1

Engineering Mathematics

1.1 The Greek alphabet

NameSymbolExamples of use
CapitalLower case
alphaAαAngles, angular acceleration, various coefficients
betaBβAngles, coefficients
gammaΓγShear strain, surface tension, kinematic viscosity
deltaΔδDifferences, damping coefficient
epsilonEεLinear strain
zetaZζ
etaHηDynamic viscosity, efficiency
thetaΘθAngles, temperature, volume strain
iotaIι
kappaKκCompressibility
lambdaΛλWavelength, thermal conductivity
muMμPoisson’s ratio, coefficient of friction
nuNvDynamic viscosity
xiΞξ
omicronOο
piΠπMathematical constant
rhoPρDensity
sigmaΣσNormal stress, standard deviation, sum of
tauTτShear stress
upsilonYv
phiϕϕAngles, heat flow rate, potential energy
chiXX
psiΨψHelix angle (gears)
omegaΩωAngular velocity, solid angle (ω) electrical resistance (Ω)

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1.2 Mathematical symbols

Is equal to=
Is identically equal to
Approaches
Is smaller than<
Is smaller than or equal to
Magnitude of a|a|si1_e
Square root of aasi2_e
Mean value of aˉasi3_e
Sumsi4_e
Complex operatori, j
Imaginary part of zIm z
Argument of zarg z
Is not equal to
Is approximately equal to
Is proportional tosi5_e
Is larger than>
Is larger than or equal to
a raised to power nansi6_e
nth root of anasi7_e
Factorial aa!
Productsi8_e
Real part of zRe z
Modulus of z|z|si9_e
Complex conjugate of zz*
a multiplied by bab, ab,a×bsi10_e
a divided by ba/b,ab,ab1si11_e
Function of xf(x)si12_e
Variation of xδxsi13_e
Finite increment of xΔxsi14_e
Limit to which f(x) tends as x approaches alimxaf(X)si15_e
Differential coefficient of f(x) with respect to xdfdx,df/dx,f(x)si16_e
Indefinite integral of f(x) with respect to xf(x)dxsi17_e
Increase in value of f(x) as x increases from a to b[f(x)]basi18_e
Definite integral of f(x) from x = a to x = bbaf(x)dxsi19_e
Logarithm to the base 10 of xlgX,log10Xsi20_e
Logarithm to the base a of xlogaXsi21_e
Exponential of xexp x, eXsi22_e
Natural logarithmIn x, logexsi23_e
Inverse sine of xarcsinxsi24_e
Inverse cosine of xarccosxsi25_e
Inverse tangent of xarctanxsi26_e
Inverse secant of xarcsecxsi27_e
Inverse cosecant of xarccosecxsi28_e
Inverse cotangent of xarccotxsi29_e
Inverse hyperbolic sine of xarcsinhxsi30_e
Inverse hyperbolic cosine of xarcoshxsi31_e
Inverse hyperbolic tangent of xartanhxsi32_e
Inverse hyperbolic cosecant of xarcosechxsi33_e
Inverse hyperbolic secant of xarsechxsi34_e
Inverse hyperbolic cotangent of xarcothxsi35_e
VectorA
Magnitude of vector A|A|,Asi36_e
Scalar products of vectors A and BABsi37_e
Vector products of vectors A and BA×B,ABsi38_e

1.3 Units: SI

1.3.1 Basic and supplementary units

The International System of Units (SI) is based on nine physical quantities.

Physical quantityUnit nameUnit symbol
Lengthmetrem
Masskilogramkg
Timeseconds
Plane angleradianrad
Amount of substancemolemol
Electric currentampereA
Luminous intensitycandelacd
Solid anglesteradiansr
Thermodynamic temperaturekelvinK

1.3.2 Derived units

By dimensionally appropriate multiplication and/or division of the units shown above, derived units are obtained. Some of these are given special names.

Physical quantityUnit nameUnit symbolDerivation
Electric capacitancefaradF(A2 s4)/(kg m2)
Electric chargecoulombCAs
Electric conductancesiemensS(A2 s3)/(kg m2)
Electric potential differencevoltV(kg m2)/(A s3)
Electrical resistanceohmΩ(kg m2)/(A2 s3)
EnergyjouleJ(kg m2)/s2
ForcenewtonN(kg m)/s2
FrequencyhertzHz1/s
Illuminanceluxlx(cd sr)/m2
InductancehenryH(kg m2)/(A2 s2)
Luminous fluxlumenlmcd sr
Magnetic fluxweberWb(kg m2)/(A s2)
Magnetic flux densityteslaTkg/(A s2)
PowerwattW(kg m2)/s3
PressurepascalPakg/(m s2)

t0025

Some other derived units not having special names.

Physical quantityUnitUnit symbol
Accelerationmetre per second squaredm/s2
Angular velocityradian per secondrad/s
Areasquare metrem2
Current densityampere per square metreA/m2
Densitykilogram per cubic metrekg/m3
Dynamic viscositypascal secondPa s
Electric charge densitycoulomb per cubic metreC/m3
Electric field strengthvolt per metreV/m
Energy densityjoule per cubic metreJ/m3
Heat capacityjoule per kelvinJ/K
Heat flux densitywatt per square metreW/m2
Kinematic viscositysquare metre per secondm2/s
Luminancecandela per square metrecd/m2
Magnetic field strengthampere per metreA/m
Moment of forcenewton metreN m
Permeabilityhenry per metreH/m
Permittivityfarad per metreF/m
Specific volumecubic metre per kilogramm3/kg
Surface tensionnewton per metreN/m
Thermal conductivitywatt per metre kelvinW/(m K)
Velocitymetre per secondm/s
Volumecubic metrem3

1.3.3 Units: not SI

Some of the units which are not part of the SI system, but which are recognized for continued use with the SI system, are as shown.

Physical quantityUnit nameUnit symbolDefinition
Angledegree°(π/180) rad
Angleminute'(π/10800) rad
Anglesecond"(π/648000) rad
Celsius temperaturedegree Celsius°CK – 273.2 (For K see 1.3.1)
Dynamic viscositypoiseP10−1 Pas
Energycaloriecal≈4.18J(π/180)rad
Fahrenheit temperaturedegree Fahrenheit°F(95)C+32si42_e
Forcekilogram forcekgf≈9.807 N
Kinematic viscositystokesSt10–4m2/s
Lengthinchin.2.54 Χ 10−2m
Lengthmicronµm10−6m
Masspoundlb≈0.454kg
Masstonnet103kg
Pressureatmosphereatm101 325 Pa
Pressurebarbar105 Pa
Pressuremillimetre of mercurymm Hg≈ 133.322 Pa
Pressuretorrtorr≈ 133.322 Pa
Thermodynamic temperaturedegree Rankine°R°F + 459.7
Timeminutemin60 s
Timehourh3600s
Timedayd86400s

t0035

1.3.4 Notes on writing symbols

(a) Symbols should be in roman type lettering: thus cm, not cm.

(b) Symbols should remain unaltered in the plural: thus cm, not cms.

(c) There should be a space between the product of two symbols: thus N m, not Nm.

(d) Index notation may be used: thus m/s may be written as m s−1 and W/(m K) as Wm−1 K−1

1.3.5 Decimal multiples of units

For quantities which are much larger or much smaller than the units so far given, decimal multiples of units are used.

Internationally agreed multiples are as shown.

For small quantities

MultiplePrefixSymbol
10−1decid
10−2centic
10−3millim
10−6microµ
10−9nanon
10−12picop
10−15femtof
10−18attoa

For large quantities

MultiplePrefixSymbol
10decada
102hectoh
103kilok
106megaM
109gigaG
1012teraT
1015petaP
1018exaE

Notes

(a) A prefix is used with the gram, not the kilogram: thus Mg, not kkg.

(b) A prefix may be used for one or more of the unit symbols: thus kN m, N mm and kN mm are all acceptable.

(c) Compound prefixes should not be used: thus ns, not mµs.

1.4 Conversion factors for units

The conversion factors shown below are accurate to five significant figures where FPS is the foot-pound-second system.

1.4.1 FPS to SI units

Acceleration
1 ft/s2= 0.30480 m/s2
Angular velocity
1 rev/min= 0.104 72 rad/s
Area
1 in.2= 6.4516cm2
1 ft2= 0.092 903 m2
1 yd2= 0.83613 m2
1 acre= 0.404 69 ha
Density
1 lb/ft3= 16.018 kg/m3
Energy
1 ft pdl= 0.042 140 J
1 ft lbf= 1.355 82 J
1 kWh= 3.6000 MJ
1 therm= 0.105 51 GJ
Force
1 pdl= 0.138 26N
1 lbf= 4.4482 N
Length
1 in.= 2.5400 cm
1 ft= 0.304 80 m
1 yd= 0.91440m
1 mi= 1.6093 km
Mass
1 oz= 28.350 g
1 lb= 0.453 59 kg
1 cwt= 50.802 kg
1 ton= 1.0161 tonne
Moment of force
1 lbf ft= 1.3558 Nm
Plane angle
= 0.017 45 rad
Power
1 ft lbf/s= 1.3558 W
1 hp= 0.745 70 kW
Pressure and stress
1 in. Hg= 33.864 mbar
1 lbf/in.2= 6.8948 kPa
1 tonf/in.2= 15.444 N/mm2
Specific heat capacity
1 Btu/(lb°F)= 4.1868 kJ/(kg°C)
Velocity
1 ft/s= 0.304 80 m/s
1 mi/h= 1.6093 km/h
Volume
1 in.3= 16.387 cm3
1 ft3= 0.028317m3
1 yd3= 0.764 56 m3
1 pt= 0.568 261
1 gal= 4.5461 l

t0050

1.4.2 SI to FPS units

Acceleration
1 m/s2= 3.2808 ft/s2
Angular velocity
1 rad/s= 9.5493 rev/min
Area
1 cm2= 0.155 00 in.2
1m2= 10.764 ft2
1m2= 1.1960yd2
1 ha= 2.4711 acre
Density
1 kg/m3= 0.062 428 lb/ft3
Energy
1J= 23.730 ft pdl
1J= 0.737 56ft lbf
1 MJ= 0.277 78 kWh
1 GJ= 9.4781 therm
Force
1N= 7.2330 pdl
1N= 0.22481 lbf
Length
1 cm= 0.393 70 in.
1 m= 3.2808ft
1 m= 1.0936 yd
1 km= 0.621 37 mi
Mass
1g= 0.035 274oz
1 kg= 2.2046 lb
1 kg= 2.2046 lb
1 tonne= 0.984 21 ton
Moment of force
1 Nm= 0.737 56 lbf ft
Plane angle
1 rad= 57.296°
Power
1W= 0.737 56ft lbf/s
1 kW= 1.3410 hp
Pressure and stress
1 mbar= 0.029 53 in. Hg
1 kPa= 0.145 04 lbf/in.2
1 N/mm2= 0.064 749tonf/in.2
Specific heat capacity
1 kJ/(kg °C)= 0.23885 Btu/(lb°F)
Velocity
1 m/s= 3.2808 ft/s
km/h= 0.621 37 mi/h
Volume
1cm3= 0.061 024 in.3
1m3= 35.315ft3
1m3= 1.3080yd3
1l= 1.7598 pt
1l= 0.21997 gal

t0055

1.5 Preferred numbers

When one is buying, say, an electric lamp for use in the home, the normal range of lamps available is 15, 25, 40, 60, 100W and so on. These watt values approximately follow a geometric progression, roughly giving a uniform percentage change in light emission between consecutive sizes. In general, the relationship between the sizes of a commodity is not random but based on a system of preferred numbers.

Preferred numbers are based on R numbers devised by Colonel Charles Renard. The principal series used are R5, R10, R20, R40 and R80, and subsets of these series. The values within a series are approximate geometric progressions based on common ratios of 510,1010,2010,4010and8010,si43_e representing changes between various sizes within a series of 58% for the R5 series, 26% for the R10, 12% for the R20, 6% for the R40 and 3% for the R80 series.

Further details on the values and use of preferred numbers may be found in BS 2045:1965. The rounded values for the R5 series are given as 1.00, 1.60, 2.50, 4.00, 6.30 and 10.00; these values indicate that the electric lamp sizes given above are based on the R5 series. Many of the standards in use are based on series of preferred numbers and these include such standards as sheet and wire gauges, nut and bolt sizes, standard currents (A) and rotating speeds of machine tool spindles.

1.6 Mensuration

1.6.1 Plane figures

f01-01-9780750665087

f01-02-9780750665087

f01-03-9780750665087

f01-04-9780750665087

f01-05-9780750665087

f01-06-9780750665087

f01-07-9780750665087

f01-08-9780750665087

f01-09-9780750665087

Several methods are used to find the shaded area, such as the mid-ordinate rule, the trapezoidal rule and Simpson’s rule. As an example of these, Simpson’s rule is as shown. Divide x1x2 into an even number of equal parts of width d. Let p, q, r, … be the lengths of vertical lines measured from some datum, and let A be the approximate area of the irregular plane, shown shaded. Then:

A=d3[(p+t)+4(q+s)+2r]d3[(p+t)+4(u+w)+2r]

si52_e

In general, the statement of Simpson’s rule is:

Approximate area=(d/3)×[(first+last)+4(sum of evens)+2(sum of odds)]

si53_e

where first, last, evens, odds refer to ordinate lengths and d is the width of the equal parts of the datum line.

1.6.2 Solid objects

f01-10-9780750665087

f01-11-9780750665087

f01-12-9780750665087

f01-13-9780750665087

f01-14-9780750665087

f01-15-9780750665087

f01-16-9780750665087

f01-17-9780750665087

The volume of any regular solid can be found by using the prismoidal rule. Three parallel planes of areas A1, A3 and A2 are considered to be at the ends and at the centre of the solid, respectively. Then:

Volume=(l/6)(A1+4A2+A3)

si61_e

Where:

l is the length of the solid.

f01-18-9780750665087

Various methods can be used to determine volumes of irregular solids; one of these is by applying the principles of Simpson’s rule (see earlier this section). The solid is considered to be divided into an even number of sections by equally spaced, parallel planes, distance d apart and having areas of A1, A2, A3, …. Assuming, say, seven such planes, then approximate volume =(d/3)[(A1+A7)+4(A2+A4+A6)+2(A3+A5)].si62_e

1.7 Powers, roots and reciprocals

nn2nsi63_e10nsi64_en3(n)1/3si65_e(10n)1/3si66_e(100n)1/3si67_e1/n
111.0003.16211.0002.1544.6421.000 00
241.4144.47281.2602.7145.8480.500 00
391.7325.477271.4423.1076.6940.333 33
4162.0006.325641.5873.4207.3680.250 00
5252.2367.0711251.7103.6847.9370.200 00
6362.4497.7462161.8173.9158.4340.166 67
7492.6468.3673431.9134.1218.8790.142 86
8642.8288.9445122.0004.3099.2830.125 00
9813.0009.4877292.0804.4819.6550.111 11
101003.16210.0001 0002.1544.64210.0000.100 00
111213.31710.4881 3312.2244.79110.3230.090 91
121443.46410.9541 7382.2894.93210.6270.08333
131693.60611.4022 1972.3515.06610.9140.076 92
141963.74211.8322 7442.4105.19211.1870.071 43
152253.87312.24733752.4665.31311.4470.066 67
162564.00012.64940962.5205.42911.6960.062 50
172894.12313.03849132.5715.54011.9350.058 82
183244.24313.4165 8322.6215.64612.1640.055 56
193614.35913.78468592.6685.74912.3860.052 63
204004.47214.1428 0002.7145.84812.5990.050 00
214414.58314.4919 2612.7595.94412.8060.047 62
224844.69014.83210 6482.8026.03713.0060.045 45
235294.79615.16612 1672.8446.12713.2000.043 48
245764.89915.49213 8242.8846.21413.3890.041 67
256255.00015.81115 6252.9246.30013.5720.040 00
266765.09916.12517 5762.9626.38313.7510.038 46
277295.19616.43219 6833.0006.46313.9250.037 04
287845.29216.73321 9523.0376.54214.0950.035 71
298415.38517.029243893.0726.61914.2600.034 48
309005.47717.32127 0003.1076.69414.4220.033 33
319615.56817.607297913.1416.76814.5810.032 26
3210245.65717.88932 7683.1756.84014.7360.031 25
3310895.74518.16635 9373.2086.91014.8880.030 30
3411565.83118.43939 3043.2406.98015.0370.029 41
3512255.91618.70842 8753.2717.04715.1830.028 57
3612966.00018.97446 6563.3027.11415.3260.027 78
3713696.08319.23550 6533.3327.17915.4670.027 03
3814446.16419.49454 8723.3627.24315.6050.026 32
3915216.24519.74859 3193.3917.30615.7410.025 64
4016006.32520.00064 0003.4207.36815.8740.025 00
4116816.43020.24868 9213.4487.42916.0050.024 39
4217646.48120.49474 0883.4767.48916.1340.023 81
4318496.55720.73679 5073.5037.54816.2610.023 26
4419366.63320.97685 1843.5307.60616.3860.022 73
4520256.70821.21391 1253.5577.66316.5100.022 22
4621166.78221.44897 3363.5837.71916.6310.021 74
4722096.85621.679103 8233.6097.77516.7510.021 28
4823046.92821.909110 5923.6347.83016.8690.020 83
4924017.00022.136117 6493.6597.88416.9850.020 41
5025007.07122.361125 0003.6847.93717.1000.020 00
5126017.14122.583132 6513.7087.99017.2130.019 61
5227047.21122.804140 6083.7338.04117.3250.019 23
5328097.28023.022148 8773.7568.09317.4350.018 87
5429167.34823.238157 4643.7808.14317.5440.018 52
5530257.41623.452166 3753.8038.19317.6520.018 18
5631367.48323.664175 6163.8268.24317.7580.017 86
5732497.55023.875185 1933.8498.29117.8630.017 54
5833647.61624.083195 1123.8718.34017.9670.017 24
5934817.68124.290205 3793.8938.38718.0700.016 95
6036007.74624.495216 0003.9158.43418.1710.016 67
6137217.81024.698226 9813.9368.48118.2720.016 39
6238447.87424.900238 3283.9588.52718.3710.016 13
6339697.93725.100250 0473.9798.57318.4690.015 87
6440968.00025.298262 1444.0008.61818.5660.015 62
6542258.06225.495274 6254.0218.66218.6630.015 38
6643568.12425.690287 4964.0418.70718.7580.015 15
6744898.18525.884300 7634.0628.75018.8520.014 93
6846248.24626.077314 4324.0828.79418.9450.014 71
6947618.30726.268328 5094.1028.83719.0380.014 49
7049008.36726.458343 0004.1218.87919.1290.014 29
7150418.42626.646357 9114.1418.92119.2200.014 08
7251848.48526.833373 2484.1608.96319.3100.013 89
7353298.54427.019389 0174.1799.00419.3990.013 70
7454768.60227.203405 2244.1989.04519.4870.013 51
7556258.66027.386421 8754.2179.08619.5740.013 33
7657768.71827.568438 9764.2369.12619.6610.013 16
7759298.77527.749456 5334.2549.16619.7470.012 99
7860848.83227.928474 5524.2739.20519.8320.012 82
7962418.88828.107493 0394.2919.24419.9160.012 66
8064008.94428.284512 0004.3099.28320.0000.012 50
8165619.00028.460531 4414.3279.32220.0830.012 35
8267249.05528.636551 3684.3449.36020.1650.012 20
8368899.11028.810571 7874.3629.39820.2470.012 05
8470569.16528.983592 7044.3809.43520.3280.011 90
8572259.22029.155614 1254.3979.47320.4080.011 76
8673969.27429.326636 0564.4149.51020.4880.011 63
8775699.32729.496658 5034.4319.54620.5670.011 49
8877449.38129.665681 4724.4489.58320.6460.011 36
8979219.43429.833704 9694.4659.61920.7240.011 24
9081009.48730.000729 0004.4819.65520.8010.011 11
9182819.53930.166753 5714.4989.69120.8780.010 99
9284649.59230.332778 6884.5149.72620.9540.010 87
9386499.64430.496804 3574.5319.76121.0290.010 75
9488369.69530.659830 5844.5479.79621.1050.010 64
9590259.74730.822857 3754.5639.83021.1790.010 53
9692169.79830.984884 7364.5799.86521.2530.010 42
9794099.84931.145912 6734.5959.89921.3270.010 31
9896049.89931.305941 1924.6109.93321.4000.010 20
9998019.95031.464970 2994.6269.96721.4720.010 10

t0060_at0060_b

1.8 Progressions

A set of numbers in which one number is connected to the next number by some law is called a series or a progression.

1.8.1 Arithmetic progressions

The relationship between consecutive numbers in an arithmetic progression is that they are connected by a common difference. For the set of numbers 3, 6, 9, 12, 15, …, the series is obtained by adding 3 to the preceding number; that is, the common difference is 3. In general, when a is the first term and d is the common difference, the arithmetic progression is of the form:

Term1st2nd3rd4thlast
Valueaa + da + 2da + 3d, …a +(n − 1)d

t0065

where:

n is the number of terms in the progression.

The sum Sn of all the terms is given by the average value of the terms times the number of terms; that is:

Sn=[(first+last)/2]×(numberofterms)=[(a+a+(n1)d)/2]×n=(n/2)[2a+(n1)d]

si68_e

1.8.2 Geometric progressions

The relationship between consecutive numbers in a geometric progression is that they are connected by a common ratio. For the set of numbers 3, 6, 12, 24, 48, …, the series is obtained by multiplying the preceding number by 2. In general, when a is the first term and r is the common ratio, the geometric progression is of the form:

Term1st2nd3rd4thlast
Valueaarar2ar3, …ar(n − 1)

t0070

where:

n is the number of terms in the progression.

The sum Sn of all the terms may be found as follows:

Sn=a+ar+ar2+ar3+...+arn1

si69_e  (1)

Multiplying each term of equation (1) by r gives

rSn=ar+ar2+ar3+...+arn1+arn

si70_e  (2)

Subtracting equation (2) from (1) gives:

Sn(1r)=aarnSn=[a(1r2)]/(1r)

si71_e  (3)

Alternatively, multiplying both numerator and denominator by −1 gives:

Sn=[a(rn1)]/(r1)

si72_e  (4)

It is usual to use equation (3) when r<1 and (4) when r>1.

When 1>r>1,si73_eeach term of a geometric progression is smaller than the preceding term and the terms are said to converge. It is possible to find the sum of all the terms of a converging series. In this case, such a sum is called the sum to infinity. The term [a(1rn)]/(1r)si74_ecan be rewritten as [a/(1r)][arn/(1r)].si75_eSince r is less than 1, rn becomes smaller and smaller as n grows larger and larger. When n is very large, rn effectively becomes zero, and thus [arn/(1r)].si76_ebecomes zero. It follows that the sum to infinity of a geometric progression is a/(1r),si77_ewhich is valid when 1>r>1.si78_e

1.8.3 Harmonic progressions

The relationship between numbers in a harmonic progression is that the reciprocals of consecutive terms form an arithmetic progression. Thus for the arithmetic progression 1, 2, 3, 4, 5, …, the corresponding harmonic progression is 1, 1/2, 1/3, 1/4, 1/5, ….

1.9 Trigonometric formulae

1.9.1 Basic definitions

In the right-angled triangle shown below, a is the side opposite to angle A, b is the hypotenuse of the triangle and c is the side adjacent to angle A. By definition:

sinA=opp/hyp=a/bcosA=adj/hyp=c/btanA=opp/adj=a/ccosecA=hyp/opp=b/a=1/sinAsecA=hyp/adj=b/c=1/cosAcotA=adj/opp=c/a=1/tanA

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1.9.2 Identities

sin2A+cos2A=11+tan2A=sec2A1+cot2A=cosec2Asin(A)=sinAcos(A)=cosAtan(A)=tanA

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1.9.3 Compound and double angle formulae

sin(A+B)=sinAcosB+cosAsinBsin(AB)=sinAcosBcosAsinBcos(A+B)=cosAcosBsinAsinBcos(AB)=cosAcosB+sinAsinBtan(A+B)=(tanA+tanB)/(1tanAtanB)tan(AB)=(tanAtanB)/(1+tanAtanB)sin2A=2sinAcosAcos2A=cos2Asin2A=2cos2A1=12sin2Atan2A=(2tanA)/(1tan2A)

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1.9.4 ‘Product to sum’ formulae

sinAcosB=12[sin(A+B)+sin(AB)]cosAsinB=12[sin(A+B)sin(AB)]cosAcosB=12[cos(A+B)+cos(AB)]sinAsinB=12[cos(A+B)cos(AB)]

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1.9.5 Triangle formulae

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With reference to the above figure:

Sine rule:

a/sinA=b/sinB=c/sinC

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Cosine rule:

a2=b2+c22bccosAb2=c2+a22cacosBc2=a2+b22abcosC

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Area:

Area=12absinC=12bcsinA=12casinB

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Also:

Area=s(sa)(sa)(sc)

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where:

s is the semi-perimeter, that is, (a + b + c)/2.

1.10 Circles: some definitions and properties

For a circle of diameter d and radius r:

The circumference is πd or 2πr

The area is πd2/4si87_e or πr2.si88_e

An arc of a circle is part of the circumference.

A tangent to a circle is a straight line which meets the circle at one point only. A radius drawn from the point where a tangent meets a circle is at right angles to the tangent.

A sector of a circle is the area between an arc of the circle and two radii. The area of a sector is, 12r2θ,si89_e where θ is the angle in radians between the radii.

A chord is a straight line joining two points on the circumference of a circle. When two chords intersect, the product of the parts of one chord is equal to the products of the parts of the other chord. In the following figure, AE × BE = CE × ED.

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A segment of a circle is the area bounded by a chord and an arc. Angles in the same segment of a circle are equal: in the following figure, angle A = angle B.

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1.10.1 Circles: areas and circumferences

DiameterAreaCircumference
10.78543.142
23.14166.283
37.06869.425
412.56612.57
519.63515.71
628.27418.85
738.48521.99
850.26525.13
963.61728.27
1078.54031.42
1195.03334.56
12113.1037.70
13132.7340.84
14153.9443.98
15176.7147.12
16201.0650.27
17226.9853.41
18254.4756.55
19283.5359.69
20314.1662.83
21346.3665.97
22380.1369.11
23415.4872.26
24452.3975.40
25490.8778.54
26530.9381.68
27572.5684.82
28616.7587.96
29660.5291.11
30706.8694.25
31754.7797.39
32804.25100.5
33855.30103.7
34907.92106.8
35962.11110.0
361017.9113.1
371075.2116.2
381134.1119.4
391194.6122.5
401256.6125.7
411320.3128.8
421385.4131.9
431452.2135.1
441520.5138.2
451590.4141.4
461661.9144.5
471734.9147.7
481809.6150.8
491885.7153.9
501963.5157.1
512042.8160.2
522123.7163.4
532206.2166.5
542290.2169.6
552375.8172.8
562463.0175.9
572551.8179.1
582642.1182.2
592734.0185.4
602827.4188.4
612922.5191.6
623019.1194.8
633117.2197.9
643217.0201.1
653318.3204.2
663421.2207.3
673525.7210.5
683631.7213.6
693739.3216.8
703848.5219.9
713959.2223.1
724071.5226.2
734185.4229.3
744300.8232.5
754417.9235.6
764536.5238.8
774656.6241.9
784778.4245.0
794901.7248.2
805026.5251.3
815153.0254.5
825381.0257.6
835410.6260.8
845541.8263.9
855674.5267.0
865808.8270.2
875944.7273.3
886082.1276.5
896221.1279.6
906361.7282.7
916503.9285.9
926647.6289.0
936792.9292.2
946939.8295.3
957088.2298.5
967238.2301.6
977389.8304.7
987543.0307.9
997697.7311.0

1.11 Quadratic equations

The solutions (roots) of a quadratic equation:

ax2+ bx + c= 0

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are:

x=b±b24ac2a

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1.12 Natural logarithms

The natural logarithm of a positive real number x is denoted by In x. It is defined to be a number such that:

elnx=x

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where:

e = 2.1782 which is the base of natural logarithms.

Natural logarithms have the following properties:

In(xy)=Inx+InyIn(x/y)=InxInyInyx=xIny

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1.13 Statistics: an introduction

1.13.1 Basic concepts

To understand the fairly advanced statistics underlying quality control, a certain basic level of statistics is assumed by most texts dealing with this subject. The brief introduction given below should help to lead readers into the various texts dealing with quality control.

The arithmetic mean, or mean, is the average value of a set of data. Its value can be found by adding together the values of the members of the set and then dividing by the number of members in the set. Mathematically:

X=(X1+X2+……+XN)/N

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Thus the mean of the set of numbers 4, 6, 9, 3 and 8 is (4+6+9+3+8)/5=6.si95_e

The median is either the middle value or the mean of the two middle values of a set of numbers arranged in order of magnitude. Thus the numbers 3, 4, 5, 6, 8, 9, 13 and 15 have a median value of (6+8)/2=7,si96_e and the numbers 4, 5, 7, 9, 10, 11, 15, 17 and 19 have a median value of 10.

The mode is the value in a set of numbers which occurs most frequently. Thus the set 2, 3, 3, 4, 5, 6, 6, 6, 7, 8, 9 and 9 has a modal value of 6.

The range of a set of numbers is the difference between the largest value and the smallest value. Thus the range of the set of numbers 3, 2, 9, 7, 4, 1, 12, 3, 17 and 4 is 17 − 1 = 16.

The standard deviation, sometimes called the root mean square deviation, is defined by:

s=[(X1X)2+(X2X)2++(XNX)2]/N

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Thus for the numbers 2, 5 and 11, the mean in (2 + 5 + 11)/3), that is 6. The standard deviation is:

s=[(26)2+(56)2+(116)2]/3=(16+1+25)/3=143.74

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Usually s is used to denote the standard deviation of a population (the whole set of values) and σ is used to denote the standard deviation of a sample.

1.13.2 Probability

When an event can happen x ways out of a total of n possible and equally likely ways, the probability of the occurrence of the event is given by p=x/n.si99_eThe probability of an event occurring is therefore a number between 0 and 1. If q is the probability of an event not occurring it also follows that p+q=1.si100_e Thus when a fair six-sided dice is thrown, the probability of getting a particular number, say a three, is 1/6, since there are six sides and the number three only appears on one of the six sides.

1.13.3 Binomial distribution

The binomial distribution as applied to quality control may be stated as follows.

The probability of having 0, 1, 2, 3, …, n defective items in a sample of n items drawn at random from a large population, whose probability of a defective item is p and of a nondefective item is q, is given by the successive terms of the expansion of (q+p)n,si101_e taking terms in succession from the right.

Thus if a sample of, say, four items is drawn at random from a machine producing an average of 5% defective items, the probability of having 0, 1, 2, 3 or 4 defective items in the sample can be determined as follows. By repeated multiplication:

(q+p)4=q4+4q3p+6q2p2+4qp3+p4

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The values of q and p are q = 0.95 and p = 0.05. Thus:

(0.95+0.05)4=0.954+(4×0.953×0.05)+(6×0.952×0.052)+(4×0.95×0.053)+0.054=0.8145+0.1715+0.011354+

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This indicates that

(a) 81% of the samples taken are likely to have no defective items in them.

(b) 17% of the samples taken are likely to have one defective item.

(c) 1% of the samples taken are likely to have two defective items.

(d) There will hardly ever be three or four defective items in a sample.

As far as quality control is concerned, if by repeated sampling these percentages are roughly maintained, the inspector is satisfied that the machine is continuing to produce about 5% defective items. However, if the percentages alter then it is likely that the defect rate has also altered. Similarly, a customer receiving a large batch of items can, by random sampling, find the number of defective items in the samples and by using the binomial distribution can predict the probable number of defective items in the whole batch.

1.13.4 Poisson distribution

The calculations involved in a binomial distribution can be very long when the sample number n is larger than about six or seven, and an approximation to them can be obtained by using a Poisson distribution. A statement for this is:

When the chance of an event occurring at any instant is constant and the expectation np of the event occurring is λ, then the probabilities of the event occurring 0, 1, 2, 3, 4, … times are given by:

eλ,λeλ,λ2eλ/2!,λ3eλ/3!,λ4eλ/4!,

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where:

e is the constant 2.71828 … and 2!=2 × 1, 3!=3 × 2 × 1, 4!=4 × 3 × 2 × 1, and so on (where 4! is read ‘four factorial').

Applying the Poisson distribution statement to the machine producing 5% defective items, used above to illustrate a use of the binomial distribution, gives:

expectation np  4 × 0.05 =0.2 probability of no defective items iseλ=e0.2=0.8187probability of one defective item isλeλ=0.2e0.2=0.1637probability of two defective items isλ2eλ/2!=0.22e0.2/2=0.0164

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It can be seen that these probabilities of approximately 82%, 16% and 2% compare quite well with the results obtained previously.

1.13.5 Normal distribution

Data associated with measured quantities such as mass, length, time and temperature is called continuous, that is, the data can have any values between certain limits. Suppose that the lengths of items produced by a certain machine tool were plotted as a graph, as shown in the figure; then it is likely that the resulting shape would be mathematically definable. The shape is given by y=(1/σ)ez,si106_e where z=(X2/2σ2),si107_e is the standard deviation of the data, and x is the frequency with which the data occurs. Such a curve is called a normal probability or a normal distribution curve.

Important properties of this curve to quality control are:

(a) The area enclosed by the curve and vertical lines at ±1 standard deviation from the mean value is approximately 67% of the total area.

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(b) The area enclosed by the curve and vertical lines at ±2 standard deviations from the mean value is approximately 95% of the total area.

(c) The area enclosed by the curve and vertical lines at ±3 standard deviations from the mean value is approximately 99.75% of the total area.

(d) The area enclosed by the curve is proportional to the frequency of the population.

To illustrate a use of these properties, consider a sample of 30 round items drawn at random from a batch of 1000 items produced by a machine. By measurement it is established that the mean diameter of the samples is 0.503 cm and that the standard deviation of the samples is 0.0005 cm. The normal distribution curve theory may be used to predict the reject rate if, say, only items having a diameter of 0.502-0.504 cm are acceptable. The range of items accepted is. Since the standard deviation is 0.0005 cm, this range corresponds to ±2 standard deviations. From (b) above, it follows that 95% of the items are acceptable, that is, that the sample is likely to have 28 to 29 acceptable items and the batch is likely to have 95% of 1000, that is, 950 acceptable items.

This example was selected to give exactly ±2 standard deviations. However, sets of tables are available of partial areas under the standard normal curve, which enable any standard deviation to be related to the area under the curve.

1.14 Differential calculus (Derivatives)

Ify=xnthendydx=nxn1Ify=axnthendydx=anxn1or

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Iff(x)=axnthenf'(x)=anxn1Ify=sinθthendydθ=cosθIfy=cosθthendydθ=sinθIfy=tanθthendydθ=sec2θIfy=cotθthendydθ=cosec2θIfy=secθthendydθ=tanθsecθ=sinθcos2θIfy=cosecθthendydθ=cotθcosecθ=cosθsin2θIfy=sin1xathendydx=1a2x2Ify=cos1xathendydx=1a2x2Ify=tan1xathendydx=aa2+x2Ify=cot1xathendydx=aa2+x2Ify=sec1xathendydx=axx2a2Ify=cosec1xathendydx=axx2a2Ify=exthendydx=exIfy=eaxthendydx=aeaxIfy=axthendydx=axlnaIfy=lnxthendydx=1x

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Product rule

If y = uv where u and v are both functions of x, then dydx=udvdx+vdudxsi110_e

Quotient rule

If y=uvsi111_e where u and v are both functions of x, then dydx=vdudxudvdxv2si112_e

Function of a function

If y is a function of x then dydx=dydu×dudxsi113_e

Successive differentiation

If y = f(x) then its first derivative is written dydxsi114_e or f″(x)

If this expression is differentiated a second time then the second derivative is obtained and is written d2ydx2si115_e or f״(x).si116_e

1.15 Integral calculus (Standard forms)

xndx=xn+1n+1+c(n1)

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Where

C = the constant of integration

axndx=axn1n+1+c(n1)cosθdθ=sinθ+csinθdθ=cosθ+csec2θdθ=tanθ+ccosec2θdθ=cotθ+ctanθsecθdθ=secθ+ccotθcosecθdθ=cosecθ+c

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dxa2x2=sin1xa+cdxa2x2=cos1xa+cadxa2+x2=tan1xa+cadxa2+x2=cot1xa+cadxxx2a2=sec1xa+cadxxx2a2=cosec1xa+cexdx=ex+ceax=eaxa+caxdx=axIna+cdxx=lnx+csinhxdx=coshx+ccoshxdx=sinhx+csech2dx=tanhx+cdxa2+x2=sinh1xa+corln[x+x2+a2a]+cdxx2a2=cosh1xa+corln[x+x2a2a]+cdxa2x2=1atanhxa+cor12aIn(a+x)(ax)+c

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1.15.1 Integration by parts

udv=uvvdu+c

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1.15.2 Definite integrals

The foregoing integrals contain an arbitrary constant ‘c’ and are called indefinite integrals. Definite integrals are those to which limits are applied thus: [x]ba=(b)(a),si121_e therefore:

y=31x2dx=[x33+c]31=[333+c][133+c]=(9+c)[13+c]=823

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Note how the constant of integration (c) is eliminated in a definite integral.

1.16 Binomial theorem

(a+x)n=an+nan1x+n(n1)2!an2x2+n(n1)(n2)3!an3x3++xn

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Where 3! is factorial 3 and equals 1 × 2 × 3.

1.17 Maclaurin’s theorem

f(x)=f(0)+xf(0)+x22!f(0)+……

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1.18 Taylor’s theorem

f(x+h)=f(x)+hf(x)+h22!f(x)+……

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For further information on Engineering Mathematics the reader is referred to the following Pocket Book: Newnes Engineering Mathematics Pocket Book, Third Edition, John Bird, 0750649925

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