Mass, force and weight

Một phần của tài liệu mechanical engineers pocket book (Trang 58 - 63)

2.2.1 Mass

●Mass is the quantity of matter in a body. It is the sum total of the masses of all the sub- atomic particles in that body.

●Matter occupies space and can be solid, liquid or gaseous.

●Unless matter is added to or removed from a body, the mass of that body never varies.

It is constant under all conditions. There are as many atoms in a kilogram of, say, metal on the moon as there are in the same kilogram of metal on planet Earth. However, that kilogram of metal will weighless on the moon than on planet Earth (see Section 2.2.4).

●The basic unit of massis the kilogram (kg). The most commonly used multiple of this basic unit is the tonne (1000 kg) and the most commonly used sub-multiple is the gram (0.001 kg).

2.2.2 Force

To understand how massand weightare related it is necessary to consider the concept of force. A force or a system of forces cannot be seen; only the effect of a force or a system of forces can be seen. That is:

●A force can change or try to change the shape of an object.

●A force can move or try to move a body that is at rest. If the magnitude of the force is sufficiently great it will cause the body to move in the direction of the application of the force. If the force is of insufficient magnitude to overcome the resistance to move- ment it will still tryto move the body, albeit unsuccessfully.

●A force can change or try to change the motion of a body that is already moving. For example:

1. The force of a headwind can decrease the speed of an aircraft over the ground, whereas the force of a tailwind can increase the speed of an aircraft over the ground.

2. The force of a crosswind can cause a car to swerve off course.

●The effect of any force depends on the following:

1. The magnitude (size) of the force measured in newtons (N).

2. The direction of the force.

3. The point of application of the force.

4. The ability of a body to resist the effects of the force.

●As already stated a force cannot be seen; however, it can be represented by a vector.

2.2.3 Vectors

Quantities can be divided into two categories:

●Scalar quantities

●Vector quantities.

Scalar quantitieshave magnitude (size) only. For example:

●The speed of a car can be stated as 50 kilometres per hour (km/h).

●The power of an engine can be rated as 150 kilowatts (kW).

●The current flowing in an electric circuit can be 12 amperes (A).

Vector quantitieshave both magnitudeand direction.For example, the velocity of a car is 50 km/h due north from London. Velocity is a vector quantity since it has both magnitude (speed) and direction (due north).

Similarly, vectors can be used to represent forces and systems of forces. Figure 2.1 shows how a vector can be used to represent a force (F) acting on the point (P) in a direction at 30° to the horizontal with a magnitude of 150 newtons (N). Vector diagrams will be con- sidered in detail in Section 2.3.

30°

F 150 N

P

Figure 2.1 Vector representation of a force.

To represent a force by a vector the following information is required:

●The point of application of the force.

●The magnitude (size) of the force.

●The line of action of the force.

●The direction in which the force is acting. The direction in which the force is acting is shown by the arrowhead. This can be at the end of the vector or at the midpoint of the vector, whichever is the more convenient.

2.2.4 Weight

A solid, liquid or gas of mass 1 kg will weigh 9.81 N due to the gravitational attraction of planet Earth. Since planet Earth is not a perfect sphere a mass of 1 kg will weigh slightly more at the poles and slightly less at the equator. However, for all practical purposes, the average weightof a mass of 1 kg is taken to be 9.81 N on planet Earth:

●The force of gravityattracts the massof any body (solid, liquid or gas) towards the centre of planet Earth.

●The weightof a body is the force of gravity acting on that body.

●Therefore weight is a forcemeasured in newtons.

●The factor 9.81 is the free-fall acceleration of a body due to the force gravity, it is 9.81 metres per second squared (m/s2). Acceleration due to gravity is discussed further in Section 3.6.7.

●Since the weight of a body of mass 1 kg is approximately 9.81 N (average value) on planet Earth, the weight of that body will change on a planet having a different force of gravity or when travelling through space. For example, the gravitational attraction of the Moon is approximately 1/6 that of planet Earth. Therefore a mass of 1 kg will weigh 1/69.811.64 N on the Moon.

2.2.5 Mass per unit volume (density)

A solid object has a volume of 60 cm3. If the mass of this solid is 600 grams (g) then, by proportion,

1 cm3has a mass of 600 g/60 cm310 gram per cm3(10 g/cm3)

Since 1 cm3is unit volume in this instance, then the mass per unit volumeof the solid shown is 10 g/cm3. Mass per unit volumeof any body is also called the density of that body. The symbol for density is the Greek letter ‘rho’ (). The general expression for mass per unit volume (density) is:

m/V where:

density mmass

Vvolume

The densities of some common solids, liquids and gases used in engineering are given in Table 2.1.

2.2.6 Weight per unit volume

The weight per unit volume of a substance can be determined by:

(a) direct measurement,

(b) conversion calculation from the density of the substance.

(a) Weight per unit volume by direct measurement:

Weight per unit volume (N/m3)weight (N)/volume (m3)W/V

(b) Weight per unit volume by conversion calculation:

Weight per unit volumeW/V (1)

Density ()m/V (2)

Weightm9.81 (3)

Substituting equation (3) in equation (2):

Weight per unit volume(m9.81)/V But:

m/V Therefore:

Weight per unit volume 9.81 Note:

●This conversion only applies to planet Earth. Anywhere else in space the local value of gravitational acceleration ‘g’ must be used.

●The value for density must be expressed in kilograms per unit volume.

2.2.7 Relative density

The relative density of a substance may be defined as the ratio:

(Density of the substance)/(density of pure water at 4°C)

Table 2.1 Density of common substances.

Substance Density

kg/m3 g/cm3

Aluminium 2720 2.72

Brass 8480 8.48

Copper 8790 8.79

Cast iron 7200 7.20

Lead 11 350 11.35

Nylon 1120 1.12

PVC 1360 1.36

Rubber 960 0.96

Steel 7820 7.82

Tin 7280 7.28

Zinc 7120 7.12

Alcohol 800 0.80

Mercury 13 590 13.59

Paraffin 800 0.80

Petrol 720 0.72

Water (pure at 4°C) 1000 1.00

Acetylene 1.17 0.001 7

Air (dry) 1.30 0.001 3

Carbon dioxide 1.98 0.001 98

Hydrogen 0.09 0.000 09

Nitrogen 1.25 0.001 25

Oxygen 1.43 0.001 43

or

(Mass of the substance)/(mass of an equal volume of pure water at 4°C) Since relative density is a ratio there are no units.

The relative densities of some common substances used in engineering are given in Table 2.2.

Table 2.2 Relative densities of some common substances.

Substance Relative density (d)

Aluminium 2.72

Brass 8.48

Cadmium 8.57

Chromium 7.03

Copper 8.79

Cast iron 7.20

Lead 11.35

Nickel 8.73

Nylon 1.12

PVC 1.36

Rubber 0.96

Steel 7.82

Tin 7.28

Zinc 7.12

Alcohol 0.80

Mercury 13.95

Paraffin 0.80

Petrol 0.72

Water (pure @ 4°C) 1.00

Water (sea) 1.02

Acetylene 0.001 7

Air (dry) 0.001 3

Carbon dioxide 0.001 98

Carbon monoxide 0.001 26

Hydrogen 0.000 09

Nitrogen 0.001 25

Oxygen 0.001 43

2.2.8 Pressure (fluids)

The pressure acting on the surface area of a body is defined as the normal force per unit areaacting on the surface. Normal force means the force acting at right angles to the sur- face. The SI unit of fluid pressure is the pascal (Pa), where 1 Pa is equal to 1 Nm2. Pressure (p)F/A

where:

ppressure in pascals

Fforce in newtons acting at right angles (normal) to the surface Aarea of the surface in metres squared

Similarly:

1 MPa1 MN/m21 N/mm2

Since the pascal is a very small unit a more practical unit is the bar, where:

1 bar105pascals.

Note:

Atmospheric pressureis usually expressed in millibars.

Gauge pressureis the fluid pressure indicated by a bourdon tube pressure gauge, a U-tube manometer or similar device so that the indicated pressure is additional to the atmospheric pressure.

Absolute pressureused in physical science and thermodynamics is the pressure relative to a perfect vacuum, that is:

Absolute pressureatmospheric pressuregauge pressure

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