Roymech engineering encyclopedia

Simple Machines – Mechanical Advantage and Velocity Ratio


Simple machines transmit or modify force and motion to perform mechanical work. They can provide force multiplication, change the direction of an applied force, or exchange force for movement.

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This page summarises the mechanical advantage, velocity ratio and ideal relationships for the six traditional simple machines: the inclined plane, wedge, lever, wheel and axle, pulley and screw.

Contents


Simple Machine Principles

A simple machine is an idealised mechanical device that transmits or modifies force and motion. An applied effort produces an output force that acts against a load or resistance.

The advantage of a machine is not the creation of energy. Ideally, a reduction in the required input force is obtained at the expense of a greater input movement. Conversely, a mechanism may increase output movement or speed at the expense of output force.

The six traditional simple machines are:

  1. Inclined plane
  2. Wedge
  3. Lever
  4. Wheel and axle
  5. Pulley
  6. Screw

Mechanical Advantage

The actual mechanical advantage of a machine is the ratio of the output load or resistance W to the applied effort F:

MA = W F

A mechanical advantage greater than one indicates force multiplication.

Velocity Ratio

The velocity ratio is the ratio of the distance moved by the effort to the corresponding distance moved by the load:

VR = distance moved by effort distance moved by load

Equivalently, for compatible instantaneous velocities:

VR = veffort vload

Velocity ratio is determined by the geometry and kinematics of the machine. For an ideal, rigid, frictionless machine:

MA = VR

Efficiency

Machine efficiency is the ratio of useful output work to input work:

η = useful output work input work

For a machine operating through corresponding effort and load movements:

η = MA VR

or, as a percentage:

η  (%) = MA VR × 100

Real machines have mechanical advantage below the ideal value because energy is dissipated by friction, deformation and other losses.

Law of a Machine

For some real machines, over a useful operating range, the relationship between effort and load can be represented empirically by the linear law of the machine:

F = a + bW

where F is the effort, W is the load, and a and b are constants determined experimentally for the particular machine and operating conditions.

Engineering note: The velocity ratio can normally be obtained directly from machine geometry. Actual mechanical advantage and efficiency also depend on losses such as friction and therefore cannot generally be determined from ideal geometry alone.

Inclined Plane

An inclined plane allows a load to be raised through a vertical distance by moving it through a greater distance along a slope.

Inclined plane showing effort force, load and slope angle

For an incline at angle θ to the horizontal, movement through a distance x along the slope produces a vertical rise:

h = x sinθ

Therefore the velocity ratio is:

VR = x h = 1 sinθ

For a frictionless incline with the effort applied parallel to the slope, equilibrium or constant-speed motion requires:

F = W sinθ

and hence:

MA = VR = 1 sinθ

With friction present, a greater effort is required and the actual mechanical advantage is lower than the ideal value.


Wedge

A wedge is effectively a moving inclined plane. An input movement along the length of the wedge produces a smaller transverse movement and can therefore generate a larger transverse force.

Single and double wedge geometry used to determine velocity ratio

Single Wedge

For a single wedge with wedge angle θ as shown:

VR = 1 tanθ

Symmetrical Double Wedge

For a symmetrical double wedge having total included angle θ, each face is inclined at θ/2 to the centreline. If the output displacement being considered is the total separation of the two opposing surfaces:

VR = 1 2 tan θ2
Wedge notation: Wedge formulae depend on how the wedge angle and output displacement are defined. The geometry shown in the diagram should always be checked before applying a quoted velocity ratio.

Friction is particularly important in practical wedges. It reduces mechanical advantage and may make a wedge self-locking under suitable geometry and friction conditions.


Lever

A lever is a rigid member that rotates about a fulcrum. Its ideal mechanical advantage is determined by the perpendicular moment arms of the effort and load about the fulcrum.

First, second and third class lever arrangements

For equilibrium of an ideal lever:

F LF = W LW

where LF and LW are the perpendicular moment arms of the effort and load respectively.

Therefore:

MA = VR = LF LW

Lever Classes

Using dimensions A and B as shown in the original diagram:

First-Class Lever

VR = BA

The fulcrum lies between the effort and the load.

Second-Class Lever

VR = A+B A

The load lies between the fulcrum and the effort.

Third-Class Lever

VR = A A+B

The effort lies between the fulcrum and the load.

A third-class lever has a mechanical advantage below one in the ideal case, but provides increased output displacement and velocity.


Wheel and Axle

A wheel and axle consists of two effective radii rotating together about a common axis. If the effort acts tangentially at radius R and the load acts at radius r:

Wheel and axle machine with effort radius R and load radius r

VR = R r

For the ideal machine:

MA = R r

This follows directly from equality of moments:

FR = Wr

Pulley Systems

Block and Tackle

A pulley system can change the direction of an applied force and, when moving pulleys are used, provide force multiplication.

Simple moving pulley supported by two rope segments

Moving Pulley / Block and Tackle

For an ideal pulley arrangement, the velocity ratio is equal to the number n of rope segments directly supporting the moving block:

VR = n

The simple arrangement shown has two supporting rope segments and therefore:

VR = 2

Practical block-and-tackle systems may contain several sheaves in the fixed and moving blocks, increasing the number of supporting rope segments.

Differential pulley with upper sheaves of radii R and r

Differential Pulley

For an ideal differential pulley having upper pitch radii R and r:

VR = 2R R−r

Equivalent forms may be written using pitch diameters instead of radii. The endless chain engages with the upper wheels so that the required differential movement is positively transmitted without slip.

Pulley terminology: A single fixed pulley changes the direction of the effort but ideally has VR = 1. Force multiplication is obtained when the load is carried by a moving pulley or moving block supported by multiple rope or chain segments.

Screw

A screw can be regarded kinematically as an inclined plane wrapped around a cylinder. Rotation of the screw converts circumferential movement into axial movement.

Screw machine operated by an effort applied at handle radius R

If the effort is applied at radius R, one complete revolution moves the effort through:

seffort = 2πR

If the screw advances axially by lead L during one revolution, the velocity ratio is:

VR = 2πR L

For a single-start screw, the lead equals the thread pitch p, giving:

VR = 2πR p

For a multi-start screw:

L = np

where n is the number of thread starts.

Engineering note: The geometrical velocity ratio does not include thread friction, collar friction or other losses. Real screw efficiency and the possibility of self-locking require a frictional power-screw analysis. See the RoyMech Power Screw reference for detailed screw calculations.

Related RoyMech Mechanics References

Related RoyMech Machine-Element References

External Simple Machine References

  1. Simple Machines in Appliances, Gadgets, and Everyday Life – examples of simple machines in practical devices.
  2. Simple Machines – University of Arkansas – introductory reference material.
  3. Machines – J. B. Calvert – detailed notes on machines and mechanical principles.
  4. Simple Machine – Wikipedia – general reference material and further links.


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