Inclined plane

Inclined planes are widely used in the form of loading ramps to load and unload goods on trucks, ships and planes. Wheelchair ramps are used to allow people in wheelchairs to get over vertical obstacles without exceeding their strength. Escalators and slanted conveyor belts are also forms of an inclined plane.In a funicular or cable railway a railroad car is pulled up a steep inclined plane using cables. Inclined planes also allow heavy fragile objects, including humans, to be safely lowered down a vertical distance by using the normal force of the plane to reduce the gravitational force. Aircraft evacuation slides allow people to rapidly and safely reach the ground from the height of a passenger airliner. Other inclined planes are built into permanent structures. Roads for vehicles and railroads have inclined planes in the form of gradual slopes, ramps, and causeways to allow vehicles to surmount vertical obstacles such as hills without losing traction on the road surface. Similarly, pedestrian paths and sidewalks have gentle ramps to limit their slope, to ensure that pedestrians can keep traction. Inclined planes are also used as entertainment for people to slide down in a controlled way, in playground slides, water slides, ski slopes and skateboard parks. ==History==

Inclined planes have been used by people since prehistoric times to move heavy objects. The sloping roads and causeways built by ancient civilizations such as the Romans are examples of early inclined planes that have survived, and show that they understood the value of this device for moving things uphill. The heavy stones used in ancient stone structures such as Stonehenge are believed to have been moved and set in place using inclined planes made of earth, although it is hard to find evidence of such temporary building ramps. The Egyptian pyramids were constructed using inclined planes, Siege ramps enabled ancient armies to surmount fortress walls. The ancient Greeks constructed a paved ramp 6 km (3.7 miles) long, the Diolkos, to drag ships overland across the Isthmus of Corinth. This view persisted among a few later scientists; as late as 1826 Karl von Langsdorf wrote that an inclined plane "...is no more a machine than is the slope of a mountain". The problem of calculating the force required to push a weight up an inclined plane (its mechanical advantage) was attempted by Greek philosophers Heron of Alexandria (c. 10 - 60 CE) and Pappus of Alexandria (c. 290 - 350 CE), but their solutions were incorrect. It was not until the Renaissance that the inclined plane was solved mathematically and classed with the other simple machines. The first correct analysis of the inclined plane appeared in the work of 13th century author Jordanus de Nemore, however his solution was apparently not communicated to other philosophers of the time. The first elementary rules of sliding friction on an inclined plane were discovered by Leonardo da Vinci (1452-1519), but remained unpublished in his notebooks. They were rediscovered by Guillaume Amontons (1699) and were further developed by Charles-Augustin de Coulomb (1785). ==Terminology==

Slope The mechanical advantage of an inclined plane depends on its slope, meaning its gradient or steepness. The smaller the slope, the larger the mechanical advantage, and the smaller the force needed to raise a given weight. A plane's slope s is equal to the difference in height between its two ends, or "rise", divided by its horizontal length, or "run". It can also be expressed by the angle the plane makes with the horizontal, \theta. . ==Frictionless inclined plane==

If there is no friction between the object being moved and the plane, the device is called an ideal inclined plane. This condition might be approached if the object is rolling like a barrel, or supported on wheels or casters. Due to conservation of energy, for a frictionless inclined plane the work done on the load lifting it, W_\text{out}, is equal to the work done by the input force, W_\text{in} :W_{\rm out} = W_{\rm in} \, Work is defined as the force multiplied by the displacement an object moves. The work done on the load is equal to its weight multiplied by the vertical displacement it rises, which is the "rise" of the inclined plane :W_{\rm out} = F_{\rm w} \cdot \text{Rise} \, The input work is equal to the force F_\text{i} on the object times the diagonal length of the inclined plane. :W_{\rm in} = F_{\rm i} \cdot \text{Length} \, Substituting these values into the conservation of energy equation above and rearranging :\text{MA} = \frac{F_{\rm w}}{F_{\rm i}} = \frac {\text{Length}}{\text{Rise}} \, To express the mechanical advantage by the angle \theta of the plane, it can be seen from the diagram (above) that :\sin \theta = \frac {\text{Rise}}{\text{Length}} \, So So the mechanical advantage of a frictionless inclined plane is equal to the reciprocal of the sine of the slope angle. The input force F_{\rm i} from this equation is the force needed to hold the load motionless on the inclined plane, or push it up at a constant velocity. If the input force is greater than this, the load will accelerate up the plane. If the force is less, it will accelerate down the plane. ==Inclined plane with friction==

Where there is friction between the plane and the load, as for example with a heavy box being slid up a ramp, some of the work applied by the input force is dissipated as heat by friction, W_\text{fric}, so less work is done on the load. Due to conservation of energy, the sum of the output work and the frictional energy losses is equal to the input work :W_\text{in} = W_\text{fric} + W_\text{out} \, Therefore, more input force is required, and the mechanical advantage is lower, than if friction were not present. With friction, the load will only move if the net force parallel to the surface is greater than the frictional force F_\text{f} opposing it. The maximum friction force is given by :F_f = \mu F_n \, where F_\text{n} is the normal force between the load and the plane, directed normal to the surface, and \mu is the coefficient of static friction between the two surfaces, which varies with the material. When no input force is applied, if the inclination angle \theta of the plane is less than some maximum value \phi the component of gravitational force parallel to the plane will be too small to overcome friction, and the load will remain motionless. This angle is called the angle of repose and depends on the composition of the surfaces, but is independent of the load weight. It is shown below that the tangent of the angle of repose \phi is equal to \mu :\phi = \tan^{-1} \mu \, With friction, there is always some range of input force F_\text{i} for which the load is stationary, neither sliding up or down the plane, whereas with a frictionless inclined plane there is only one particular value of input force for which the load is stationary. Analysis that is perpendicular to the plane, Fi = f = input force, Fw = mg = weight of the load, where m = mass, g = gravity A load resting on an inclined plane, when considered as a free body has three forces acting on it: • The applied force, F_\text{i} exerted on the load to move it, which acts parallel to the inclined plane. • The weight of the load, F_\text{w}, which acts vertically downwards • The force of the plane on the load. This can be resolved into two components: • The normal force F_\text{n} of the inclined plane on the load, supporting it. This is directed perpendicular (normal) to the surface. • The frictional force, F_\text{f} of the plane on the load acts parallel to the surface, and is always in a direction opposite to the motion of the object. It is equal to the normal force multiplied by the coefficient of static friction μ between the two surfaces. Using Newton's second law of motion the load will be stationary or in steady motion if the sum of the forces on it is zero. Since the direction of the frictional force is opposite for the case of uphill and downhill motion, these two cases must be considered separately: • Uphill motion: The total force on the load is toward the uphill side, so the frictional force is directed down the plane, opposing the input force. = F_i - F_f - F_w \sin \theta = 0 \, :\sum F_{\perp} = F_n - F_w \cos \theta = 0 \, :Substituting F_f = \mu F_n \, into first equation :F_i - \mu F_n - F_w \sin \theta = 0 \, :Solving second equation to get F_n = F_w \cos \theta \, and substituting into the above equation :F_i - \mu F_w \cos \theta - F_w \sin \theta = 0 \, :\frac {F_w}{F_i} = \frac {1} {\sin \theta + \mu \cos \theta} \, :Defining \mu = \tan \phi \, :\frac {F_w}{F_i} = \frac {1} {\sin \theta + \tan \phi \cos \theta} = \dfrac{1}{\sin \theta + \dfrac {\sin \phi}{\cos \phi} \cos \theta} = \frac {\cos \phi} {\sin \theta \cos \phi + \cos \theta \sin \phi } \, :Using a sum-of-angles trigonometric identity on the denominator, }} :The mechanical advantage is :where \phi = \tan^{-1} \mu \,. This is the condition for impending motion up the inclined plane. If the applied force Fi is greater than given by this equation, the load will move up the plane. • Downhill motion: The total force on the load is toward the downhill side, so the frictional force is directed up the plane. = F_i + F_f - F_w \sin \theta = 0 \, :\sum F_{\perp} = F_n - F_w \cos \theta = 0 \, :Substituting F_f = \mu F_n \, into first equation :F_i + \mu F_n - F_w \sin \theta = 0 \, :Solving second equation to get F_n = F_w \cos \theta \, and substituting into the above equation :F_i + \mu F_w \cos \theta - F_w \sin \theta = 0 \, :\frac {F_w}{F_i} = \frac {1} {\sin \theta - \mu \cos \theta} \, :Substituting in \mu = \tan \phi \, and simplifying as above :\frac {F_w}{F_i} = \frac {\cos \phi} {\sin \theta \cos \phi - \cos \theta \sin \phi } \, :Using another trigonometric identity on the denominator, }} :The mechanical advantage is :This is the condition for impending motion down the plane; if the applied force Fi is less than given in this equation, the load will slide down the plane. There are three cases: :#\theta : The mechanical advantage is negative. In the absence of applied force the load will remain motionless, and requires some negative (downhill) applied force to slide down. :#\theta = \phi\,: The 'angle of repose'. The mechanical advantage is infinite. With no applied force, load will not slide, but the slightest negative (downhill) force will cause it to slide. :#\theta > \phi\,: The mechanical advantage is positive. In the absence of applied force the load will slide down the plane, and requires some positive (uphill) force to hold it motionless ==Mechanical advantage using power==

that is perpendicular to the plane, W=mg, where m = mass, g = gravity, and θ (theta) = Angle of inclination of the plane The mechanical advantage of an inclined plane is the ratio of the weight of the load on the ramp to the force required to pull it up the ramp. If energy is not dissipated or stored in the movement of the load, then this mechanical advantage can be computed from the dimensions of the ramp. In order to show this, let the position r of a rail car on along the ramp with an angle, θ, above the horizontal be given by :\mathbf{r} = R (\cos\theta, \sin\theta), where R is the distance along the ramp. The velocity of the car up the ramp is now :\mathbf{v} = V (\cos\theta, \sin\theta). Because there are no losses, the power used by force F to move the load up the ramp equals the power out, which is the vertical lift of the weight W of the load. The input power pulling the car up the ramp is given by :P_{\mathrm{in}} = F V,\! and the power out is :P_{\mathrm{out}} = \mathbf{W}\cdot\mathbf{v} = (0, W)\cdot V (\cos\theta, \sin\theta) = WV\sin\theta. Equate the power in to the power out to obtain the mechanical advantage as : \mathrm{MA} = \frac{W}{F} = \frac{1}{\sin\theta}. The mechanical advantage of an inclined plane can also be calculated from the ratio of length of the ramp L to its height H, because the sine of the angle of the ramp is given by : \sin\theta = \frac{H}{L}, therefore, : \mathrm{MA} = \frac{W}{F} = \frac{L}{H}. Example: If the height of a ramp is H = 1 meter and its length is L = 5 meters, then the mechanical advantage is : \mathrm{MA} = \frac{W}{F} = 5, which means that a 20 lb force will lift a 100 lb load. The Liverpool Minard inclined plane has the dimensions 1804 meters by 37.50 meters, which provides a mechanical advantage of : \mathrm{MA} = \frac{W}{F} = 1804/37.50 = 48.1, so a 100 lb tension force on the cable will lift a 4810 lb load. The grade of this incline is 2%, which means the angle θ is small enough that sin θ≈tan θ. ==See also==