an MA of 1.<\/figcaption><\/figure>\n<\/figure>\n<section id=\"fs-id2588505\" class=\"section-summary\">\n<h1>Section Summary<\/h1>\n<ul id=\"fs-id1167981\">\n<li id=\"import-auto-id1238080\">Simple machines are devices that can be used to multiply or augment a force that we apply \u2013 often at the expense of a distance through which we have to apply the force.<\/li>\n<li id=\"import-auto-id2697990\">The ratio of output to input forces for any simple machine is called its mechanical advantage<\/li>\n<li id=\"import-auto-id1279635\">A few simple machines are the lever, nail puller, wheelbarrow, crank, etc.<\/li>\n<\/ul>\n<\/section>\n<section id=\"fs-id3028918\" class=\"conceptual-questions\">\n<div class=\"bcc-box bcc-info\">\n<h3>Conceptual Questions<\/h3>\n<div id=\"fs-id2730066\" class=\"exercise\">\n<div id=\"fs-id2696305\" class=\"problem\">\n<p><strong>1: <\/strong>Why are the forces exerted on the outside world by the limbs of our bodies usually much smaller than the forces exerted by muscles inside the body?<\/p>\n<\/div>\n<\/div>\n<div id=\"fs-id1428982\" class=\"exercise\">\n<div id=\"fs-id1398239\" class=\"problem\">\n<p id=\"import-auto-id2738965\"><strong>2: <\/strong>Explain why the forces in our joints are several times larger than the forces we exert on the outside world with our limbs. Can these forces be even greater than muscle forces (see previous Question)?<\/p>\n<\/div>\n<\/div>\n<\/div>\n<\/section>\n<div>\n<h2>Glossary<\/h2>\n<dl id=\"import-auto-id3034634\" class=\"definition\">\n<dt>mechanical advantage<\/dt>\n<dd id=\"fs-id1370336\">the ratio of output to input forces for any simple machine<\/dd>\n<\/dl>\n<\/div>\n","protected":false},"author":71,"menu_order":8,"template":"","meta":{"pb_show_title":"on","pb_short_title":"","pb_subtitle":"","pb_authors":[],"pb_section_license":""},"chapter-type":[],"contributor":[],"license":[],"class_list":["post-461","chapter","type-chapter","status-publish","hentry"],"part":429,"_links":{"self":[{"href":"https:\/\/pressbooks.bccampus.ca\/humanbiomechanics\/wp-json\/pressbooks\/v2\/chapters\/461","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/pressbooks.bccampus.ca\/humanbiomechanics\/wp-json\/pressbooks\/v2\/chapters"}],"about":[{"href":"https:\/\/pressbooks.bccampus.ca\/humanbiomechanics\/wp-json\/wp\/v2\/types\/chapter"}],"author":[{"embeddable":true,"href":"https:\/\/pressbooks.bccampus.ca\/humanbiomechanics\/wp-json\/wp\/v2\/users\/71"}],"version-history":[{"count":2,"href":"https:\/\/pressbooks.bccampus.ca\/humanbiomechanics\/wp-json\/pressbooks\/v2\/chapters\/461\/revisions"}],"predecessor-version":[{"id":1122,"href":"https:\/\/pressbooks.bccampus.ca\/humanbiomechanics\/wp-json\/pressbooks\/v2\/chapters\/461\/revisions\/1122"}],"part":[{"href":"https:\/\/pressbooks.bccampus.ca\/humanbiomechanics\/wp-json\/pressbooks\/v2\/parts\/429"}],"metadata":[{"href":"https:\/\/pressbooks.bccampus.ca\/humanbiomechanics\/wp-json\/pressbooks\/v2\/chapters\/461\/metadata\/"}],"wp:attachment":[{"href":"https:\/\/pressbooks.bccampus.ca\/humanbiomechanics\/wp-json\/wp\/v2\/media?parent=461"}],"wp:term":[{"taxonomy":"chapter-type","embeddable":true,"href":"https:\/\/pressbooks.bccampus.ca\/humanbiomechanics\/wp-json\/pressbooks\/v2\/chapter-type?post=461"},{"taxonomy":"contributor","embeddable":true,"href":"https:\/\/pressbooks.bccampus.ca\/humanbiomechanics\/wp-json\/wp\/v2\/contributor?post=461"},{"taxonomy":"license","embeddable":true,"href":"https:\/\/pressbooks.bccampus.ca\/humanbiomechanics\/wp-json\/wp\/v2\/license?post=461"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}