Performing mechanical work. A useful formula

Every body that makes a movement can be characterized by work. In other words, it characterizes the action of forces.

Work is defined as:
The product of the modulus of force and the path traveled by the body, multiplied by the cosine of the angle between the direction of force and movement.

Work is measured in Joules:
1 [J] = = [kg* m2/s2]

For example, body A, under the influence of a force of 5 N, traveled 10 m. Determine the work done by the body.

Since the direction of movement and the action of the force coincide, the angle between the force vector and the displacement vector will be equal to 0°. The formula will be simplified because the cosine of an angle of 0° is equal to 1.

Substituting the initial parameters into the formula, we find:
A= 15 J.

Let's consider another example: a body weighing 2 kg, moving with an acceleration of 6 m/s2, has traveled 10 m. Determine the work done by the body if it moved upward along an inclined plane at an angle of 60°.

To begin with, let's calculate how much force needs to be applied to impart an acceleration of 6 m/s2 to the body.

F = 2 kg * 6 m/s2 = 12 H.
Under the influence of a force of 12N, the body moved 10 m. The work can be calculated using the already known formula:

Where, a is equal to 30°. Substituting the initial data into the formula we get:
A= 103.2 J.

Power

Many machines and mechanisms perform the same work in different periods of time. To compare them, the concept of power is introduced.
Power is a quantity that shows the amount of work performed per unit of time.

Power is measured in Watts, after the Scottish engineer James Watt.
1 [Watt] = 1 [J/s].

For example, a large crane lifted a load weighing 10 tons to a height of 30 m in 1 minute. A small crane lifted 2 tons of bricks to the same height in 1 minute. Compare crane capacities.
Let's define the work performed by cranes. The load rises 30m, while overcoming the force of gravity, so the force expended on lifting the load will be equal to the force of interaction between the Earth and the load (F = m * g). And work is the product of forces by the distance traveled by the loads, that is, by the height.

For a large crane A1 = 10,000 kg * 30 m * 10 m/s2 = 3,000,000 J, and for a small crane A2 = 2,000 kg * 30 m * 10 m/s2 = 600,000 J.
Power can be calculated by dividing work by time. Both cranes lifted the load in 1 minute (60 seconds).

From here:
N1 = 3,000,000 J/60 s = 50,000 W = 50 kW.
N2 = 600,000 J/ 60 s = 10,000 W = 10 kW.
From the above data it is clearly seen that the first crane is 5 times more powerful than the second.

Mechanical work. Units of work.

In everyday life, we understand everything by the concept of “work”.

In physics, the concept Job somewhat different. It is a definite physical quantity, which means it can be measured. In physics it is studied primarily mechanical work .

Let's look at examples of mechanical work.

The train moves under the traction force of an electric locomotive, and mechanical work is performed. When a gun is fired, the pressure force of the powder gases does work - it moves the bullet along the barrel, and the speed of the bullet increases.

From these examples it is clear that mechanical work is performed when a body moves under the influence of force. Mechanical work occurs also in the case when a force acting on a body (for example, the force of friction) reduces the speed of its movement.

Wanting to move the cabinet, we press hard on it, but if it does not move, then we do not perform mechanical work. One can imagine a case when a body moves without the participation of forces (by inertia); in this case, mechanical work is also not performed.

So, mechanical work is done only when a force acts on a body and it moves .

It is not difficult to understand that the greater the force acts on the body and the longer the path that the body travels under the influence of this force, the greater the work done.

Mechanical work is directly proportional to the force applied and directly proportional to the distance traveled .

Therefore, we agreed to measure mechanical work by the product of force and the path traveled along this direction of this force:

work = force × path

Where A- Job, F- strength and s- distance traveled.

A unit of work is taken to be the work done by a force of 1N over a path of 1 m.

Unit of work - joule (J ) named after the English scientist Joule. Thus,

1 J = 1N m.

Also used kilojoules (kJ) .

1 kJ = 1000 J.

Formula A = Fs applicable when the force F constant and coincides with the direction of movement of the body.

If the direction of the force coincides with the direction of motion of the body, then this force does positive work.

If the body moves in the direction opposite to the direction of the applied force, for example, the sliding friction force, then this force does negative work.

If the direction of the force acting on the body is perpendicular to the direction of movement, then this force does no work, the work is zero:

In the future, speaking about mechanical work, we will briefly call it in one word - work.

Example. Calculate the work done when lifting a granite slab with a volume of 0.5 m3 to a height of 20 m. The density of granite is 2500 kg/m3.

Given:

ρ = 2500 kg/m 3

Solution:

where F is the force that must be applied to uniformly lift the slab up. This force is equal in modulus to the force Fstrand acting on the slab, i.e. F = Fstrand. And the force of gravity can be determined by the mass of the slab: Fweight = gm. Let's calculate the mass of the slab, knowing its volume and the density of granite: m = ρV; s = h, i.e. the path is equal to the lifting height.

So, m = 2500 kg/m3 · 0.5 m3 = 1250 kg.

F = 9.8 N/kg · 1250 kg ≈ 12,250 N.

A = 12,250 N · 20 m = 245,000 J = 245 kJ.

Answer: A =245 kJ.

Levers.Power.Energy

To perform the same work, different engines require different time. For example, crane at a construction site lifts it up in a few minutes top floor buildings are hundreds of bricks. If these bricks were moved by a worker, it would take him several hours to do this. Another example. A horse can plow a hectare of land in 10-12 hours, while a tractor with a multi-share plow ( ploughshare- part of the plow that cuts the layer of earth from below and transfers it to the dump; multi-ploughshare - many ploughshares), this work will be completed in 40-50 minutes.

It is clear that a crane does the same work faster than a worker, and a tractor does the same work faster than a horse. The speed of work is characterized by a special quantity called power.

Power is equal to the ratio of work to the time during which it was performed.

To calculate power, you need to divide the work by the time during which this work was done. power = work/time.

Where N- power, A- Job, t- time of work completed.

Power is a constant quantity when the same work is done every second; in other cases the ratio A/t determines the average power:

N avg = A/t . The unit of power is taken to be the power at which J of work is done in 1 s.

This unit is called the watt ( W) in honor of another English scientist, Watt.

1 watt = 1 joule/1 second, or 1 W = 1 J/s.

Watt (joule per second) - W (1 J/s).

Larger units of power are widely used in technology - kilowatt (kW), megawatt (MW) .

1 MW = 1,000,000 W

1 kW = 1000 W

1 mW = 0.001 W

1 W = 0.000001 MW

1 W = 0.001 kW

1 W = 1000 mW

Example. Find the power of the water flow flowing through the dam if the height of the water fall is 25 m and its flow rate is 120 m3 per minute.

Given:

ρ = 1000 kg/m3

Solution:

Mass of falling water: m = ρV,

m = 1000 kg/m3 120 m3 = 120,000 kg (12 104 kg).

Gravity acting on water:

F = 9.8 m/s2 120,000 kg ≈ 1,200,000 N (12 105 N)

Work done by flow per minute:

A - 1,200,000 N · 25 m = 30,000,000 J (3 · 107 J).

Flow power: N = A/t,

N = 30,000,000 J / 60 s = 500,000 W = 0.5 MW.

Answer: N = 0.5 MW.

Various engines have powers ranging from hundredths and tenths of a kilowatt (electric razor engine, sewing machine) up to hundreds of thousands of kilowatts (water and steam turbines).

Table 5.

Power of some engines, kW.

Each engine has a plate (engine passport), which indicates some information about the engine, including its power.

Human power at normal conditions work on average is 70-80 W. When jumping or running up stairs, a person can develop power up to 730 W, and in some cases even more.

From the formula N = A/t it follows that

To calculate the work, it is necessary to multiply the power by the time during which this work was performed.

Example. The room fan motor has a power of 35 watts. How much work does he do in 10 minutes?

Let's write down the conditions of the problem and solve it.

Given:

Solution:

A = 35 W * 600s = 21,000 W * s = 21,000 J = 21 kJ.

Answer A= 21 kJ.

Simple mechanisms.

Since time immemorial, man has used various devices to perform mechanical work.

Everyone knows that a heavy object (a stone, a cabinet, a machine tool), which cannot be moved by hand, can be moved with the help of a sufficiently long stick - a lever.

It is currently believed that with the help of levers three thousand years ago during the construction of the pyramids in Ancient Egypt moved and raised heavy stone slabs to great heights.

In many cases, instead of lifting a heavy load to a certain height, it can be rolled or pulled to the same height along inclined plane or lift with blocks.

Devices used to convert force are called mechanisms .

Simple mechanisms include: levers and its varieties - block, gate; inclined plane and its varieties - wedge, screw. In most cases simple mechanisms used to gain strength, that is, to increase the force acting on the body several times.

Simple mechanisms are found in both household and all complex industrial and factory machines that cut, twist and stamp large sheets steel or draw the finest threads from which fabrics are then made. The same mechanisms can be found in modern complex automatic machines, printing and counting machines.

Lever arm. Balance of forces on the lever.

Let's consider the simplest and most common mechanism - the lever.

The lever is solid, which can rotate around a fixed support.

The pictures show how a worker uses a crowbar as a lever to lift a load. In the first case, the worker with force F presses the end of the crowbar B, in the second - raises the end B.

The worker needs to overcome the weight of the load P- force directed vertically downwards. To do this, he turns the crowbar around an axis passing through the only motionless the breaking point is the point of its support ABOUT. Force F with which the worker acts on the lever is less force P, thus the worker receives gain in strength. Using a lever, you can lift such a heavy load that you cannot lift it on your own.

The figure shows a lever whose axis of rotation is ABOUT(fulcrum) is located between the points of application of forces A And IN. Another picture shows a diagram of this lever. Both forces F 1 and F 2 acting on the lever are directed in one direction.

The shortest distance between the fulcrum and the straight line along which the force acts on the lever is called the arm of force.

To find the arm of the force, you need to lower the perpendicular from the fulcrum to the line of action of the force.

The length of this perpendicular will be the arm of this force. The figure shows that OA- shoulder strength F 1; OB- shoulder strength F 2. The forces acting on the lever can rotate it around its axis in two directions: clockwise or counterclockwise. Yes, strength F 1 rotates the lever clockwise, and the force F 2 rotates it counterclockwise.

The condition under which the lever is in equilibrium under the influence of forces applied to it can be established experimentally. It must be remembered that the result of the action of a force depends not only on its numerical value (modulus), but also on the point at which it is applied to the body, or how it is directed.

Various weights are suspended from the lever (see figure) on both sides of the fulcrum so that each time the lever remains in balance. The forces acting on the lever are equal to the weights of these loads. For each case, the force modules and their shoulders are measured. From the experience shown in Figure 154, it is clear that force 2 N balances the force 4 N. In this case, as can be seen from the figure, the shoulder of lesser strength is 2 times larger than the shoulder of greater strength.

Based on such experiments, the condition (rule) of lever equilibrium was established.

A lever is in equilibrium when the forces acting on it are inversely proportional to the arms of these forces.

This rule can be written as a formula:

F 1/F 2 = l 2/ l 1 ,

Where F 1And F 2 - forces acting on the lever, l 1And l 2 , - the shoulders of these forces (see figure).

The rule of lever equilibrium was established by Archimedes around 287 - 212. BC e. (but in the last paragraph it was said that levers were used by the Egyptians? Or here important role plays on the word "installed"?)

From this rule it follows that a smaller force can be used to balance a larger force using a lever. Let one arm of the lever be 3 times larger than the other (see figure). Then, by applying a force of, for example, 400 N at point B, you can lift a stone weighing 1200 N. To lift an even heavier load, you need to increase the length of the lever arm on which the worker acts.

Example. Using a lever, a worker lifts a slab weighing 240 kg (see Fig. 149). What force does he apply to the larger lever arm of 2.4 m if the smaller arm is 0.6 m?

Let's write down the conditions of the problem and solve it.

Given:

Solution:

According to the lever equilibrium rule, F1/F2 = l2/l1, whence F1 = F2 l2/l1, where F2 = P is the weight of the stone. Stone weight asd = gm, F = 9.8 N 240 kg ≈ 2400 N

Then, F1 = 2400 N · 0.6/2.4 = 600 N.

Answer: F1 = 600 N.

In our example, the worker overcomes a force of 2400 N, applying a force of 600 N to the lever. But in this case, the arm on which the worker acts is 4 times longer than the one on which the weight of the stone acts ( l 1 : l 2 = 2.4 m: 0.6 m = 4).

By applying the rule of leverage, a smaller force can balance a larger force. In this case, the shoulder of lesser force should be longer than the shoulder of greater strength.

Moment of power.

You already know the rule of lever equilibrium:

F 1 / F 2 = l 2 / l 1 ,

Using the property of proportion (the product of its extreme members is equal to the product of its middle members), we write it in this form:

F 1l 1 = F 2 l 2 .

On the left side of the equality is the product of force F 1 on her shoulder l 1, and on the right - the product of force F 2 on her shoulder l 2 .

The product of the modulus of the force rotating the body and its shoulder is called moment of force; it is designated by the letter M. This means

A lever is in equilibrium under the action of two forces if the moment of the force rotating it clockwise is equal to the moment of the force rotating it counterclockwise.

This rule is called rule of moments , can be written as a formula:

M1 = M2

Indeed, in the experiment we considered (§ 56), the acting forces were equal to 2 N and 4 N, their shoulders respectively amounted to 4 and 2 lever pressures, i.e. the moments of these forces are the same when the lever is in equilibrium.

The moment of force, like any physical quantity, can be measured. The unit of moment of force is taken to be a moment of force of 1 N, the arm of which is exactly 1 m.

This unit is called newton meter (N m).

The moment of force characterizes the action of a force, and shows that it depends simultaneously on both the modulus of the force and its leverage. Indeed, we already know, for example, that the action of a force on a door depends both on the magnitude of the force and on where the force is applied. The easier it is to turn the door, the farther from the axis of rotation the force acting on it is applied. It’s better to unscrew the nut long wrench than short. The easier it is to lift a bucket from the well, the longer the handle of the gate, etc.

Levers in technology, everyday life and nature.

The rule of leverage (or the rule of moments) underlies the action of various kinds of tools and devices used in technology and everyday life where a gain in strength or travel is required.

We have a gain in strength when working with scissors. Scissors - this is a lever(fig), the axis of rotation of which occurs through a screw connecting both halves of the scissors. Acting force F 1 is the muscular strength of the hand of the person gripping the scissors. Counterforce F 2 is the resistance force of the material being cut with scissors. Depending on the purpose of the scissors, their design varies. Office scissors, designed for cutting paper, have long blades and handles that are almost the same length. No paper cutting required great strength, and with a long blade it is more convenient to cut in a straight line. Cutting scissors sheet metal(Fig.) have handles much longer than the blades, since the resistance force of the metal is great and to balance it, the arm of the acting force has to be significantly increased. The difference between the length of the handles and the distance of the cutting part and the axis of rotation is even greater wire cutters(Fig.), designed for cutting wire.

Levers various types available on many cars. The handle of a sewing machine, the pedals or handbrake of a bicycle, the pedals of a car and tractor, and the keys of a piano are all examples of levers used in these machines and tools.

Examples of the use of levers are the handles of vices and workbenches, the lever drilling machine etc.

The action of lever scales is based on the principle of the lever (Fig.). The training scales shown in Figure 48 (p. 42) act as equal-arm lever . IN decimal scales The shoulder from which the cup with weights is suspended is 10 times longer than the shoulder carrying the load. This makes weighing large loads much easier. When weighing a load on a decimal scale, you should multiply the mass of the weights by 10.

The device of scales for weighing freight cars of cars is also based on the rule of leverage.

Levers are also found in different parts bodies of animals and humans. These are, for example, arms, legs, jaws. Many levers can be found in the body of insects (by reading a book about insects and the structure of their bodies), birds, and in the structure of plants.

Application of the law of equilibrium of a lever to a block.

Block It is a wheel with a groove, mounted in a holder. A rope, cable or chain is passed through the block groove.

Fixed block This is called a block whose axis is fixed and does not rise or fall when lifting loads (Fig.).

A fixed block can be considered as an equal-armed lever, in which the arms of forces are equal to the radius of the wheel (Fig): OA = OB = r. Such a block does not provide a gain in strength. ( F 1 = F 2), but allows you to change the direction of the force. Movable block - this is a block. the axis of which rises and falls along with the load (Fig.). The figure shows the corresponding lever: ABOUT- fulcrum point of the lever, OA- shoulder strength R And OB- shoulder strength F. Since the shoulder OB 2 times the shoulder OA, then the strength F 2 times less force R:

F = P/2 .

Thus, the movable block gives a 2-fold increase in strength .

This can be proven using the concept of moment of force. When the block is in equilibrium, the moments of forces F And R equal to each other. But the shoulder of strength F 2 times the leverage R, and, therefore, the power itself F 2 times less force R.

Usually in practice a combination of a fixed block and a movable one is used (Fig.). The fixed block is used for convenience only. It does not give a gain in force, but it changes the direction of the force. For example, it allows you to lift a load while standing on the ground. This comes in handy for many people or workers. However, it gives a gain in strength 2 times greater than usual!

Equality of work when using simple mechanisms. "Golden rule" of mechanics.

The simple mechanisms we have considered are used when performing work in cases where it is necessary to balance another force through the action of one force.

Naturally, the question arises: while giving a gain in strength or path, don’t simple mechanisms give a gain in work? The answer to this question can be obtained from experience.

By balancing two different magnitude forces on a lever F 1 and F 2 (fig.), set the lever in motion. It turns out that at the same time the point of application of the smaller force F 2 goes further s 2, and the point of application of the greater force F 1 - shorter path s 1. Having measured these paths and force modules, we find that the paths traversed by the points of application of forces on the lever are inversely proportional to the forces:

s 1 / s 2 = F 2 / F 1.

Thus, acting on the long arm of the lever, we gain in strength, but at the same time we lose by the same amount along the way.

Product of force F on the way s there is work. Our experiments show that the work done by the forces applied to the lever is equal to each other:

F 1 s 1 = F 2 s 2, i.e. A 1 = A 2.

So, When using leverage, you won’t be able to win at work.

By using leverage, we can gain either power or distance. By applying force to the short arm of the lever, we gain in distance, but lose by the same amount in strength.

There is a legend that Archimedes, delighted with the discovery of the rule of leverage, exclaimed: “Give me a fulcrum and I will turn the Earth over!”

Of course, Archimedes could not cope with such a task even if he had been given a fulcrum (which should have been outside the Earth) and a lever of the required length.

To raise the earth just 1 cm, the long arm of the lever would have to describe an arc of enormous length. It would take millions of years to move the long end of the lever along this path, for example, at a speed of 1 m/s!

A stationary block does not give any gain in work, which is easy to verify experimentally (see figure). Ways, passable points application of forces F And F, are the same, the forces are the same, which means the work is the same.

You can measure and compare the work done with the help of a moving block. In order to lift a load to a height h using a movable block, it is necessary to move the end of the rope to which the dynamometer is attached, as experience shows (Fig.), to a height of 2h.

Thus, getting a 2-fold gain in strength, they lose 2-fold on the way, therefore, the movable block does not give a gain in work.

Centuries-old practice has shown that None of the mechanisms gives a gain in performance. They use various mechanisms in order to win in strength or in travel, depending on the working conditions.

Already ancient scientists knew a rule applicable to all mechanisms: no matter how many times we win in strength, the same number of times we lose in distance. This rule has been called the "golden rule" of mechanics.

Efficiency of the mechanism.

When considering the design and action of the lever, we did not take into account friction, as well as the weight of the lever. in these ideal conditions work done by the applied force (we will call this work full), is equal to useful work on lifting loads or overcoming any resistance.

In practice, the total work done with the help of a mechanism is always slightly greater useful work.

Part of the work is done against the friction force in the mechanism and by moving it individual parts. So, when using a movable block, you have to additionally do work to lift the block itself, the rope and determine the friction force in the axis of the block.

Whatever mechanism we take, the useful work done with its help is always only a part full work. This means, denoting useful work by the letter Ap, total (expended) work by the letter Az, we can write:

Up< Аз или Ап / Аз < 1.

The ratio of useful work to total work is called the efficiency of the mechanism.

The efficiency factor is abbreviated as efficiency.

Efficiency = Ap / Az.

Efficiency is usually expressed as a percentage and is denoted by the Greek letter η, read as “eta”:

η = Ap / Az · 100%.

Example: A load weighing 100 kg is suspended on the short arm of a lever. To lift it, a force of 250 N is applied to the long arm. The load is raised to a height h1 = 0.08 m, and the point of application driving force dropped to a height h2 = 0.4 m. Find the efficiency of the lever.

Let's write down the conditions of the problem and solve it.

Given :

Solution :

η = Ap / Az · 100%.

Total (expended) work Az = Fh2.

Useful work Ap = Рh1

P = 9.8 100 kg ≈ 1000 N.

Ap = 1000 N · 0.08 = 80 J.

Az = 250 N · 0.4 m = 100 J.

η = 80 J/100 J 100% = 80%.

Answer : η = 80%.

But " Golden Rule"is carried out in this case as well. Part of the useful work - 20% of it - is spent on overcoming friction in the axis of the lever and air resistance, as well as on the movement of the lever itself.

The efficiency of any mechanism is always less than 100%. When designing mechanisms, people strive to increase their efficiency. To achieve this, friction in the axes of the mechanisms and their weight are reduced.

Energy.

In factories and factories, machines and machines are driven by electric motors, which consume electrical energy (hence the name).

A compressed spring (Fig.), when straightened, does work, raises a load to a height, or makes a cart move. A stationary load raised above the ground does not do work, but if this load falls, it can do work (for example, it can drive a pile into the ground). Every moving body has the ability to do work. Thus, steel ball A (Fig.) rolled down from an inclined plane, hitting wooden block B, moves it some distance. At the same time, work is done. If a body or several interacting bodies (a system of bodies) can do work, they are said to have energy. Energy - a physical quantity showing how much work a body (or several bodies) can do. Energy is expressed in the SI system in the same units as work, i.e. in joules. How great job a body can accomplish, the more energy it possesses. When work is done, the energy of bodies changes. Work done is equal to the change in energy. Potential and kinetic energy. Potential (from lat. potency - possibility) energy is the energy that is determined by the relative position of interacting bodies and parts of the same body. Potential energy, for example, is possessed by a body raised relative to the surface of the Earth, because the energy depends on the relative position of it and the Earth. and their mutual attraction. If we consider the potential energy of a body lying on the Earth to be zero, then the potential energy of a body raised to a certain height will be determined by the work done by gravity when the body falls to the Earth. Let us denote the potential energy of the body E n, because E = A, and work, as we know, is equal to the product of force and path, then A = Fh, Where F- gravity. This means that the potential energy En is equal to: E = Fh, or E = gmh, Where g- acceleration of gravity, m- body mass, h- the height to which the body is raised. Water in rivers held by dams has enormous potential energy. Falling down, the water does work, driving powerful turbines of power plants. The potential energy of a copra hammer (Fig.) is used in construction to carry out the work of driving piles. When opening a door with a spring, work is done to stretch (or compress) the spring. Due to the acquired energy, the spring, contracting (or straightening), does work, closing the door. The energy of compressed and untwisted springs is used, for example, in watches, various wind-up toys, etc. Any elastic deformed body has potential energy. The potential energy of compressed gas is used in the operation of heat engines, in jackhammers, which are widely used in the mining industry, in road construction, excavation of hard soil, etc. The energy that a body possesses as a result of its movement is called kinetic (from the Greek. kinema - movement) energy. The kinetic energy of a body is denoted by the letter E To. Moving water, driving the turbines of hydroelectric power stations, consumes its kinetic energy and does the work. Moving air, the wind, also has kinetic energy. What does kinetic energy depend on? Let's turn to experience (see figure). If you roll ball A from different heights, then you can notice that the greater the height the ball rolls, the greater its speed and the further it moves the block, i.e., it does more work. This means that the kinetic energy of a body depends on its speed. Due to its speed, a flying bullet has high kinetic energy. The kinetic energy of a body also depends on its mass. Let's do our experiment again, but we'll roll another ball of greater mass from the inclined plane. Bar B will move further, i.e. more work will be done. This means that the kinetic energy of the second ball is greater than the first. The greater the mass of a body and the speed at which it moves, the greater its kinetic energy. In order to determine the kinetic energy of a body, the formula is used: Ek = mv^2 /2, Where m- body mass, v- speed of body movement. The kinetic energy of bodies is used in technology. The water retained by the dam has, as already mentioned, great potential energy. When water falls from a dam, it moves and has the same high kinetic energy. It drives a turbine connected to a generator electric current. Due to the kinetic energy of water, electrical energy is generated. The energy of moving water has great importance in the national economy. This energy is used using powerful hydroelectric power plants. The energy of falling water is an environmentally friendly source of energy, unlike fuel energy. All bodies in nature, relative to the conventional zero value, have either potential or kinetic energy, and sometimes both together. For example, a flying airplane has both kinetic and potential energy relative to the Earth. We became acquainted with two types of mechanical energy. Other types of energy (electrical, internal, etc.) will be discussed in other sections of the physics course. Conversion of one type of mechanical energy into another. The phenomenon of transformation of one type of mechanical energy into another is very convenient to observe on the device shown in the figure. By winding the thread onto the axis, the device disk is lifted. A disk raised upward has some potential energy. If you let go of it, it will spin and begin to fall. As it falls, the potential energy of the disk decreases, but at the same time its kinetic energy increases. At the end of the fall, the disk has such a reserve of kinetic energy that it can rise again to almost its previous height. (Part of the energy is spent working against the frictional force, so the disk does not reach its original height.) Having risen up, the disk falls again and then rises again. In this experiment, when the disk moves downward, its potential energy turns into kinetic energy, and when it moves up, the kinetic energy turns into potential energy. The transformation of energy from one type to another also occurs when two elastic bodies collide, for example, a rubber ball on the floor or a steel ball on a steel plate. If you lift a steel ball (rice) above a steel plate and release it from your hands, it will fall. As the ball falls, its potential energy decreases, and its kinetic energy increases, as the speed of the ball increases. When the ball hits the plate, both the ball and the plate will be compressed. The kinetic energy that the ball had will turn into potential energy of the compressed plate and the compressed ball. Then, thanks to the action of elastic forces, the plate and the ball will take their original shape. The ball will bounce off the slab, and their potential energy will again turn into the kinetic energy of the ball: the ball will bounce up at a speed almost equal to the speed it had at the moment it hit the slab. As the ball rises upward, the speed of the ball, and therefore its kinetic energy, decreases, while the potential energy increases. Having bounced off the plate, the ball rises to almost the same height from which it began to fall. At the top point of the rise, all its kinetic energy will again turn into potential. Natural phenomena are usually accompanied by the transformation of one type of energy into another. Energy can be transferred from one body to another. For example, when archery, the potential energy of a drawn bowstring is converted into the kinetic energy of a flying arrow.

Do you know what work is? Without any doubt. Every person knows what work is, provided that he was born and lives on planet Earth. What is mechanical work?

This concept is also known to most people on the planet, although some individuals have a rather vague understanding of this process. But we are not talking about them now. Even fewer people have any idea what it is mechanical work from the point of view of physics. In physics, mechanical work is not human labor for food, it is a physical quantity that may be completely unrelated to either a person or any other living creature. How so? Let's figure it out now.

Mechanical work in physics

Let's give two examples. In the first example, the waters of the river, faced with an abyss, noisily fall down in the form of a waterfall. The second example is a person who holds a heavy object with outstretched arms, for example, holding a broken roof over a porch country house from falling while his wife and children frantically search for something to support her. When is mechanical work performed?

Definition of mechanical work

Almost everyone, without hesitation, will answer: in the second. And they will be wrong. The opposite is true. In physics, mechanical work is described with the following definitions: Mechanical work is performed when a force acts on a body and it moves. Mechanical work is directly proportional to the force applied and the distance traveled.

Mechanical work formula

Mechanical work is determined by the formula:

where A is work,
F - strength,
s is the distance traveled.

So, despite all the heroism of the tired roof holder, the work he has done is zero, but the water, falling under the influence of gravity from a high cliff, does the most mechanical work. That is, if we push a heavy cabinet unsuccessfully, then the work we have done from the point of view of physics will be equal to zero, despite the fact that we apply a lot of force. But if we move the cabinet a certain distance, then we will do work equal to the product of the applied force and the distance over which we moved the body.

The unit of work is 1 J. This is the work done by a force of 1 Newton to move a body over a distance of 1 m. If the direction of the applied force coincides with the direction of movement of the body, then this force does positive work. An example is when we push a body and it moves. And in the case when a force is applied in the direction opposite to the movement of the body, for example, friction force, then this force does negative work. If the applied force does not affect the movement of the body in any way, then the force performed by this work is equal to zero.

Efficiency shows the ratio of the useful work performed by a mechanism or device to the work expended. Often, work expended is the amount of energy a device consumes to do the work.

You will need

1. - automobile;
2. - thermometer;
3. - calculator.

Instructions

1. In order to calculate the coefficient useful actions(efficiency) divide the useful work Ap by the work expended Az, and multiply the result by 100% (efficiency = Ap/Az∙100%). You will receive the result as a percentage.
2. When calculating the efficiency of a heat engine, consider the useful work to be the mechanical work performed by the mechanism. For the work expended, take the amount of heat released by the burned fuel, which is the source of energy for the engine.
3. Example. The average traction force of a car engine is 882 N. It consumes 7 kg of gasoline per 100 km of travel. Determine the efficiency of its engine. Find a rewarding job first. It is equal to the product of force F and the distance S covered by the body under its influence Аn=F∙S. Determine the amount of heat that will be released when burning 7 kg of gasoline, this will be the work expended Az = Q = q∙m, where q is the specific heat of combustion of the fuel, for gasoline it is equal to 42∙10^6 J/kg, and m is the mass this fuel. The engine efficiency will be equal to efficiency=(F∙S)/(q∙m)∙100%= (882∙100000)/(42∙10^6∙7)∙100%=30%.
4. In general, to find the efficiency of any heat engine (engine) internal combustion, steam engine, turbines, etc.), where work is performed by gas, has a coefficient useful actions equal to the difference in the heat given off by the heater Q1 and received by the refrigerator Q2, find the difference between the heat of the heater and the refrigerator, and divide by the heat of the heater efficiency = (Q1-Q2)/Q1. Here, efficiency is measured in submultiple units from 0 to 1; to convert the result into percentages, multiply it by 100.
5. To obtain the efficiency of an ideal heat engine (Carnot machine), find the ratio of the temperature difference between the heater T1 and the refrigerator T2 to the heater temperature efficiency = (T1-T2)/T1. This is the maximum possible efficiency for a specific type of heat engine with given temperatures of the heater and refrigerator.
6. For an electric motor, find the work expended as the product of power and the time it takes to complete it. For example, if a crane electric motor with a power of 3.2 kW lifts a load weighing 800 kg to a height of 3.6 m in 10 s, then its efficiency is equal to the ratio of useful work Аp=m∙g∙h, where m is the mass of the load, g≈10 m /s² acceleration of free fall, h – height to which the load was raised, and expended work Az=P∙t, where P – engine power, t – time of its operation. Get the formula for determining efficiency=Ap/Az∙100%=(m∙g∙h)/(P∙t) ∙100%=%=(800∙10∙3.6)/(3200∙10) ∙100% =90%.

What is the formula for useful work?

Using this or that mechanism, we perform work that always exceeds that which is necessary to achieve the goal. In accordance with this, a distinction is made between the complete or expended work Az and the useful work Ap. If, for example, our goal is to lift a load of mass m to a height H, then useful work is that which is due only to overcoming the force of gravity acting on the load. With a uniform lifting of the load, when the force we apply is equal to the gravitational force of the load, this work can be found as follows:
Ap =FH= mgH

What is work in physics definition formula. nn

Victor Chernobrovin

In physics, “mechanical work” is the work of some force (gravity, elasticity, friction, etc.) on a body, as a result of which the body moves. Sometimes you can come across the expression “the body has done work,” which in principle means “the force acting on the body has done work.”

Evgeny Makarov

Work is a physical quantity, numerically equal to the product of force and displacement in the direction of action of this force and caused by it.
Accordingly, the formula A = F*s. If the movement in the direction does not coincide with the direction of the force, then the cosine of the angle appears.

Aysha Allakulova

novel of sparrows

Work is a process that requires the application of mental or physical effort, the goal of which is to obtain a certain result. It is work, as a rule, that determines social status person. And it is, in fact, the main engine of progress in society. Work, as a phenomenon, is inherent only to living organisms and, above all, to humans.

Mechanic

Mechanical work is a physical quantity that is a scalar quantitative measure of the action of a force or forces on a body or system, depending on the numerical value, direction of the force (forces) and on the movement of the point (points), body or system.

Help me understand the formula!!

Syoma

in each specific case we consider different useful energy, but usually this is the work or heat that interested us (for example, the work of a gas to move a piston), and the energy expended is the energy that we gave up to make our everything work (for example, the energy released when wood is burned under a cylinder with a piston, inside of which there is gas, which, expanding, did the work that we considered as useful)
well it has to be like this somehow

Let's take a steam locomotive as an example.
In order for a steam locomotive to travel x km, it is necessary to spend y tons of coal. When coal is burned, only Q1 of heat is released, but not all of the heat is converted into useful work (according to the laws of thermodynamics, this is impossible). Useful work in in this case- movement of the locomotive.
Let a resistance force F act on the steam locomotive while moving (it arises due to friction in the mechanisms and other factors).
So, having traveled x km, the locomotive will do work Q2 = x*F
Thus,
Q1 - energy expended
Q2 - useful work

DeltaQ = (Q1 - Q2) - energy spent on overcoming friction, heating the surrounding air, etc.

Technical support

Efficiency is useful WORK relative to the work expended.
For example, efficiency = 60%, 60 joules from the combustion of the substance are used for heating. It's rewarding work.
We are interested in the energy expended, that is, how much heat was released if 60 J were spent on heating.
Let's write it down.

Efficiency=Apol/Azatr
0.6=60/Azatr
Azatr=60/0.6=100J

As we can see, if a substance burns at such an efficiency and 100 J (work expended) is released during combustion, then only 60% was used for heating, that is, 60 J (useful work). The rest of the heat dissipated.

Prokhorov Anton

It must be understood in the literal sense: If we are talking about thermal energy, then we consider spent the energy that the fuel provides, and we consider useful the energy that we were able to use to achieve our goal, for example, what energy a pot of water received.
Useful energy is always less than expended!

Futynehf

Efficiency is expressed as a percentage, characterizing the percentage that went to useful work out of everything spent. Simply put, the energy expended is useful energy + the energy of heat loss in the system (if we are talking about heat, etc.) friction. heat from exhaust gases if we mean a car

Efficiency formula? Is the work useful and complete?

Orbital constellation

Efficiency
Efficiency
(efficiency), a characteristic of the efficiency of a system (device, machine) in relation to the conversion or transmission of energy; determined by the ratio of usefully used energy to the total amount of energy received by the system; usually denoted h = Wfull/Wcymar.
IN electric motors efficiency - the ratio of the performed (useful) mechanical work to electrical energy, received from the source; in heat engines - the ratio of useful mechanical work to the amount of heat expended; in electrical transformers, the ratio of electromagnetic energy received in the secondary winding to the energy consumed by the primary winding. To calculate efficiency different types energy and mechanical work are expressed in the same units based on the mechanical equivalent of heat, and other similar relationships. Due to its generality, the concept of efficiency allows us to compare and evaluate such various systems like nuclear reactors, electric generators and engines, thermal power plants, semiconductor devices, biological objects, etc.
http://ru.wikipedia.org/wiki/Work_of_force
Payload is a term that is used in many fields of science and technology.
The “efficiency” parameter is often introduced as the ratio of the “weight” of the payload to the total “weight” of the system. In this case, “weight” can be measured both in kilograms/tons, and bits (when transmitting packets over a network), or minutes/hours (when calculating the efficiency of processor time), or in other units.
http://ru.wikipedia.org/wiki/Payload

What is useful work and what is wasted work?

Vladimir Popov

Using this or that mechanism, we perform work that always exceeds that which is necessary to achieve the goal. In accordance with this, a distinction is made between the complete or expended work Az and the useful work Ap. If, for example, our goal is to lift a load of mass w to a height H, then useful work is that which is due only to overcoming the force of gravity acting on the load. With a uniform lifting of the load, when the force we apply is equal to the gravitational force of the load, this work can be found as follows:

If we use a block or some other mechanism to lift a load, then, in addition to the gravity of the load, we also have to overcome the gravity of the parts of the mechanism, as well as the frictional force acting in the mechanism. For example, using a movable block, we will be forced to do additional work to lift the block itself with a cable and to overcome the friction force in the axis of the block. In addition, while winning in strength, we always lose along the way (this will be discussed in more detail below), which also affects work. All this leads to the fact that the work we expended turns out to be more useful:
Az > Ap.
Useful work is always only a small part of the total work done by a person using a machine.
A physical quantity that shows what proportion of useful work is the total work expended is called the efficiency of the mechanism.

Gorgeous

Efficiency (efficiency factor) shows what proportion of the total work expended is useful work.
To find efficiency, you need to find the ratio of useful work to expended:

The horse pulls the cart with some force, let's denote it F traction. Grandfather, sitting on the cart, presses on it with some force. Let's denote it F pressure The cart moves along the direction of the horse's traction force (to the right), but in the direction of the grandfather's pressure force (downward) the cart does not move. That's why in physics they say that F traction does work on the cart, and F the pressure does not do work on the cart.

So, work of force on the body or mechanical work– a physical quantity whose modulus is equal to the product of the force and the path traveled by the body along the direction of action of this force s:

In honor of the English scientist D. Joule, the unit of mechanical work was named 1 joule(according to the formula, 1 J = 1 N m).

If a certain force acts on the body in question, then some body acts on it. That's why the work of force on the body and the work of the body on the body are complete synonyms. However, the work of the first body on the second and the work of the second body on the first are partial synonyms, since the moduli of these works are always equal, and their signs are always opposite. That is why there is a “±” sign in the formula. Let's discuss the signs of work in more detail.

Numerical values ​​of force and path are always non-negative quantities. In contrast, mechanical work can have both positive and negative signs. If the direction of the force coincides with the direction of motion of the body, then the work done by the force is considered positive. If the direction of force is opposite to the direction of motion of the body, the work done by a force is considered negative(we take “–” from the “±” formula). If the direction of motion of the body is perpendicular to the direction of the force, then such a force does not do any work, that is, A = 0.

Consider three illustrations of three aspects of mechanical work.

Doing work by force may look different from the perspective of different observers. Let's consider an example: a girl rides up in an elevator. Does it perform mechanical work? A girl can do work only on those bodies that are acted upon by force. There is only one such body - the elevator cabin, since the girl presses on its floor with her weight. Now we need to find out whether the cabin goes a certain way. Let's consider two options: with a stationary and moving observer.

Let the observer boy sit on the ground first. In relation to it, the elevator car moves upward and passes a certain distance. The girl’s weight is directed in the opposite direction - down, therefore, the girl performs negative mechanical work on the cabin: A dev< 0. Вообразим, что мальчик-наблюдатель пересел внутрь кабины движущегося лифта. Как и ранее, вес девочки действует на пол кабины. Но теперь по отношению к такому наблюдателю кабина лифта не движется. Поэтому с точки зрения наблюдателя в кабине лифта девочка не совершает механическую работу: A dev = 0.

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