Technical reference book on technical mechanics. Download textbook on technical mechanics


Arkusha A.I. Guide to solving problems in theoretical mechanics, 1971
(8.5Mb) - Download
Arkusha A.I., Frolov M.I. Technical mechanics, 1983
(130Mb) - Download
Bat M.I., Dzhanelidze G.Yu., Kelzon A.S. Theoretical mechanics in examples and problems,
Vol.1 - Statics and kinematics, 1967 (7 MB) - Download
Vol.2-Dynamics, 1966 (7.1 MB) - Download
Berezova O.A., Drushlyak G.E., Solodovnkov R.V. Theoretical mechanics,
Collection of problems, 1980. (7.2 MB) - Download
Butenin N.V., Lunts Ya.L., Merkin D.R. Theoretical mechanics course,
Vol.1 - Statics and kinematics, 1979 (2.8 MB) - Download
Gernet M.M. Theoretical mechanics course, 1973
(5.6Mb) - Download
Dievsky V.A., Malysheva I.A. Theoretical mechanics. Collection of tasks, 2009
(25Mb) - Download
Ishlinsky A.Yu. Theoretical mechanics. Letter designations of quantities, 1980
(0.3Mb) - Download
Kepe O.E. Collection of short problems on theoretical mechanics, 1989
(8MB) - Download
Kirsanov M.N. Reshebnik. Theoretical mechanics, 2002
(2.8Mb) - Download
, 1986 and later years of publication.
(6MB) - Download
Meshchersky I.V. Collection of problems on theoretical mechanics, 1975
(9Mb) - Download
Loytsyansky L.G., Lurie A.I. Theoretical mechanics course,
Vol.1 - Statics and kinematics, 1982 (10.3 MB) - Download
Vol.2-Dynamics, 1983 (12.9 MB) - Download
Novozhilov I.M., Zatsepin M.F. Typical computer-based calculations for theoretical mechanics.,
1986 (2.2 MB) - Download
Olofinskaya V.P. Technical mechanics, 2007
(10Mb) - Download
Setkov V.I. Collection of problems on technical mechanics., 2003
(7Mb) - Download
Starzhinsky V.M. Theoretical mechanics. Short course on the full program of technical colleges, 1980
(0.8Mb) - Download
Targ S.M. Short course in theoretical mechanics, 1986
(6.5Mb) - Download
Theoretical mechanics. Methodological instructions and test assignments for part-time students of construction, transport, mechanical engineering and instrument-making specialties of higher educational institutions. Ed. Targa S.M. , ed. 3, 1982
(1.9Mb) - Download
Theoretical mechanics: Guidelines and test assignments for part-time students of thermal power, mining, metallurgical, electrical instrument making and automation and technological specialties, as well as specialties of geological, electrical engineering, electronic engineering and automation, chemical technology and engineering economic higher educational institutions. Ed. Targa S.M. , ed. 3, 1983
(2.8Mb) - Download
Theoretical mechanics: Guidelines and test assignments for part-time students of energy, mining, metallurgical, electrical instrument making and automation, technological specialties, as well as geological, electrical, electronic engineering and automation, chemical-technological and engineering-economic specialties of universities. Ed. Targa S.M. , ed. 4, 1988
(1.1Mb) -

I couldn’t find a textbook on technical mechanics!

So I decided to post it for those in need! Below is a description of the textbooks in more detail

4 textbooks on technical mechanics, download for free, without SMS and registration:

1. Technical mechanics. A course of lectures with options for practical and test tasks (Olofinskaya V.P.) (DJVU format)

2. Technical mechanics Portaev L.P. (DJVU format)

3. Collection of problems in technical mechanics V.I. Setkov (PDF format)

4. Collection of problems on technical mechanics.

DJVUCNTL program for opening DJVU files (installed on XP without problems)

File type WinRAR archive.

OS: Windows All

Russian language

License: Freeware

Size: 35.0 MB

Technical mechanics. A course of lectures with options for practical and test tasks

Olofinskaya V.P.

Publisher: Forum

Year of publication: 2012

Number of pages: 348

Russian language

Format: DJVU

Size: 5.2 MB

The proposed book presents a course of lectures on two sections of technical mechanics - “Theoretical Mechanics” and “Strength of Materials”. Each section contains options for practical exercises on main topics. This textbook can be used for independent study of the discipline "Technical Mechanics", in particular during distance learning, as well as in preparation for exams and tests.

The textbook is written in accordance with the state educational standard, intended for students of technical schools and colleges, and can also be recommended for university students.

Publisher: Stroyizdat

Genre: Construction, repair, Education, Mechanics

The main axioms of statics when forces act on a completely rigid body and the laws of plane movement of a point and a rigid body are presented. Methods for calculating elastically deformable conventional systems operating under the criteria of tension, shear, torsion, bending and their general effects are presented. Methods are given for calculating multi-span statically determinate and indeterminate beams and frames, three-hinged arches, flat trusses, and retaining walls. The theoretical provisions of the material being explained will be accompanied by examples from construction practice.

Publisher: Academy

Genre: Education, Mechanics

Tasks for calculation-analytical and calculation-graphical work in all sections of the technical mechanics course are given.

Guide to solving problems in theoretical mechanics.

Publisher: Higher School

Genre: Education, Mechanics

The manual contains selected standard problems throughout the course of theoretical mechanics, uniform guidelines and recommendations for solving problems. Problem solving will often be accompanied by thorough explanations. However, many problems are solved using several techniques. The manual is intended for students of correspondence and evening technical schools and has the task of giving them support in acquiring initial skills in solving problems in theoretical mechanics. The manual is used, among other things, by students of full-time technical schools.

Download free archiver

Problem solving

Determination of beam support reactions,

Determination of support and pinching reactions,

5th ed., rev. - M.: 2002. - 336 p.

The manual contains systematically selected typical problems throughout the course, general guidelines and tips for solving problems. Problem solving is accompanied by detailed explanations. Many problems are solved in several ways.

For students of mechanical engineering specialties of secondary specialized educational institutions. May be useful for students of technical universities.

Format: djvu (2002 , 5th ed., revised, 336 pp.)

Size: 6.2 MB

Download: yandex.disk

Format: pdf(1976 , 3rd ed., revised, 288 pp.)

Size: 20.5 MB

Download: yandex.disk


Content
Preface
Chapter I. Operations on vectors
§ 1-1. Vector addition. Rules for parallelogram, triangle and polygon
§ 2-1. Decomposition of a vector into two components. Vector difference
§ 3-1. Addition and decomposition of vectors in a graphic-analytical way
§ 4-1. Projection method. Projection of a vector onto an axis. Projections of a vector onto two mutually perpendicular axes. Determination of a vector sum by the projection method
Section one Statics
Chapter II. Plane system of converging forces.
§ 5-2. Addition of two forces
§ 7-2. Polygon of forces. Determination of the resultant of converging forces
§ 8-2. Equilibrium of Converging Forces
§ 9-2. Equilibrium of three non-parallel forces
Chapter III. Arbitrary flat system of forces
§ 10-3. Moment of a couple of forces. Addition of force pairs. Equilibrium of force pairs
§ 11-3. Moment of force about a point
§ 12-3. Determination of the resultant arbitrary plane system of forces
§ 13-3. Varignon's theorem
§ 14-3. Equilibrium of an arbitrary plane system of forces
§ 15-3. Equilibrium taking into account friction forces
§ 16-3. Articulated systems
§ 17-3. Statically definable trusses. Methods for cutting nodes and through sections
Chapter IV. Spatial system of forces
§ 18-4. Force parallelepiped rule
§ 19-4. Projection of force onto three mutually perpendicular axes. Determination of the resultant system of spatial forces applied to a point
§ 20-4. Equilibrium of a spatial system of converging forces
§ 21-4. Moment of force about the axis
§ 22-4. Equilibrium of an arbitrary spatial system of forces
Chapter V. Center of gravity........................
§ 23-5. Determining the position of the center of gravity of a body composed of thin homogeneous rods
§ 24-5. Determining the position of the center of gravity of figures composed of plates
§ 25-5. Determination of the position of the center of gravity of sections composed of standard rolled profiles
§ 26-5. Determining the position of the center of gravity of a body composed of parts having a simple geometric shape
Section two Kinematics
Chapter VI. Kinematics of a point
§ 27-6. Uniform linear motion of a point
§ 28-6. Uniform curvilinear movement of a point
§ 29-6. Uniform motion of a point
§ 30-6. Uneven movement of a point along any trajectory
§ 31-6. Determination of the trajectory, speed and acceleration of a point if the law of its motion is given in coordinate form
§ 32-6. Kinematic method for determining the radius of curvature of a trajectory
Chapter VII. Rotational motion of a rigid body
§ 33-7. Uniform rotational movement
§ 34-7. Equally alternating rotational motion
§ 35-7. Uneven rotational movement
Chapter VIII. Complex movement of point and body
§ 36-8. Addition of the movements of a point when the portable and relative movements are directed along the same straight line
§ 37-8. Addition of the movements of a point when the portable and relative movements are directed at an angle to each other
§ 38-8. Plane-parallel body motion
Chapter IX. Elements of kinematics of mechanisms
§ 39-9. Determination of gear ratios of various gears
§ 40-9. Determination of gear ratios of the simplest planetary and differential gears
Section three Dynamics
Chapter X. Motion of a material point
§ 41-10. Basic law of point dynamics
§ 42-10. Application of d'Alembert's principle to solving problems involving the rectilinear motion of a point
§ 43-10. Application of d'Alembert's principle to solving problems involving the curvilinear motion of a point
Chapter XI. Work and power. Efficiency
§ 44-11. Work and power in forward motion
§ 45-11. Rotational work and power
Chapter XII. Basic theorems of dynamics
§ 46-12. Problems involving translational movement of the body
§ 47-12. Problems involving rotational movement of the body

The manual contains the basic concepts and terms of one of the main disciplines of the subject block “Technical Mechanics”. This discipline includes such sections as “Theoretical Mechanics”, “Strength of Materials”, “Theory of Mechanisms and Machines”.

The methodological manual is intended to assist students in self-studying the course “Technical Mechanics”.

Theoretical mechanics 4

I. Statics 4

1. Basic concepts and axioms of statics 4

2. System of converging forces 6

3. Flat system of arbitrarily located forces 9

4. The concept of a farm. Truss calculation 11

5. Spatial system of forces 11

II. Kinematics of a point and a rigid body 13

1. Basic concepts of kinematics 13

2. Translational and rotational motions of a rigid body 15

3. Plane-parallel motion of a rigid body 16

III. Dynamics of point 21

1. Basic concepts and definitions. Laws of dynamics 21

2. General theorems for the dynamics of a point 21

Strength of materials22

1. Basic concepts 22

2. External and internal forces. Section method 22

3. The concept of voltage 24

4. Tension and compression of straight timber 25

5. Shear and crushing 27

6. Torsion 28

7. Transverse bend 29

8. Longitudinal bending. The essence of the phenomenon of longitudinal bending. Euler's formula. Critical voltage 32

Theory of mechanisms and machines 34

1. Structural analysis of mechanisms 34

2. Classification of flat mechanisms 36

3. Kinematic study of flat mechanisms 37

4. Cam mechanisms 38

5. Gear mechanisms 40

6. Dynamics of mechanisms and machines 43

Bibliography45

THEORETICAL MECHANICS

I. Statics

1. Basic concepts and axioms of statics

The science of the general laws of motion and equilibrium of material bodies and the resulting interactions between bodies is called theoretical mechanics.

Static is a branch of mechanics that sets out the general doctrine of forces and studies the conditions of equilibrium of material bodies under the influence of forces.

Absolutely solid body A body is called the distance between any two points of which always remains constant.

A quantity that is a quantitative measure of the mechanical interaction of material bodies is called by force.

Scalar quantities- these are those that are completely characterized by their numerical value.

Vector quantities – These are those that, in addition to their numerical value, are also characterized by direction in space.

Force is a vector quantity(Fig. 1).

Strength is characterized by:

– direction;

– numerical value or module;

– point of application.

Straight DE, along which the force is directed, is called line of action of force.

The set of forces acting on any solid body is called system of forces.

A body that is not attached to other bodies, to which any movement in space can be imparted from a given position, is called free.

If one system of forces acting on a free rigid body can be replaced by another system without changing the state of rest or motion in which the body is located, then such two systems of forces are called equivalent.

The system of forces under the influence of which a free rigid body can be at rest is called balanced or equivalent to zero.

Resultant – this is the force that alone replaces the action of a given system of forces on a solid body.

A force equal to the resultant in magnitude, directly opposite to it in direction and acting along the same straight line is called balancing force.

External are the forces acting on the particles of a given body from other material bodies.

Internal are the forces with which the particles of a given body act on each other.

A force applied to a body at any one point is called concentrated.

Forces acting on all points of a given volume or a given part of the surface of a body are called distributed.

Axiom 1. If two forces act on a free absolutely rigid body, then the body can be in equilibrium if and only if these forces are equal in magnitude and directed along the same straight line in opposite directions (Fig. 2).

Axiom 2. The action of one system of forces on an absolutely rigid body will not change if a balanced system of forces is added to it or subtracted from it.

Corollary of the 1st and 2nd axioms. The action of a force on an absolutely rigid body will not change if the point of application of the force is moved along its line of action to any other point of the body.

Axiom 3 (parallelogram of forces axiom). Two forces applied to a body at one point have a resultant applied at the same point and represented by the diagonal of a parallelogram built on these forces, as on the sides (Fig. 3).

R = F 1 + F 2

Vector R, equal to the diagonal of a parallelogram built on vectors F 1 and F 2, called geometric sum of vectors.

Axiom 4. With any action of one material body on another, there is a reaction of the same magnitude, but opposite in direction.

Axiom 5(hardening principle). The equilibrium of a changing (deformable) body under the influence of a given system of forces will not be disturbed if the body is considered hardened (absolutely solid).

A body that is not attached to other bodies and can make any movement in space from a given position is called free.

A body whose movements in space are prevented by some other bodies fastened or in contact with it is called unfree.

Everything that limits the movement of a given body in space is called communication.

The force with which a given connection acts on a body, preventing one or another of its movements, is called bond reaction force or communication reaction.

The communication reaction is directed in the direction opposite to the one where the connection prevents the body from moving.

Axiom of connections. Any unfree body can be considered as free if we discard the connections and replace their action with the reactions of these connections.

2. System of converging forces

Converging forces are called whose lines of action intersect at one point (Fig. 4a).

The system of converging forces has resultant, equal to the geometric sum (principal vector) of these forces and applied at the point of their intersection.

Geometric sum, or main vector several forces, is depicted by the closing side of a force polygon constructed from these forces (Fig. 4b).

2.1. Projection of force onto the axis and onto the plane

Projection of force onto the axis is a scalar quantity equal to the length of the segment taken with the appropriate sign, enclosed between the projections of the beginning and end of the force. The projection has a plus sign if the movement from its beginning to the end occurs in the positive direction of the axis, and a minus sign if in the negative direction (Fig. 5).

Projection of force on the axis is equal to the product of the modulus of the force and the cosine of the angle between the direction of the force and the positive direction of the axis:

F X = F cos.

Projection of force onto a plane is called the vector enclosed between the projections of the beginning and end of the force onto this plane (Fig. 6).

F xy = F cos Q

F x = F xy cos= F cos Q cos

F y = F xy cos= F cos Q cos

Projection of the sum vector on any axis is equal to the algebraic sum of the projections of the summands of the vectors onto the same axis (Fig. 7).

R = F 1 + F 2 + F 3 + F 4

R x = ∑F ix R y = ∑F iy

To balance a system of converging forces It is necessary and sufficient that the force polygon constructed from these forces be closed - this is a geometric equilibrium condition.

Analytical equilibrium condition. For the system of converging forces to be in equilibrium, it is necessary and sufficient that the sum of the projections of these forces on each of the two coordinate axes be equal to zero.

F ix = 0 ∑F iy = 0 R =

2.2. Three Forces Theorem

If a free solid body is in equilibrium under the action of three non-parallel forces lying in the same plane, then the lines of action of these forces intersect at one point (Fig. 8).

2.3. Moment of force relative to the center (point)

Moment of force relative to the center is called a quantity equal to taken with the corresponding sign, the product of the force modulus and the length h(Fig. 9).

M = ± F· h

Perpendicular h, lowered from the center ABOUT to the line of action of the force F, called force arm F relative to the center ABOUT.

The moment has a plus sign, if the force tends to rotate the body around the center ABOUT counterclockwise, and minus sign- if clockwise. Educational - methodical allowanceBook >> Philosophy

Educational allowance includes 10 ... create a completely new science - classical mechanics. Classical Mechanics– the science of the laws of motion... of optoelectronic devices, the field of scientific and technical use). 8.What technologies are used in...

  • Technical operation of vehicles in agriculture

    Study Guide >> Transport

    ... : Yu.G. Korepanov T38 Technical operation of vehicles in agriculture: educationally-methodical allowance/ Yu.G. Korepanov. ... mechanics. The purpose of the course project: To deepen and consolidate theoretical and practical knowledge in the subject " Technical ...

  • Production technical infrastructure of TMO service enterprises

    Course work >> Transport

    For relax; masters room ( mechanics); smoking rooms For storing technological clothes... Educational-methodical allowance. – Tyumen: TyumGNGU, 1996. – 245 p. Napolsky G. M. Technological design of motor transport enterprises and stations technical ...

  • Educational-introductory practice at KamchatSTU

    Practice report >> Pedagogy

    Ship power plants, navigation, theoretical Mechanics, physical education, refrigeration machines and... methodological and other works of department staff. Preparation of textbooks, educational benefits and other manuals. Propaganda of scientific and technical ...

  • Latest materials in the section:

    Electrical diagrams for free
    Electrical diagrams for free

    Imagine a match that, after being struck on a box, flares up, but does not light up. What good is such a match? It will be useful in theatrical...

    How to produce hydrogen from water Producing hydrogen from aluminum by electrolysis
    How to produce hydrogen from water Producing hydrogen from aluminum by electrolysis

    “Hydrogen is only generated when needed, so you can only produce as much as you need,” Woodall explained at the university...

    Artificial gravity in Sci-Fi Looking for the truth
    Artificial gravity in Sci-Fi Looking for the truth

    Problems with the vestibular system are not the only consequence of prolonged exposure to microgravity. Astronauts who spend...