Important physical formulas. Buy a higher education diploma inexpensively

Important physical formulas.  Buy a higher education diploma inexpensively
Important physical formulas. Buy a higher education diploma inexpensively

If kinematics only describes the movement of bodies, then dynamics studies the causes of this movement under the influence of forces acting on the body.

Dynamics– a branch of mechanics that studies the interactions of bodies, the causes of movement and the type of movement that occurs. Interaction- a process during which bodies exert mutual influence on each other. In physics, all interactions are necessarily paired. This means that bodies interact with each other in pairs. That is, every action necessarily generates a reaction.

Force is a quantitative measure of the intensity of interaction between bodies. Force causes a change in the speed of the body as a whole or its parts (deformation). Force is a vector quantity. The straight line along which the force is directed is called the line of action of the force. The force is characterized by three parameters: the point of application, the module ( numerical value) and direction. In the International System of Units (SI), force is measured in Newtons (N). Calibrated springs are used to measure forces. Such calibrated springs are called dynamometers. Strength is measured by the stretch of a dynamometer.

A force that has the same effect on a body as all the forces acting on it taken together is called resultant force. It is equal to the vector sum of all forces acting on the body:

To find the vector sum of several forces, you need to make a drawing, where you correctly draw all the forces and their vector sum, and using this drawing, using knowledge from geometry (mainly the Pythagorean theorem and the cosine theorem), find the length of the resulting vector.

Types of forces:

1. Gravity. Applied to the center of mass of the body and directed vertically downwards (or what is the same: perpendicular to the horizon line), and is equal to:

Where: g- acceleration free fall, m- body mass. Don’t get confused: the force of gravity is perpendicular to the horizon, and not to the surface on which the body lies. Thus, if the body lies on an inclined surface, the force of gravity will still be directed straight down.

2. Friction force. It is applied to the surface of contact of the body with the support and is directed tangentially to it in the direction opposite to the one where other forces are pulling or trying to pull the body.

3. Force viscous friction(medium resistance force). Occurs when a body moves in a liquid or gas and is directed against the speed of movement.

4. Ground reaction force. Acts on the body from the side of the support and is directed perpendicular to the support from it. When a body rests on an angle, the reaction force of the support is directed perpendicular to the surface of the body.

5. Thread tension force. Directed along the thread away from the body.

6. Elastic force. Occurs when the body is deformed and is directed against the deformation.

Pay attention and note for yourself the obvious fact: if the body is at rest, then the resultant of the forces is zero.

Force projections

In most dynamics problems, more than one force acts on a body. In order to find the resultant of all forces in this case, you can use the following algorithm:

  1. Let's find the projections of all forces onto the OX axis and sum them up, taking into account their signs. So we get the projection of the resultant force on the OX axis.
  2. Let's find the projections of all forces onto the OY axis and sum them up, taking into account their signs. This way we get the projection of the resultant force onto the OY axis.
  3. The resultant of all forces will be found according to the formula (Pythagorean theorem):

At the same time, please note Special attention that:

  1. If the force is perpendicular to one of the axes, then the projection onto this axis will be equal to zero.
  2. If, when projecting a force onto one of the axes, the sine of the angle “pops up,” then when projecting the same force onto another axis there will always be a cosine (of the same angle). When projecting, it is easy to remember which axis the sine or cosine will be on. If the angle is adjacent to the projection, then when the force is projected onto this axis there will be a cosine.
  3. If the force is directed in the same direction as the axis, then its projection onto this axis will be positive, and if the force is directed in the direction opposite to the axis, then its projection onto this axis will be negative.

Newton's laws

The laws of dynamics, which describe the influence of various interactions on the motion of bodies, were in one of their simplest forms first clearly and clearly formulated by Isaac Newton in the book “Mathematical Principles of Natural Philosophy” (1687), therefore these laws are also called Newton’s Laws. Newton's formulation of the laws of motion is valid only in inertial systems reference (ISO). ISO is a reference system associated with a body moving by inertia (uniformly and rectilinearly).

There are other restrictions on the applicability of Newton's laws. For example, they give accurate results only as long as they are applied to bodies whose speeds are much less than the speed of light, and whose sizes significantly exceed the sizes of atoms and molecules (a generalization of classical mechanics to bodies moving at an arbitrary speed is relativistic mechanics, and to bodies , whose dimensions are comparable to atomic ones - quantum mechanics).

Newton's first law (or law of inertia)

Formulation: In ISO, if no forces act on the body or the action of the forces is compensated (that is, the resultant of the forces is zero), then the body maintains a state of rest or uniform linear motion.

The property of bodies to maintain their speed in the absence of the action of other bodies on it is called inertia. Therefore, Newton's first law is called the law of inertia. So, the reason for a change in the speed of movement of a body as a whole or its parts is always its interaction with other bodies. To quantitatively describe changes in the movement of a body under the influence of other bodies, it is necessary to introduce a new quantity - body mass.

Weight is a property of a body that characterizes its inertia (the ability to maintain a constant speed. In the International System of Units (SI), body mass is measured in kilograms (kg). Body mass is a scalar quantity. Mass is also a measure of the amount of matter:

Newton's second law - the fundamental law of dynamics

When starting to formulate the second law, we should remember that two new physical quantities are introduced in dynamics - body mass and force. The first of these quantities – mass – is a quantitative characteristic of the inert properties of a body. It shows how the body reacts to external influences. The second - force - is a quantitative measure of the action of one body on another.

Formulation: The acceleration acquired by a body in ISO is directly proportional to the resultant of all forces acting on the body, and inversely proportional to the mass of this body:

However, when solving problems in dynamics, it is advisable to write Newton’s second law in the form:

If several forces simultaneously act on a body, then the force in the formula expressing Newton’s second law must be understood as the resultant of all forces. If the resultant force is zero, then the body will remain in a state of rest or uniform linear motion, because the acceleration will be zero (Newton's first law).

Newton's third law

Formulation: In ISO, bodies act on each other with forces equal in magnitude and opposite in direction, lying on the same straight line and having the same physical nature:

These forces are applied to different bodies and therefore cannot balance each other. Please note that you can only add forces that simultaneously act on one of the bodies. When two bodies interact, forces arise that are equal in magnitude and opposite in direction, but they cannot be added, because they are attached to different bodies.

Algorithm for solving dynamics problems

Dynamics problems are solved using Newton's laws. The following procedure is recommended:

1. Having analyzed the condition of the problem, establish which forces act on which bodies;

2. Show in the figure all forces in the form of vectors, that is, directed segments applied to the bodies on which they act;

3. Choose a reference system, one useful coordinate axis direct in the same direction as the acceleration of the body in question, and the other - perpendicular to the acceleration;

4. Write Newton's II law in vector form:

5. Go to the scalar form of the equation, that is, write down all its terms in the same order in projections onto each of the axes, without vector signs, but taking into account that the forces directed against the selected axes will have negative projections, and thus on the left side Newton's law they will be subtracted, not added. The result will be expressions like:

6. Create a system of equations, supplementing the equations obtained in the previous paragraph, if necessary, with kinematic or other simple equations;

8. If several bodies are involved in the movement, the analysis of forces and recording of equations is carried out for each of them separately. If a dynamics problem describes several situations, then a similar analysis is performed for each situation.

When solving problems, also consider the following: the direction of the body's velocity and the resultant forces do not necessarily coincide.

Elastic force

Deformation refers to any change in the shape or size of the body. Elastic deformations are those in which the body completely restores its shape after the cessation of the deforming force. For example, after the load was removed from the spring, its undeformed length did not change. When a body undergoes elastic deformation, a force arises that tends to restore the previous size and shape of the body. It is called elastic force. The simplest type of deformation is unilateral tensile or compression deformation.

For small deformations, the elastic force is proportional to the deformation of the body and is directed in the direction opposite to the direction of movement of the body particles during deformation:

Where: k– body rigidity, X– the amount of stretching (or compression, deformation of the body), it is equal to the difference between the final and initial length of the deformed body. And it is not equal to either its initial or final length separately. Rigidity does not depend either on the magnitude of the applied force or on the deformation of the body, but is determined only by the material from which the body is made, its shape and dimensions. In the SI system, stiffness is measured in N/m.

The statement about the proportionality of the force of elasticity and deformation is called Hooke's law. Spiral springs are often used in technology. When springs are stretched or compressed, elastic forces arise, which also obey Hooke's law. The coefficient k is called the spring stiffness. Within the limits of applicability of Hooke's law, springs are capable of greatly changing their length. Therefore, they are often used to measure forces. A spring whose tension is calibrated in units of force is called a dynamometer.

Thus, each specific body (not material) has its own rigidity and it does not change for a given body. Thus, if in a dynamics problem you stretched the same spring several times, you must understand that its stiffness was the same in all cases. On the other hand, if in the problem there were several springs of different sizes, but, for example, they were all steel, then nevertheless they will all have different stiffnesses. Since stiffness is not a material characteristic, it cannot be found in any tables. The stiffness of each specific body will either be given to you in the dynamics problem, or its value should be the subject of some additional research when solving this problem.

When compressed, the elastic force prevents compression, and when stretched, it prevents stretching. Let's also consider how we can express the stiffness of several springs connected in a certain way. When connecting springs in parallel overall coefficient stiffness is calculated by the formula:

When connecting springs in series The overall stiffness coefficient can be found from the expression:

Body weight

The force of gravity with which bodies are attracted to the Earth must be distinguished from the weight of the body. The concept of weight is widely used in Everyday life in the wrong sense, weight means mass, but this is not so.

Body weight is the force with which the body acts on a support or suspension. Weight is a force, which, like all forces, is measured in newtons (and not in kilograms), and is designated P. In this case, it is assumed that the body is motionless relative to the support or suspension. According to Newton's third law, weight is often equal to either the reaction force of the support (if the body is lying on a support), or the tension force of a thread or the elastic force of a spring (if the body is hanging on a thread or spring). Let's make a reservation right away - weight is not always equal to gravity.

Weightlessness is a state that occurs when body weight is zero. In this state, the body does not act on the support, but the support acts on the body.

An increase in body weight caused by accelerated movement of a support or suspension is called overload. Overload is calculated using the formula:

Where: P– weight of the body experiencing overload, P 0 – weight of the same body at rest. Overload is a dimensionless quantity. This is clearly seen from the formula. Therefore, do not believe science fiction writers who in their books measure it in g.

Remember that weight is never shown in pictures. It is simply calculated using formulas. And the pictures depict the tension force of the thread or the reaction force of the support, which, according to Newton’s third law, are numerically equal to the weight, but are directed in the other direction.

So, let us note again three essential important points which are often confused:

  • Even though the weight and ground reaction force are equal in magnitude and opposite in direction, their sum is not zero. These forces cannot be added at all, because they are applied to different bodies.
  • Body mass and body weight should not be confused. Mass is a characteristic of the body, measured in kilograms; weight is the force exerted on a support or suspension, measured in Newtons.
  • If you need to find the weight of a body R, then first find the ground reaction force N, or thread tension T, and according to Newton's third law, the weight is equal to one of these forces and opposite in direction.

Friction force

Friction- one of the types of interaction between bodies. It occurs in the area of ​​​​contact of two bodies during their relative movement or an attempt to cause such movement. Friction, like all other types of interaction, obeys Newton’s third law: if a friction force acts on one of the bodies, then a force of the same magnitude, but directed in the opposite direction, also acts on the second body.

Dry friction that occurs when bodies are at relative rest is called static friction. Static friction force always equal in magnitude to the external causing force and directed in the opposite direction to it. The static friction force cannot exceed a certain maximum value, which is determined by the formula:

Where: μ is a dimensionless quantity called the coefficient of static friction, and N– ground reaction force.

If external force greater than the maximum value of the friction force, relative slip occurs. The friction force in this case is called sliding friction force. It is always directed in the direction opposite to the direction of movement. The sliding friction force can be considered equal to the maximum static friction force.

Proportionality factor μ therefore also called sliding friction coefficient. Friction coefficient μ – dimensionless quantity. The friction coefficient is positive and less than unity. It depends on the materials of the contacting bodies and on the quality of processing of their surfaces. Thus, the friction coefficient is a certain specific number for each specific pair of interacting bodies. You won't be able to find it in any tables. For you, it must either be given in the problem, or you yourself must find it while solving it from some formulas.

If, as part of solving a problem, you get a friction coefficient greater than one or negative, you are solving this problem in dynamics incorrectly.

If the problem statement asks to find the minimum force under the influence of which movement begins, then they look for the maximum force under the influence of which movement does not yet begin. This makes it possible to equate the acceleration of bodies to zero, which means significantly simplifying the solution of the problem. In this case, the friction force is assumed to be equal to its maximum value. In this way, the moment is considered at which an increase in the desired force by a very small amount will immediately cause movement.

Features of solving problems in dynamics with several bodies

Bound bodies

An algorithm for solving problems in dynamics in which several bodies connected by threads are considered:

  1. Make a drawing.
  2. Write down Newton's second law for each body separately.
  3. If the thread is inextensible (and this will be the case in most problems), then the accelerations of all bodies will be identical in magnitude.
  4. If the thread is weightless, the block has no mass, and there is no friction in the axis of the block, then the tension force is the same at any point of the thread.

Movement of the body through the body

In problems of this type, it is important to take into account that the friction force on the surface of contacting bodies acts on both the upper body and the lower body, that is, friction forces occur in pairs. At the same time, they are aimed at different sides and have equal magnitude, determined by the weight of the upper body. If the lower body also moves, then it must be taken into account that it is also affected by the friction force from the support.

Rotational movement

When a body moves in a circle, regardless of the plane in which the movement occurs, the body will move with centripetal acceleration, which will be directed towards the center of the circle along which the body is moving. However, the concept of a circle should not be taken literally. A body can only move through a circular arc (for example, move along a bridge). In all problems of this type, one of the axes is necessarily selected in the direction of centripetal acceleration, i.e. to the center of a circle (or arc of a circle). It is advisable to direct the second axis perpendicular to the first. Otherwise, the algorithm for solving these problems coincides with solving other problems in dynamics:

1. Having selected the axes, write down Newton's law in projections onto each axis, for each of the bodies participating in the problem, or for each of the situations described in the problem.

2. If necessary, supplement the system of equations with the necessary equations from other topics in physics. It is especially important to remember the formula for centripetal acceleration:

3. Solve the resulting system of equations using mathematical methods.

There are also a number of tasks involving rotation in vertical plane on a rod or thread. At first glance, it may seem that such tasks will be the same. This is wrong. The fact is that the rod can experience both tensile and compressive deformations. The thread cannot be compressed; it immediately bends, and the body simply collapses on it.

Movement on a thread. Since the thread only stretches, when a body moves on the thread in a vertical plane, only tensile deformation will occur in the thread and, as a consequence, the elastic force arising in the thread will always be directed towards the center of the circle.

Body movement on a rod. The rod, unlike the thread, can be compressed. Therefore, at the top point of the trajectory, the speed of the body attached to the rod can be equal to zero, in contrast to the thread, where the speed must be no less than a certain value so that the thread does not fold. The elastic forces arising in the rod can be directed both towards the center of the circle and in the opposite direction.

Turning the car. If a body moves along a solid horizontal surface in a circle (for example, a car is going through a turn), then the force that keeps the body on the trajectory will be the friction force. In this case, the friction force is directed towards the turn, and not against it (most common mistake), it helps the car turn. For example, when a car turns right, the friction force is directed in the direction of the turn (to the right).

The law of universal gravitation. Satellites

All bodies attract each other with forces directly proportional to their masses and inversely proportional to the square of the distance between them. Thus law universal gravity in formula form looks like this:

This notation of the law of universal gravitation is valid for material points, balls, spheres, for which r measured between centers. Proportionality factor G is the same for all bodies in nature. He is called gravitational constant. In the SI system it is equal to:

One of the manifestations of the force of universal gravity is the force of gravity. This is the common name for the force of attraction of bodies towards the Earth or another planet. If M– mass of the planet, R n is its radius, then acceleration of free fall at the surface of the planet:

If you move away from the surface of the Earth at some distance h, then the acceleration of free fall at this height will be equal (with the help of simple transformations you can also obtain the relationship between the acceleration of free fall on the surface of the planet and the acceleration of free fall at a certain height above the surface of the planet):

Let us now consider the question of artificial satellites of planets. Artificial satellites move outside the atmosphere (if the planet has one), and they are affected only by gravitational forces from the planet. Depending on the initial speed the trajectory of a cosmic body can be different. We will consider here only the case of motion artificial satellite in a circular orbit at almost zero altitude above the planet. The orbital radius of such satellites (the distance between the center of the planet and the point where the satellite is located) can be approximately taken equal to the radius of the planet R n. Then the centripetal acceleration of the satellite imparted to it by gravitational forces is approximately equal to the acceleration of gravity g. The speed of a satellite in orbit near the surface (at zero altitude above the planet's surface) is called first escape velocity. First escape velocity is found by the formula:

The motion of a satellite can be thought of as a free fall, similar to the motion of projectiles or ballistic missiles. The only difference is that the speed of the satellite is so high that the radius of curvature of its trajectory equal to the radius planets. For satellites moving along circular trajectories at a considerable distance from the planet, gravitational attraction weakens in inverse proportion to the square of the radius r trajectories. The speed of the satellite in this case is found using the formula:

Kepler's law for the periods of revolution of two bodies rotating around one attractive center:

If we are talking about planet Earth, then it is easy to calculate that with a radius r educational materials on that website. To do this, you need nothing at all, namely: devote three to four hours every day to preparing for the CT in physics and mathematics, studying theory and solving problems. The fact is that CT is an exam where it is not enough just to know physics or mathematics, you also need to be able to solve it quickly and without failures a large number of tasks for different topics And of varying complexity. The latter can only be learned by solving thousands of problems.

  • Learn all the formulas and laws in physics, and formulas and methods in mathematics. In fact, this is also very simple to do, necessary formulas in physics there are only about 200 pieces, and in mathematics even a little less. Each of these subjects has about a dozen standard methods for solving problems basic level difficulties that can also be learned, and thus solved completely automatically and without difficulty right moment most of the DH. After this, you will only have to think about the most difficult tasks.
  • Attend all three stages of rehearsal testing in physics and mathematics. Each RT can be visited twice to decide on both options. Again, on the CT, in addition to the ability to quickly and efficiently solve problems, and knowledge of formulas and methods, you must also be able to properly plan time, distribute forces, and most importantly, correctly fill out the answer form, without confusing the numbers of answers and problems, or your own last name. Also, during RT, it is important to get used to the style of asking questions in problems, which may seem very unusual to an unprepared person at the DT.
  • Successful, diligent and responsible implementation of these three points will allow you to show up on the CT excellent result, the maximum of what you are capable of.

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    Mass in dynamics.

    Weight m in dynamics can be considered as a measure of the inertia of a body, that is, its ability to maintain its speed unchanged until other bodies act on it.

    Newton's first law (law of inertia).

    Any body retains its original state relative to the inertial frame of reference (that is, relative to rest or uniform linear motion) until other bodies act on it.

    Inertial reference systems.

    A reference system associated with a body at rest or a body moving rectilinearly and uniformly is called inertial. Also, inertial reference systems are those reference systems in which the law of inertia is satisfied.

    Newton's second law.

    the product of a body's mass and acceleration is equal to the force acting on this body that creates this acceleration. The force and acceleration vectors always have the same directions.

    Newton's second law is valid only in inertial systems.

    The acceleration imparted to a body as a result of the simultaneous action of several forces is equal to the acceleration imparted to it by their resultant:

    Newton's third law.

    The forces with which two interacting bodies act on each other are directed in one straight line, equal in magnitude and opposite in direction:

    Centripetal force.

    The force with which a connection acts on a body when it moves in a circle, directed towards the center of rotation, is called centripetal force:

    Hooke's law.

    Absolute elongation Δ l of a rod under elastic deformation is directly proportional to the applied force:

    F upr - elastic force, k- rigidity of the rod material.

    The elastic force is the force that arises in a deformable body. It is proportional absolute value deformation and is directed opposite to the deformable force.

    Galileo's principle of relativity.

    All inertial frames of reference are equal, therefore the laws of mechanics are written in them in the same way. In them, time, body mass, acceleration and force are constant. The trajectory and speed of movement in different inertial systems are different.

    The law of universal gravitation.

    Two bodies are attracted to each other along the straight line connecting them with a force directly proportional to the masses of the bodies and inversely proportional to the square of the distance between them:

    G- gravitational constant (fundamental physical constant); G= 6.67·10 -11 N·m 2 /kg 2.

    Equality of inertial and gravitational masses.

    Mass can be defined as a scalar quantity that simultaneously characterizes both the inertial and gravitational properties of bodies and is a measure of both of these properties.

    Weight.

    Strength P, with which a body, due to its attraction to the Earth, acts on a horizontal support or suspension that prevents it from free fall, is called weight. Weight is the force applied to the support, not to the body:

    m- body mass, g- acceleration of gravity.

    Unit of weight - 1 N.

    First escape velocity.

    The minimum speed υ 1 that must be imparted to the body in order to enter it into a kilocircular orbit around the Earth:

    RZ is the radius of the Earth.

    Second escape velocity.

    The minimum speed υ 2 that must be imparted to the body in order to remove it from the Earth’s sphere of gravity:

    Friction force.

    The force that arises on the surface of two contacting bodies if they move relative to each other is called the friction force. The friction force that appears in the absence of relative motion of bodies is called the static friction force:

    μ - friction coefficient, depending on the materials and conditions of the rubbing surfaces, as well as on the types of motion (sliding, rolling, rest, etc.), N- force normal pressure.

    The resistance force of the environment.

    For low speeds:

    For high speeds:

    υ - movement speed, k- coefficient of resistance of the medium, depending on its properties, as well as the shape, size and condition of the surface of the moving body.

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    The session is approaching, and it’s time for us to move from theory to practice. Over the weekend we sat down and thought that many students would benefit from having a collection of basic physics formulas at their fingertips. Dry formulas with explanation: short, concise, nothing superfluous. A very useful thing when solving problems, you know. And during an exam, when exactly what was memorized the day before might “jump out” of your head, such a selection will serve an excellent purpose.

    The most problems are usually asked in the three most popular sections of physics. This Mechanics, thermodynamics And Molecular physics, electricity. Let's take them!

    Basic formulas in physics dynamics, kinematics, statics

    Let's start with the simplest. The good old favorite straight and uniform movement.

    Kinematics formulas:

    Of course, let's not forget about motion in a circle, and then we'll move on to dynamics and Newton's laws.

    After dynamics, it’s time to consider the conditions of equilibrium of bodies and liquids, i.e. statics and hydrostatics

    Now we present the basic formulas on the topic “Work and Energy”. Where would we be without them?


    Basic formulas of molecular physics and thermodynamics

    Let's finish the mechanics section with formulas for oscillations and waves and move on to molecular physics and thermodynamics.

    Coefficient useful action, Gay-Lussac's law, the Clapeyron-Mendeleev equation - all these dear formulas are collected below.

    By the way! There is now a discount for all our readers 10% on .


    Basic formulas in physics: electricity

    It's time to move on to electricity, even though it is less popular than thermodynamics. Let's start with electrostatics.

    And, to the beat of the drum, we end with the formulas for Ohm’s law, electromagnetic induction and electromagnetic vibrations.

    That's all. Of course, a whole mountain of formulas could be cited, but this is of no use. When there are too many formulas, you can easily get confused and even melt your brain. We hope our cheat sheet of basic physics formulas will help you solve your favorite problems faster and more efficiently. And if you want to clarify something or haven’t found the right formula: ask the experts student service . Our authors keep hundreds of formulas in their heads and crack problems like nuts. Contact us, and soon any task will be up to you.