Work, energy, and power
Module 3 (3): Forces and motion3.3 Work, energy, and power |
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| 3.3.1 |
Work and conservation of energy a) Work done by a force; the unit joule b) [math]W = Fx \cos\theta[/math] for work done by a force c) The principle of conservation of energy d) Energy in different forms; transfer and conservation |
| 3.3.2 |
Kinetic and potential energies a) Kinetic energy of an object;[math]E_k = \frac{1}{2} mv^2[/math] b) Gravitational potential energy of an object in a uniform gravitational field;[math]E_p = mgh[/math] c) The exchange between gravitational potential energy and kinetic energy.
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| 3.3.3 |
a) Power; the unit wat;[math]P = \frac{W}{t}[/math] c) Efficiency of a mechanical system; [math]\text{Efficiency} = \left(\frac{\text{useful output energy}}{\text{total input energy}}\right) \times 100\%[/math] |
1. Work and conservation of energy:
- Work is the transfer of energy from one object to another through a force, while conservation of energy is the principle that energy cannot be created or destroyed, only converted.
- Work is a scalar quantity, while energy is a scalar quantity that can take various forms (kinetic, potential, thermal, etc.).
- Work is done over a distance, while conservation of energy is a statement about the total energy of a system over time.
- Work and conservation of energy are related but distinct concepts. Work is the transfer of energy through a force, while conservation of energy is the principle that energy is conserved and converted between forms.
a) Work done by a force; the unit joule
- Work done by a force is a fundamental concept in physics, and it’s measured in units of joules (J).
- Work (W) is done when a force (F) is applied to an object and the object moves in the direction of the force.
- Formula:
- [math] W=F.x \\W=Fdcosθ [/math]
- Work is a scalar quantity, meaning it has only magnitude (amount of work) but no direction.
- The unit of work is typically measured in Joules (J).
- Conditions:
- Positive work: when the force and displacement are in the same direction.
- W = Fdcosθ θ=0°
W = Fd(1)
W = Fd 
- Figure 1 Displacement covers in the direction of applied force
-

Figure 2 negative work - Negative work: when the force and displacement are in opposite directions (e.g., lowering a book)
W = Fdcosθ θ = 180°
W = Fd(-1)
W = – Fd
-

Figure 3 Zero work doneZero work: when the force and displacement are perpendicular (e.g., pushing a wall)
- W=Fdcosθ θ = 90
W=Fd(0)
W=0
⇒ Examples
(1)
- Tracy is doing some weight training.
- She is holding two weights but she is not moving them.
- She gets tired holding them out, and her arms convert chemical energy into heat energy, but no work is done as the weights do not move.
- Tracy does work when she lifts the weights.

Figure 4 Tracy is using energy but not working.
(2)
- Three people are helping to push-start a friend’s car.
- Salim and Anne are pushing at the back of the car.
- Here Salim and Anne are working, because they are pushing along the direction in which the car is travelling.
- Jim does no work as he is pushing at right angles to the direction of motion.

Figure 5 Salim and Anne are working but Jim is not working as he is pushing at right angles to the car
(3)
- Calculate the work done from Figure 6 when the object is displaced 40 m from its original position.

Figure 6 Calculate the work done by considering a small displacement,[math]\vec{d}[/math] , when the applied force is [math]\vec{F}[/math] - Given data:
Displacement [math] = \vec{d} = 40m[/math]
Force = The area under a force [math] = \vec{F} \frac{1}{2} (150N + 300N) [/math]
Find data:
Work done = ?
Formula:[math]W = \vec{F} \cdot \vec{d}[/math]
Solution:
[math]W = \vec{F} \cdot \vec{d} \\
W = 225 * 40\\
W=9000J [/math]
c) The principle of conservation of energy:
- The principle of conservation of energy states that energy cannot be created or destroyed, only converted from one form to another.
- In other words, the total energy of an isolated system remains constant over time.
- This means that the sum of all the different types of energy within a system (kinetic, potential, thermal, electrical, etc.) remains the same at all times.
- Energy can be converted from one form to another, but the total energy remains constant.
- [math]\text{Total kinetic energy} = \text{total potential energy}[/math]
⇒ Examples:
(1)
- A boy throws a ball upwards with a speed of 16m/s.
- It leaves his hand at a height of 1.5m above the ground.
- Calculate the maximum height to which it rises
Solution: -
- The ball gains gravitational potential energy as it rises and loses kinetic energy when it leaves the boy’s grasp.
- The ball stops travelling at its highest point, converting all of its kinetic energy to potential energy.
- Given data:
Velocity = 16m/s - Find data:
Maximum height = ? - Formula:

- Solution:

- but the total height gained is 13m + 1.5m = 14.5m.
(2)
- A stretched catapult stores 0.7J of elastic potential.
- The catapult is used to launch a marble of mass 0.01kg.
- Calculate the initial speed of the marble.
Given data:
The stored elastic potential energy in the catapult is transferred to the marble’s kinetic energy.
Elastic potential energy ([math]\Delta E_ep)= 0.7J
Mass = 0.01kg
Find data:
Speed (velocity) = V= ?
Formula:
[math] \Delta E_{\text{ep}} = \Delta E_k[/math]
Solution:

Putting Values:

e) Transfer of energy is equal to work done.
- The transfer of energy is equal to the work done. This is a fundamental concept in physics, and it’s expressed mathematically as:
- [math]ΔE = W [/math]
- Where:
- ΔE is the change in energy
- W is the work done
- This equation states that the change in energy of an object or system is equal to the work done on it. In other words, the energy transferred to or from an object is equal to the work done on it.
- For example, if you lift an object, the work done is equal to the energy transferred to the object, which is now in the form of potential energy. Similarly, if you push an object, the work done is equal to the energy transferred to the object, which is now in the form of kinetic energy.
- This concept is a fundamental principle in physics and engineering, and it has numerous applications in various fields, including mechanics, thermodynamics, and electromagnetism.
- Energy can take various forms, such as kinetic energy, potential energy, thermal energy, and more.
- Work done is the transfer of energy from one object to another through a force.
- The unit of work and energy is the same, which is joule (J).
- The equation is a fundamental principle that relates the change in energy to the work done.
2. Kinetic and potential energy:
a) Kinetic energy of an object:
- Kinetic energy is the energy of motion. It’s the energy an object possesses due to its motion, and it’s defined as the work required to bring the object to rest.
- In other words, it’s the energy an object has because it’s moving.
- Kinetic energy is a scalar quantity, meaning it has only magnitude (amount of energy) but no direction.
- The more massive an object is and the faster it moves, the more kinetic energy it has.
- Kinetic energy can be converted into other forms of energy, such as potential energy, and vice versa.

Figure 7 A constant force accelerates a car- In Figure 7, a constant force F accelerates a car, starting at rest, over a distance s.
- Work is done to increase the kinetic energy of the car.
- We can use this idea to find a formula for kinetic energy, Ek, in terms of the car’s speed and mass.
- [math]\Delta E_k = F s \qquad (1)[/math]
- but from Newton’s Second Law:
- F = ma
- and from the equations of motion:
- [math] s = \frac{1}{2} a t^2[/math]
- Put in equation 1
- [math]\Delta E_k = ma * \frac{1}{2} at^2 \\ \Delta E_k = \frac{1}{2}ma^2t^2 [/math]
- Since

- So the kinetic energy of a body of a mass m, moving at a velocity v, is given by:
[math] E_k = \frac{1}{2} mv^2 [/math]
Note this is a scalar quantity because [math]v^2[/math] has no direction
b) Gravitational potential energy
- Gravitational potential energy is the energy an object possesses due to its height or position in a gravitational field.

Figure 8 gravitational potential energy converted into the kinetic energy - It’s the energy an object has because of its potential to fall or move downward.
- Gravitational potential energy is a type of potential energy, which means it has the potential to become kinetic energy (the energy of motion).
- The higher an object is, the more gravitational potential energy it has.
- Gravitational potential energy is always relative to a reference level, such as the ground or a table.
- When an object falls or moves downward, its gravitational potential energy is converted into kinetic energy.
- A ball at the top of a point has gravitational potential energy due to its height.
- We can calculate the gravitational potential energy by using formula
- ∆Ep = mg∆h
- Where
- ΔEp is gravitational potential energy
- m is mass of an object
- g is gravitational acceleration
- ∆h is height of an object in which potential energy store
- In Figure 8 a load with a weight W, has been lifted through a height ∆h.
The work done = increase in gravitational potential energy. - Work = W * Δh
Weight W=mg
- So, the increase in potential energy, , is given by
- ∆Ep = mg∆h

- Figure 9 A load with a weight W lifted through a height Δh.
c) The exchange between gravitational potential energy and kinetic energy:
- The exchange between gravitational potential energy (GPE) and kinetic energy (KE) occurs in the following ways:
- GPE → KE
- – An object’s height or position (GPE) is converted into motion (KE) as it falls or descends.
- The force of gravity acts on the object, increasing its velocity and KE.
- KE → GPE
- An object’s motion (KE) is converted into height or position (GPE) as it rises or climbs.
- The object’s velocity decreases, and its KE is converted into GPE.
- This conversion is illustrated in the following examples:
- – A ball rolling down a hill: GPE → KE
- A roller coaster climbing up an incline: KE → GPE
- A thrown ball flying upwards: KE → GPE
- A satellite orbiting the Earth: KE → GPE (and vice versa)
- The equation relating GPE and KE is:
- [math]GPE = mgh \\ KE = \frac{1}{2} mv^2 [/math]
- Where:
- – m is the mass of the object
- – g is the acceleration due to gravity (approximately [math]9.8 m/s ^2 [/math] on Earth)
- – h is the height or position of the object
- – v is the velocity of the object
3. Power
- Power is the rate at which work is done or energy is transferred.
- It’s the amount of energy transferred per unit time.
- In other words, power is the measure of how quickly energy is used or produced.
- Formula:
- [math] \text{Power} = \frac{\text{energy transferred}}{\text{time}} \quad \text{or} \quad \frac{\text{work done}}{\text{time}} [/math]
- The unit of power is the watt (W), or J/s.
- This definition can be used to produce a useful formula to calculate the power transferred by moving vehicles.
- [math] \text{Power} = \frac{\text{work done}}{\text{time}} \quad \text{or} \quad \frac{\text{W}}{\text{t}} \\ \text{Power} = \frac{\vec{F} \cdot \vec{s}}{t}[/math]
-
or
- [math]\text{Power} = \vec{F} \cdot \vec{v} [/math]
- Power (P) is the rate of energy transfer (measured in watts, W)
- Work (W) is the energy transferred (measured in joules, J)
- Time (t) is the time over which the energy is transferred (measured in seconds, s)
⇒ Example:
- A car is moving at a constant speed of 18m/s. The frictional forces acting against the car are 800N in total. The car has a mass of 1200kg.
- a) Calculate the power transferred by the car on a level road.
- b) The car maintains its constant speed while climbing a hill of vertical height 30m in 16s. Calculate the power transferred by the car now.
Given data:
Speed = 18m/s
Force = 800N
Mass = 1200 kg
Find data:
(a) Power transferred by the car on a level road = ?
(b) Power transferred by the car when car climbing a hill = ?
Vertical height = 30m
Time taken = 16s
Formula:
[math]\text{(a)} \quad \text{Power} = \vec{F} \cdot \vec{v}\\
\text{(b)} \quad \text{Power} = \text{previous power} + \frac{W}{t}\\
\text{Power} = \text{previous power} + \frac{mg \Delta h}{t} [/math]
Solution:
[math] \text{(a)} \quad \text{Power} = \vec{F} \cdot \vec{v}\\
\text {Power} = 800 * 18 [/math]
(a) Power transferred by the car on a level road
[math] \text{Power} = 14 \, \text{KW} [/math]
(b) Power transferred by the car when car climbing a hill
[math]\text{Power} = \text{previous power} + \frac{mg \Delta h}{t} \\
\text{Power} = 14000 + \frac{1200(9.8)(30)}{16} \\
\text{Power} = 14000 + 22050\\[/math]
[math]\text{Power} = 36 \text{KW}[/math]
⇒ Efficiency
- Efficiency is a measure of how well a system or process uses energy to produce a desired output.
- It’s defined as the ratio of useful output energy to input energy.
- Formula:
- [math]\text{Efficiency} = \frac{\text{useful output energy}}{\text{input energy}} \\ \text{Efficiency} = \frac{\text{useful output energy}}{\text{input energy}} \times 100\% [/math]
- Efficiency is usually expressed as a percentage, with 100% being the maximum possible efficiency.
- In reality, no system can achieve 100% efficiency, as some energy is always lost as waste heat, friction, or other forms of energy.
- Types of efficiency:
- Mechanical efficiency: measures the efficiency of machines or mechanisms.
- Thermal efficiency: measures the efficiency of energy conversion from heat to work.
- Electrical efficiency: measures the efficiency of electrical systems or devices.
- Energy efficiency: measures the efficiency of energy use in buildings, industries, or processes.
- Efficiency is important because it:
- Saves energy and resources
- Reduces waste and pollution
- Increases productivity and performance
- Saves money and reduces costs
- Sankey diagram: A particular flow diagram where the width of the indicated arrows corresponds to the flow amount. This chapter uses Sankey diagrams to illustrate the flow of energy through different processes.

-
Figure 12 Sankey diagram
⇒ Example
- A Sankey diagram illustrating the conversion of 100J of electrical energy into different forms of energy may be seen in Figure 12.
- Just 30J of the energy is converted into useable gravitational potential energy.
- The rest is converted to heat and sound energy.
- [math]\text{Efficiency} = \frac{\text{useful output energy}}{\text{input energy}} \\
\text{Efficiency} = \frac{30 \, \text{J}}{100 \, \text{J}} \\
\text{Efficiency} = 0.3 \text{ or } 30\% [/math]