An inclined plane is a plane surface set at an angle, other than a right angle, against a horizontal surface. The inclined plane permits one to overcome a large resistance by applying a relatively small force through a longer distance than the load is to be raised. In civil engineering the slope (ratio of rise/run) is often referred to as a grade or gradient. An inclined plane is one of the commonly-recognized simple machines.
Ramps are used as alternatives for stairways, for wheelchairs, buggies and shopping carts. Ramps may zigzag. There are also moving ramps such as the mobile staircases by which passengers board and leave an aircraft.
For example: A wagon trail on a steep hill will often traverse back and forth to reduce the gradient experienced by a team pulling a heavily loaded wagon. This same technique is used today in modern freeways which travel through steep mountain passes. Some steep passes have separate truck routes that reduce the grade by winding along a separate path to rejoin the main route after a particularly steep section is past while smaller automobiles take the straighter steeper route with a resulting saving in time.
Experiments with inclined planes helped early physicists such as Galileo Galilei quantify the behavior of nature with respect to gravity, mass, acceleration, etc.
Detailed understanding of inclined planes and their use helped lead to the understanding of how vector quantities such as forces can be usefully decomposed and manipulated mathematically. This concept of superposition and decomposition is critical in many modern fields of science, engineering, and technology.
The picture below has 3 force vectors (neglecting air resistance and the mass sliding down the inclined plane).
The first vector is the normal force, which is perpendicular to the surface upon which the object rests. It is also the force that is stopping the object from accelerating at gravity's full acceleration (On Earth, gravity acceleration is 9.8 meters/seconds squared).
The second vector is gravity, the attractive force exerted on the object by the planet. Within the gravity vector, there are two components, horizontal and vertical force in the inclined plane perspective. As you can see the angle is on the lower left corner.
What happens if we make that angle zero degrees? The plane will be horizontal and the only force acting on it is gravity (pointing downwards)and normal force (pointing upwards). The only Trigonometry function that makes zero degree = 1 is Cosine, so cosine must be the vertical force. With this fact, we can go back to the inclined plane and use the cosine function to find the vertical force, and the sine function to find the horizontal force.
The inclined plane is also in contact with the block, and the contact causes friction. So the third vector is friction. Since the block is sliding downwards, the friction vector is going the opposite of the horizontal force of gravity.
Taking all these vectors into consideration, we can say the normal force and the vertical component of gravity balances out, because it is not accelerating upwards nor downwards, but sideways. And since, friction is going the opposite direction of the horizontal gravity force, the whole equation is . The mA part is derived from Newton's laws of motion.
Key:
N = Normal force that is perpendicular to the plane
m = Mass of object
g = Acceleration due to gravity
θ (theta) = Angle of elevation of the plane, measured from the horizontal
f = Frictional force of the inclined plane
Pla inclinat | Nakloněná rovina | Schiefe Ebene | Plano inclinado | Piano inclinato | Nuožulnioji plokštuma | 入射面 | Równia pochyła | Наклонная плоскость | Kosina | Klančina | Kalteva taso
This article is licensed under the GNU Free Documentation License.
It uses material from the
"Inclined plane".
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