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Mechanical advantage and levers

We can use our knowlegde about the moments of forces (torque) to determine whether situations are balanced. For example two mass pieces are placed on a seesaw as shown in [link] . The one mass is 3 kg and the other is 6 kg. The masses are placed at distances of 2 m and 1 m (respectively) from the pivot. By looking at the clockwise and anti-clockwise moments, we can determine whether the seesaw will pivot (move) or not. If the sum of the clockwise and anti-clockwise moments is zero, the seesaw is in equilibrium (i.e. balanced).

The moments of force are balanced.

The clockwise moment can be calculated as follows:

τ 1 = F · r τ 1 = ( 6 kg ) ( 9 , 8 m · s - 2 ) ( 1 m ) τ 1 = 58 , 8 N · m clockwise

The anti-clockwise moment can be calculated as follows:

τ 2 = F · r τ 2 = ( 3 kg ) ( 9 , 8 m · s - 2 ) ( 2 m ) τ 2 = 58 , 8 N · m anti - clockwise

The sum of the moments of force will be zero:

The resultant moment is zero as the clockwise and anti-clockwise moments of force are in opposite directions and therefore cancel each other.

As we see in [link] , we can use different distances away from a pivot to balance two different forces. This principle is applied to a lever to make lifting a heavy object much easier.

Lever

A lever is a rigid object that is used with an appropriate fulcrum or pivot point to multiply the mechanical force that can be applied to another object.

A lever is used to put in a small effort to get out a large load.

Interesting fact

Archimedes reputedly said: Give me a lever long enough and a fulcrum on which to place it, and I shall move the world.

The concept of getting out more than the effort is termed mechanical advantage, and is one example of the principle of moments. The lever allows one to apply a smaller force over a greater distance. For instance to lift a certain unit of weight with a lever with an effort of half a unit we need a distance from the fulcrum in the effort's side to be twice the distance of the weight's side. It also means that to lift the weight 1 meter we need to push the lever for 2 meters. The amount of work done is always the same and independent of the dimensions of the lever (in an ideal lever). The lever only allows to trade force for distance.

Ideally, this means that the mechanical advantage of a system is the ratio of the force that performs the work (output or load) to the applied force (input or effort), assuming there is no friction in the system. In reality, the mechanical advantage will be less than the ideal value by an amount determined by the amount of friction.

mechanical advantage = load effort

For example, you want to raise an object of mass 100 kg. If the pivot is placed as shown in [link] , what is the mechanical advantage of the lever?

A lever is used to put in a small effort to get out a large load.

In order to calculate mechanical advantage, we need to determine the load and effort.

Effort is the input force and load is the output force.

The load is easy to calculate, it is simply the weight of the 100 kg object.

F l o a d = m · g = 100 kg · 9 , 8 m · s - 2 = 980 N

The effort is found by balancing torques.

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Source:  OpenStax, Siyavula textbooks: grade 11 physical science. OpenStax CNX. Jul 29, 2011 Download for free at http://cnx.org/content/col11241/1.2
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