The 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.
The 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.
The inclined plane and its active twin brother the wedge. In the broadest sense, the wedge includes all devices for cutting and piercing .
• It is easier to understand how a wedge works by looking at the inclined plane, which is nothing more than a wedge sliced in half. The wedge does its job by moving. The inclined plane is held stationary while the "wedged material" is moved over it.
• The secret of the plane's mechanical advantage lies in its ability to split the force of gravity into two smaller forces; one perpendicular to and one parallel to the plane. It is only the parallel force which needs to be counteracted by pushing an object laying on the plane.
• If there is no friction on the plane, the pushing effort required will be 1/10th the weight if the length of the plane is 10 times its height. A similar relationship holds for any plane: the extra distance makes it possible to apply an effort smaller than the weight.
wedge |
Calculation of forces acting on an object on an inclined plane
To calculate the forces on an object placed on an inclined plane, consider the three forces acting on it.
• The normal force (N) exerted on the body by the plane due to the force of gravity i.e. mg cos θ
• The force due to gravity (mg, acting vertically downwards) and
• The frictional force (f) acting parallel to the plane.
We can decompose the gravitational force into two vectors, one perpendicular to the plane and one parallel to the plane. Since there is no movement perpendicular to the plane, the component of the gravitational force in this direction (mg cos θ) must be equal and opposite to normal force exerted by the plane, N. If the remaining component of the gravitational force parallel to the surface (mg sin θ) is greater than the static frictional force fs – then the body will slide down the inclined plane with acceleration (g sin θ − fk/m), where fk is the kinetic friction force – otherwise it will remain stationary.
When the slope angle (θ) is zero, sin θ is also zero so the body does not move.
Tidak ada komentar:
Posting Komentar