fizikzauglom

GRADE 7 · WORK, POWER AND ENERGY

Efficiency and mechanical energy

Useful and total input work, kinetic and potential energy.

24 minutes12 theory cards
Start interactive lesson

Read the full lesson theory here without an account. In the interactive lesson, the same theory is presented as cards, followed by questions with feedback and practice problems. Your progress is saved.

Understanding step by step

A bicycle has stopped, and its brake pads have become hot. Has what previously enabled it to move and do work disappeared? We will follow energy from raised and moving objects to heating, and assess what fraction of the input achieves our goal.

Braking to a stopwas movingthere was motionbrake pads heated upEnergy changed form, not vanished
A bicycle brakes to a stop while its pads become noticeably hotter. The energy of motion has not disappeared; it has changed form.

Energy of interaction

Raise a load and release it: as it descends, it can lift another object through a rope. Its new position has therefore given it the ability to do work. Interaction energy that depends on the relative positions of objects is called potential energy. For the load, it belongs to the object–Earth system. A compressed spring can also do work as it expands; its potential energy is associated with deformation. Visible rest does not mean an absence of energy.

mhmgZero level
The instant after the raised load is released is shown. Gravity mg acts downwards at its centre of mass and can do work as it descends. In Ep = mgh, h is measured from the chosen zero level to the centre of mass.

Choose a zero level

From which height should we measure the load's energy: the floor or the tabletop? Choose a zero level. Measure height h vertically from it to the centre of mass, a point describing mass distribution; for a uniform rectangular block, it is at the centre. Moving the zero changes the numerical potential energy. But for the same lift, the height change, required work and energy change remain unchanged.

One load, two zero levelszero: floortablecentre of massh₁h₂zero: tableSame lift, same energy increase
Heights h₁ and h₂ are measured vertically from the floor and tabletop to the same point: the uniform block's centre of mass. The table surface and its zero level coincide. Choosing a different zero changes potential energy, but its change in the same lift stays unchanged.

Potential energy near Earth

Slowly lifting a load through height h requires overcoming its approximately constant gravitational force mg. The lifting work is mgh, so relative to the chosen zero, Eп = mgh for constant g near Earth's surface. Doubling mass or height doubles the energy; at h = 0 it is zero by our choice of reference. kg·N/kg·m gives joules. This formula describes gravity, not a spring; energy change depends on height change, not on the length of a detour.

Eп = m · g · hmкгgН/кгhмresult in joulesfor a spring, this formuladoes not apply
Multiply mass in kilograms by gravitational field strength and height in metres to obtain joules. The formula applies to gravity near Earth's surface, not to an elastic spring.

Energy of motion

A moving ball can shift an object, and a moving cart can compress a spring while slowing down. Energy associated with motion is kinetic energy Eк. It tells us how much work can be obtained during braking under suitable conditions. Motion is measured in a chosen reference frame: a ball on a bus seat is at rest relative to the bus but moves relative to the road. Kinetic energy therefore depends on the frame and is zero when the object is at rest in that frame.

mmv2vRelative to the roadEк4Eк
Identical carts move relative to the road at speeds v and 2v. The bars show translational kinetic energy: for the same mass, the right-hand energy is 4 times larger. Wheel rotation is not included here.

Why speed is squared

For translational motion in school mechanics, Eк = mv²/2. Why does speed have a stronger effect than mass? Under the same braking force, a faster object takes longer to lose speed and covers distance at a greater average speed throughout; braking work grows for both reasons. The formula quantifies the result: doubling mass doubles energy, while doubling speed quadruples it. Mass in kg and speed in m/s give energy in J.

Eк = m · v² / 2Same speedSame massm2mv2vEк2EкEк4EкMass × 2 → Eк × 2Speed × 2 → Eк × 4Bars show energy, not speed
Bar lengths represent kinetic energy. On the left, speed is unchanged: mass 2m gives energy 2Eк. On the right, mass is unchanged: speed 2v gives 4Eк. Both comparisons use the same initial energy and bar scale.

During a fall

Release a load from rest. As it falls, height and Eп decrease while speed and Eк increase. If only gravity acts and air resistance is negligible, the loss of one exactly equals the gain of the other: Eп + Eк = const. Near the ground, chosen as the zero level, almost all the initial mechanical energy has become kinetic. This relates two states without calculating position every second.

ReleasedFallingFallingZero level for EпEк = 0EпEкTotal length: Eп + Eк = const
One block is released from rest; three instants are spaced horizontally for comparison. Its centre-of-mass heights above zero are in the ratio 5 : 3 : 1, as are the blue Eп segments. Green Eк grows by the same amount that Eп falls. Total bars are equal. Air resistance is neglected.

Where the losses go

Now include air or brakes. Eп + Eк may decrease, but energy does not disappear. Some becomes internal energy of the objects and surroundings: energy of their particles' motion and interactions. Hot brakes make this visible. 'Loss' refers to our goal: the energy is less available for the original mechanical work. A complete balance includes the mechanism and surroundings as well as the moving load.

Where the difference goesMechanical energy beforeMechanical energy afterHeatingTotal length is unchangedSome became internal energy
Friction converts some mechanical energy into internal energy of the objects and surroundings. The two lower segments together equal the original bar: energy is conserved. The fraction is illustrative, not a measured loss.

What counts as useful?

A machine has a task, such as lifting a load onto a shelf. Call the work serving that goal Aпол. Call all work supplied to the machine Aзатр: it includes the useful result, heating and other transformations. Both are measured in joules. First define the goal and boundaries of the process. Deformation may be a loss for a lift but a useful result for a press; no physical process is inherently labelled 'useful'.

Goal: raise the loadbeforeliftinputusefullossesBoth works refer to one lift
The winch raises the same load from the dashed position. Useful work serves the lift; input work includes losses too. The useful and loss segments together equal the input bar; initial and final speeds are equal.

The useful fraction of work

What fraction of the input served the goal? Divide useful work by input work: η = Aпол/Aзатр for Aзатр > 0. This is efficiency, a dimensionless fraction; multiply by 100% to express it as a percentage. At fixed input, more useful work raises efficiency; reducing losses brings it closer to 100%. The ideal limit is 100%; a real machine with losses falls below it. Above 100% means this balance has omitted an energy source or defined the work incorrectly.

Example of work distributionInput: 100 Дж80 Дж useful20 Джheatingη = 80 / 100 = 0,8 = 80 %
Illustrative example: of 100 J input, 80 J is useful and 20 J becomes heating. The lower bar is divided exactly in the ratio 80 : 20 and has the same total length as the upper bar. Efficiency compares useful work with input: 0,8 = 80%.

Lifting with losses

A machine lifts a 2 kg load through 3 m using 100 J. Take g = 10 Н/кг, with equal initial and final speeds. Find the efficiency.

Given values2 кгbefore3 мInput: 100 Джg = 10 Н/кгInitial and finalspeeds are equalEfficiency — ?
A winch raises a 2 kg load from the dashed position through 3 m using 100 J. Height change is measured between corresponding points in the two positions. Initial and final speeds are equal; g = 10 Н/кг. The same apparatus is retained in the calculation.

Let's look at an example · 1

The useful result is the load's increase in potential energy: Aпол = mgh = 2·10·3 = 60 Дж.

Calculate useful work2 кгbefore3 мInput: 100 Джg = 10 Н/кгInitial and finalspeeds are equalAпол = 2 · 10 · 3 = 60 Дж
The same 2 kg load is raised 3 m. Equal initial and final speeds mean zero change in kinetic energy. Useful work equals the increase in potential energy: 2 · 10 · 3 = 60 Дж.

Let's look at an example · 2

Efficiency: η = 60/100 = 0,6 = 60%.

Useful fraction of input2 кгbefore3 мInput: 100 Джg = 10 Н/кгInitial and finalspeeds are equalη = 60 / 100 = 0,6 = 60 %
For the same lift, divide the useful 60 J by the input 100 J: η = 0,6 = 60%. The apparatus, mass, height and conditions stay unchanged.

Let's look at an example · 3

The remaining 40 J has not disappeared: it went into other transformations, such as heating the machine.

100 Дж = 60 Дж + 40 Дж2 кгbefore3 мInput: 100 Джg = 10 Н/кгInitial and finalspeeds are equal60 Дж — lifting40 Дж — other
In the same lift, 60 J of the 100 J increased potential energy; the remaining 40 J went into other transformations, such as heating. Segments represent exactly 60% and 40%; total energy is conserved.

Let's check the result

Efficiency: 60%.

Key idea · 1

Potential energy is associated with interaction and position, kinetic energy with motion: Eп = mgh and Eк = mv²/2 under the stated conditions.

Key idea · 2

Without resistance, mechanical energy is conserved during a fall; friction converts some of it into internal energy.

Key idea · 3

Efficiency compares the useful result with total input. 'Losses' mean a different route of energy transformation, not energy disappearing.

Where do we go next?

In grade 8, we will explain internal energy and thermal processes through particle motion and interactions.

Basic Concepts

3 concepts

Efficiency

The ratio of useful work to total input work, usually expressed as a percentage.

Friction and deformation make a real machine's efficiency less than one hundred percent, but energy is dissipated rather than destroyed.

Potential energy

Interaction energy that depends on the relative positions of objects or the deformation of an elastic object.

A raised load can do work as it descends; a compressed spring can do work as it returns to its original shape.

Kinetic energy

Energy of an object's motion, increasing with mass and especially rapidly with speed.

In free fall, potential energy becomes kinetic energy if air resistance is negligible.

Physical quantities

6 quantities

Efficiency

\eta

The fraction of total input work converted into useful work.

Unit: dimensionless quantity

Useful work

A_{\text{пол}}

The part of input work that serves the machine's purpose.

Unit: joule · \mathrm{Дж}

Total input work

A_{\text{затр}}

All work supplied to operate a real machine.

Unit: joule · \mathrm{Дж}

Potential energy

E_p

An object's energy associated with its position in a gravitational field.

Unit: joule · \mathrm{Дж}

Kinetic energy

E_k

An object's energy associated with its mechanical motion.

Unit: joule · \mathrm{Дж}

Height

h

An object's vertical coordinate relative to a chosen zero level; it can be negative.

Unit: meter · \mathrm{м}

Lesson formulas

3 formulas

Machine efficiency

\eta = \frac{A_{\text{пол}}}{A_{\text{затр}}}

Efficiency equals useful work divided by total input work.

Potential energy near Earth

E_p = mgh

A raised object's potential energy equals mass multiplied by gravitational acceleration and height.

Kinetic energy

E_k = \frac{mv^2}{2}

Kinetic energy equals half the mass multiplied by the square of speed.

Test the relationship

Make a prediction first. The button changes the stated quantity; then compare the result and explore other values.

Falling and energy transfer

h = h₀ − gt²/2; v = gt; Eп = mgh; Eк = mv²/2

Free fall from rest, g = 10 m/s², no air resistance. h is height above ground; v is the downward speed. Potential energy is zero at the ground. The model stops immediately before impact.

At the same height, mass increases from 2 to 4 kg. How will total mechanical energy change?

Your prediction

Initial values

h = 0h, мEпEк
0-120.25190.5500.75811112E, Джt, с
Eп Eк

Calculated result

h
5 м
v
0 м/с
Eп
100 Дж
Eк
0 Дж
E
100 Дж
Explaining the result

The decrease in potential energy equals the increase in kinetic energy. Mass scales both energies but does not change fall time. Impact and later dissipation are not modelled.

Related formulas

The same formulas in the reference, with symbols and units.

Problems on this topic

Statements, answer options and the walkthrough.