- •1. Основные понятия и положения 11
- •2. Центральное растяжение и сжатие стержня 17
- •3. Геометрические характеристики плоских сечений 42
- •4. Кручение 49
- •5. Изгиб стержней 57
- •4. Torsion 208
- •5. Bending of bars 216
- •Introduction 173
- •1. Basic concepts and principles 175
- •2. Tension and compression of a bar 181
- •3. Geometric characteristics of cross sections 202
- •Index 405 введение
- •1. Основные понятия и положения
- •1.1. Задачи сопротивления материалов, основные гипотезы и допущения
- •1.2. Типы нагрузок и деформаций
- •1.3. Определение внутренних усилий методом сечений. Напряжения
- •2. Центральное растяжение и сжатие стержня
- •2.1. Напряжения и продольная деформация при растяжении и сжатии
- •2.2. Закон Гука при растяжении и сжатии
- •2.3. Поперечная деформация при растяжении и сжатии
- •2.4. Диаграмма растяжения низкоуглеродистой стали
- •2.5. Потенциальная энергия деформации при растяжении
- •2.6. Расчеты на прочность при растяжении и сжатии
- •2.7. Статически неопределимые задачи
- •2.8. Напряжения в наклонных сечениях при растяжении (сжатии) в одном направлении
- •2.9. Закон парности касательных напряжений
- •2.10. Определение напряжений в наклонных сечениях при растяжении (сжатии) в двух направлениях
- •2.11. Определение главных напряжений и положения главных площадок
- •2.12. Зависимость между деформациями и напряжениями при плоском и объемном напряженных состояниях (обобщенный закон Гука)
- •2.13. Работа внешних и внутренних сил при растяжении (сжатии). Потенциальная энергия деформации
- •3. Геометрические характеристики плоских сечений
- •3.1. Статический момент площади
- •3.2. Полярный момент инерции
- •3.3. Осевой момент инерции
- •3.4. Момент инерции при параллельном переносе осей
- •3.5. Главные оси и главные моменты инерции
- •4. Кручение
- •4.1. Определение крутящего момента
- •4.2. Определение напряжений в стержнях круглого сечения
- •4.3. Деформации и перемещения при кручении валов
- •4.4. Потенциальная энергия при кручении
- •5. Изгиб стержней
- •5.1. Типы опор балок
- •5.2. Определение опорных реакций
- •5.3. Определение внутренних усилий при изгибе
- •5.4. Правило знаков для изгибающих моментов и поперечных сил
- •5.5. Дифференциальные зависимости при изгибе
- •5.6. Построение эпюр изгибающих моментов и поперечных сил
- •5.7. Определение нормальных напряжений
- •5.8. Условия прочности по нормальным напряжениям
- •5.9. Потенциальная энергия деформации при изгибе
- •5.10. Теорема о взаимности работ. Теорема о взаимности перемещений
- •5.11. Определение перемещений методом Мора
- •6. Теории прочности
- •6.1. Назначение гипотез прочности
- •6.2. Первая гипотеза прочности
- •6.3. Вторая и третья гипотезы прочности
- •6.4. Энергетические гипотезы прочности
- •7. Сложное сопротивление
- •7.1. Изгиб в двух плоскостях (косой изгиб)
- •7.2. Изгиб с растяжением (сжатием)
- •7.3. Внецентренное сжатие (растяжение)
- •7.4. Кручение с изгибом
- •7.5. Кручение с растяжением (сжатием)
- •7.6. Пример расчета вала на изгиб с кручением
- •8. Расчет тонкостенных сосудов
- •9. Расчет сжатых стержней на устойчивость (продольный изгиб)
- •9.1. Устойчивые и неустойчивые формы равновесия
- •9.2. Формула Эйлера для критической силы
- •9.3. Влияние способа закрепления концов стержня на критическую силу
- •9.4. Пределы применимости формулы Эйлера
- •9.5. Эмпирические формулы для определения критических напряжений
- •9.6. Практическая формула для расчета на устойчивость
- •10. Динамическое действие нагрузок
- •10.1. Динамические нагрузки
- •10.2. Вычисление напряжений при равноускоренном движении
- •10.3. Определение перемещений и напряжений при ударе
- •11. Расчет на прочность при напряжениях, циклически изменяющихся во времени (расчет на усталость)
- •11.1. Основные определения
- •11.2. Кривая усталости при симметричном цикле. Предел выносливости
- •11.3. Диаграммы предельных напряжений и амплитуд цикла
- •11.4. Факторы, влияющие на предел выносливости
- •11.5. Определение коэффициента запаса прочности при симметричном цикле
- •11.6. Определение коэффициента запаса прочности при асимметричном цикле напряжений
- •Предположим, что при увеличении нагрузки на деталь отношение Такое нагружение называется простым.
- •11.7. Практические меры повышения сопротивления усталости
- •Практикум Лабораторная работа № 1
- •Введение
- •Установка
- •Порядок выполнения
- •Контрольные вопросы
- •Литература
- •Лабораторная работа № 2
- •Введение
- •Установка
- •Порядок выполнения
- •Введение
- •Контрольные вопросы
- •Литература
- •Лабораторная работа № 3
- •Установка
- •Порядок выполнения
- •Introduction
- •Basic concepts and principles
- •Tasks, main hypothesis and assumptions of the strength of materials
- •1.2. Types of loads and deformations
- •1.3. Determining the internal forces by the method of sections. Stresses
- •2. Tension and compression of a bar
- •2.1. Stresses and a longitudinal deformation in tension and compression
- •2.2. Hooke,s law in tension and compression
- •2.3. The transverse deformation in tension and compression
- •2.4. The tension diagram of the lowcarbon steel
- •2.5. The potential deformation energy in tension
- •2.6. Strength calculation in tension and compression
- •2.7. Statically indeterminate problems
- •2.8. Stresses at inclined sections under tension (compression) in one direction
- •2.9. Law of the shearing stresses couple
- •2.10. Determination of stresses at the inclined sections in tension (compression) in two directions
- •2.11. Determining the principal stresses and the principal planes position
- •2.12. The relation between the deformations and the stresses for the plane and general stresses (a general form of Hook’s law)
- •2.13. The work of the external and internal forces in tension (compression). Strain energy
- •3. Geometric characteristics of cross sections
- •3.1. First moment of an area
- •3.2. Polar moment of inertia
- •3.3. Axial moment of inertia
- •3.4. The moment of inertia at parallel displacement of axis
- •3.5. Principal axes and principal moment of inertia
- •4. Torsion
- •4.1. Determining the twisting moment
- •4.2. Determining the stresses in the round section bar
- •4.3. The deformations and displacements in the shaft torsion
- •4.4. Internal strain energy in torsion
- •5. Bending of bars
- •5.1. Types of the beam support
- •5.2. Determining the support reactions
- •5.3. Determining the internal stresses in bending
- •5.4. The sign rule for the bending moments and the shearing forces
- •5.5. The differential relationships in bending
- •I.E. The intensity of the distributed load is equal to the derivative of the shearing force with respect to the bar section abscissa.
- •I.E. The shearing force is equal to the derivative of the bending moment with respect to the bar section abscissa.
- •I.E. The second derivative of the bending moment with respect to the bar section abscissa is equal to the intensity of the distributed load.
- •5.6. Drawing bending moment and shearing force diagrams
- •5.7. Determining the normal stress
- •5.8. Strength conditions with normal stresses
- •5.9. Strain energy in bending
- •5.10. Betty’s reciprocal theorem. Reciprocal displacement theorem
- •5.11. Determining displacements by Mohr’s method
- •6. Strengtn theory
- •6.1. The purpose of strength hypotheses
- •6.2. The first strength hypothesis
- •6.3. The second and third strength hypotheses
- •6.4. The energy hypotheses of strength
- •7. Combined stress
- •7.1. Bending in two planes (non-uniplanar bending)
- •7.2. Combined axial tension (compression) and bending
- •7.3. Eceentrical tension (compression)
- •7.4. Combined torsion and bending
- •7.5. Combined torsion and compression
- •7.6. Example of the shaft calculation in bending with torsion
- •8. Calculation of the thin-walled vessels
- •9. Stability analysis of the bars in compression (buckling)
- •9.1. Stable and unstable equilibrium forms
- •9.2. Euler’s formula for the critical force
- •9.3. Influence of bar end conditions on the critical force
- •9.4. Applicability limits of of Euler’s formula
- •9.5. Empirical formula for determining the critical stresses
- •9.6. The practical formula for the stability analysis
- •10. Dynamic load action
- •10.1. Dynamic load
- •10.2. Calculating stresses under the uniformly accelerated motion
- •10.3. Determining displacements and stresses under the impact
- •11. Stress analysis under the stresses changing cyclically in time
- •11.1. Basic definitions
- •11.2. Fatigue (Wohler’s) curve under the symmetrical cycle. Fatigue strength
- •11.3. The limit stress diagram and the cycle amplitude
- •11.4. Factors influencing on the fatigue strength
- •11.5. Determining the factor of safety under the symmetrical cycle
- •11.6. Determining the factor of safety under the asymmetrical stress cycle
- •11.7. Practical measures to increase the fatigue strength
- •Practicum Laboratory work № 1
- •Introduction
- •Installation
- •Test specimens
- •Test questions
- •Literature
- •Laboratory work № 2
- •Introduction
- •Installation
- •Test questions
- •Literature
- •Laboratory work № 3
- •Introduction
- •Installation
- •Individual task report
- •Test questions
- •Literature
- •Англо-русский терминологический словарь
- •Список фамилий ученых
- •Greek alphabet
- •Сокращения
- •Единицы измерения
- •Список наиболее употребительных знаков
- •Список использованной литературы
- •Алфавитный указатель
- •Сопротивление материалов
- •625000, Тюмень, ул. Володарского, 38.
- •625039, Г. Тюмень, ул. Киевская, 52
11.4. Factors influencing on the fatigue strength
The experiences show that the fatigue strength is subjected by the essential influence of the following factors: the stress concentration, the detail cross section dimensions, the surface condition, the character of the technological treatment and others.
Consider them more detaily.
The influence of the stress concentration. The sharp detail shape change, holes, recesses, cuts and so on decrease the fatigue strength considerably in comparison with the fatigue strength for the smooth cylindrical specimens.
This decreasing is considered by the effective stress concentration coefficient which is determined by an experimental way.
For that we
take two similar specimen series (10 specimen in each one) but the
first one is without the stress concentration and the second one has
the concentration and determines the fatigue strengths under the
symmetrical cycle for the specimens without the stress concentration
and for the specimens with the stress concentration
The relation
(11.9)
determines
the effective
stress concentration coefficient.
The experiences show that this coefficient differs from the
theoretical
because the first depends not only on the detail shape but on the
material too.
The values
are represented in the reference books. The values of the effective
concentration coefficient in bending for the stepped shafts with the
correlation
and the transition of the circular radius fillet r
is given in Fig. 11.8 as an example. These data were obtained under
the specimen test of d
=30÷50 mm for steel with the limit strength
and 1200 MPa. To compare the theoretical concentration coefficient
diagram ασ
is presented (by the dotted line).
Fig. 11.8. Fig. 11.9.
The value
of the concentration coefficients in torsion
and
are given in Fig. 11.9 and in Fig. 11.10 - in tension-compression. To
determine the effective concentration coefficients under other
correlations
the formula
must be used
(11.10)
Fig. 11.10. Fig. 11.11.
where
is the effective concentration coefficient corresponding to the
correlation
ξ is the correction coefficient determined by Fig. 11.11 thereby the
curve 1 gives the value ξ in bending, the curve 2 – in torsion.
The values
and
for the shafts with the key slots (one or two) are represented below
, MPа |
|
500 |
750 |
1000 |
|
|
|
1,5 |
1,75 |
2,0 |
|
|
600 |
700 |
800 |
900 |
1000 |
|
1,5 |
1,6 |
1,7 |
1,8 |
1,9 |
In the
cases when the experience data to determine the effective stress
concentration coefficient are missing and the known values of the
theoretical stress concentration coefficient are missing, the known
values of the theoretical stress concentration coefficient can be
used to determine
by the following empirical formula:
where q is the so-called coefficient of the material sensitivity to
the stress concentrations
For
the high-strength alloy steel the value q
is near to one. For the constructional steel on average q=0,60,8,
whereby for more durable steels it corresponds to larger values q.
For the grey pig iron the value q
is near to zero. In other words the grey pig iron is insensitive to
the stress concentration. More details about q
for steel are given in Fig. 11.12.
Fig. 11.12.
The influence of the absolute detail cross-section dimensions. The experiences show that the more absolute detail cross section dimensions are, the less the fatigue strength is.
The relation of the details fatigue strength of the diameter d to the fatigue strength of the laboratory specimen of the diameter d0=6÷10 mm. is called the influence coefficient of the absolute cross section dimensions:
(11.11)
for normal stresses. The influence coefficient of the absolute cross section dimensions can also be determined for the specimens with the stress concentration. In this case we have
(11.12)
Thereby
both the detail of the dimension d
and the specimen of the dimension
must have a geometrically similar configuration.
The value diagram is given in Fig. 11.13.
The curve 1 corresponds to the detail from the carbon steel without the concentrator, the curve 2 – to the detail from the alloy steel under the concentrator absence and from the carbon steel under the concentrator presence, the curve 3 – to the detail from the alloy steel under the concentrator presence, the curve 4 – for any steel under the highly large stress concentration (for example under the concentrator of the slot type).
Because of
absence of the sufficient quantity of the experience data about the
coefficients
(in torsion) one can approximately accept that
It is to be
noted that the experience data to determine
are insufficient.
The surface quality influence and the hardness of the surface layer. The experiences show that the rough treatment of the detail surface decreases the fatigue strength. The surface quality influence is connected with the change of the microgeometry (the roughness) and the metal condition in the surface layer that in its turn depends on the mechanical treatment way.
Fig. 11.13. Fig. 11.14.
To
appreciate the surface quality influence on the fatigue strength it
is necessary to introduce the coefficient
called by the quality
coefficient
of the surface and it is equal to the relation of the specimen
fatigue strength with the given surface roughness
to the specimen fatigue strength with the surface which is not
rougher than
(11.13)
The value
diagram
depending on the limit strength
of steel and the surface treatment form is in Fig.11.14.
Thereby the curves correspond to the following surface treatment form:
1 – polishing, 2 – grinding, 3 – precision turning, 4 – rough turning, 5 – scale presence.
Different
ways of the surface hardness (strain-hardness, cementing,
nitrogening, the surface hardening by the high-frequency current and
so on) increase strongly the fatigue strength value. It is taken into
account by introducing the hardness surface influence coefficient
The fatigue strength of the machine details can be increased in 2-3
times by the details hardness surface way.
The
coefficient values
can find in the reference book.
