Agenda:
• Energy, Power & Climate Change
Types of Energy
Heat Chemical
Light Gravitational
Sound Elastic/strain
Kinetic Nuclear
Electric
The Law of Conservation of
Energy
Energy can be changed
(transformed) from one
type to another, but it can
never be made or
This means that
the total amount of energy in the
Energy Flow diagrams
We can write energy flow diagrams to show the energy changes that occur in a given
situation.
For example, when a car brakes, its kinetic energy is transformed into heat energy in the brakes.
Kinetic heat
Other examples
When a rocket launches.
Chemical kinetic gravitational
sound
Energy degradation!
In any process that involves energy transformations, the
energy that is transferred to the surroundings (thermal energy) is no longer available to perform
Energy transfer (change)
A lamp turns
electrical energy into heat and
Sankey Diagram
Sankey Diagram
Sankey Diagram
Notice that the total amount of energy
Efficiency
Efficiency
Efficiency is defined as
Example
Efficiency = 75 = 0.15
Energy efficient light bulb
Efficiency = 75 = 0.75
100 That’s much
Energy Density
• The energy that can be obtained from a unit
mass of the fuel
• J•kg-1
• If the fuel is burnt the energy density is
Energy density
• Coal - 30 MJ.kg-1
• Wood - 16 MJ.kg-1
• Gasoline – 47 MJ.kg-1
Hydroelectric energy density?
• Imagine 1 kg falling 100m.
• Energy loss = mgh = 1x10x100 = 103 J
• If all of this is turned into electrical energy
it gives an “energy density” of the “fuel” of
Electromagnetic induction
If a magnet is
moved inside a coil an electric current is induced
Electromagnetic induction
A electric current is induced because the
Generator/dynamo
A generator
works in this way by rotating a coil in a magnetic
Non-renewable
• Finite (being depleted – will run out)
• In general from a form of potential energy
Renewable
• Mostly directly or indirectly linked with the
sun
World energy production
Fuel % total energy
production CO2g.MJ emission -1
Oil 40 70
Natural gas 23 50
Coal 23 90
Nuclear 7
-Hydroelectric 7
-Electricity production
Fossil fuels
In electricity production they are burned, the heat is used to heat water to make
Fossil fuels - Advantages
• Relatively cheap
• High energy density
• Variety of engines and devices use them
directly and easily
• Extensive distribution network in place
Fossil fuels - Disadvantages
• Will run out (finite)
• Burning coal can cause acid rain • Oil spillages etc.
• Contribute to the greenhouse effect by
A coal powered power plant has a power output of 400 MW and operates with an overall efficiency of
35%
• Calculate the rate at which thermal energy
is provided by the coal
Efficiency = useful power output/power input
Power input = output/efficiency
A coal powered power plant has a power output of 400 MW and operates with an overall efficiency of
35%
• Calculate the rate at which coal is burned (Coal energy density = 30 MJ.kg-1)
1 kg of coal burned per second would produce 30 MJ. The power station needs 1.1 x 103 MJ per
second. So
Mass burned per second = 1.1 x 103/30 = 37 kg.s-1
A coal powered power plant has a power output of 400 MW and operates with an overall efficiency of
35%
• The thermal energy produced by the power plant is removed by water. The temperature of the water must not increase by moe than 5 °C. Calculate the rate of flow of water.
Rate of heat loss = 1.1 x 103 – 0.400 x 103 = 740 MW
In one second, Q = mcΔT
740 x 106 = m x 4200 x 5
m = 35 x 103 kg
Uranium
Uranium 235 has a large unstable nucleus.
Capture
Capture
Fission
The Uranium 236 is very unstable and splits
Free neutrons
As well as the two smaller nuclei (called
Fission
Chain Reaction
If there is enough uranium (critical mass) a
chain reaction occurs. Huge amounts of
energy are released very quickly.
Bang!
Controlled fission
The chain reaction can be controlled
using control rods
and a moderator.
Fuel rods
• In a Uranium reactor these contain Enriched
Uranium (the percentage of U-235 has been
Moderator
This slows the free neutrons down, making them easier to absorb by the uranium 235 nuclei. Graphite or water is normally used.
Control rods
Heat
Heat
This heat is used to heat water (via a heat
Useful by-products
Uranium 238 in the fuel rods can also
absorb neutrons to produce plutonium 239
which is itself is highly useful as a nuclear fuel (hence breeder reactors)
Nuclear power - Advantages
• High power output
Nuclear power - disadvantages
• Waste products dangerous and difficult to
dispose of
• Major health hazard if there is an accident • Problems associated with uranium mining • Nuclear weapons
The solar constant
The solar constant
The sun’s total power output is 3.9 x 1026 W!
Only a fraction of this power actually reaches the earth, given by the formula
I (Power per unit area) = P/4πr2
The solar constant
For the earth this is 1400 W•m-2 and is called the solar constant
The solar constant
The solar constant
This 1400 W•m-2 can only shine on the cross sectional area of the earth as seen from the sun.
Area = πr
e2However, as the earth turns this is spread over the TOTAL surface area
The solar constant
Therefore the average intensity of the sun falling on the earth = (πre2/4πr
e2) 1400 W•m-2
Solar power - advantages
• “Free” once built • Renewable
Solar power - disadvantages
• Only works during the day • Affected by cloudy weather • Low power output
Water storage in lakes
Pumped storage
• Excess electricity can be used to pump
Tidal water storage
• Tide trapped behind a tidal barrage. Water
Hydroelectric - Advantages
• “Free” once built • Renewable
Hydroelectric - disadvantages
• Very dependent on location
Wind power
Wind moving at speed
v, cross
sectional area of turbines =
A
V
Wind moving at speed
v, cross
sectional area of turbines =
A
V
A
Wind moving at speed
v, cross
sectional area of turbines =
A
V
A
Mass of air per second = ρAv
If all kinetic energy of air is transformed by the turbine, the amount of energy produced per second = ½mv2 = ½ρAv3
Wind power - advantages
• “Free” once built • Renewable
• Clean
Wind power - disadvantages
• Works only if there is wind! • Low power output
• Unsightly (?) and noisy
OWC
Modeling waves
• We can simplfy the mathematics by
modeling square waves.
λ L
Modeling waves
• If the shaded part is moved down, the sea
becomes flat.
λ L
Modeling waves
• The mass of water in the shaded part =
Volume x density = Ax(λ/2)xLxρ = AλLρ/2
λ L
Modeling waves
• Loss of Ep of this water = mgh = = (AλLρ)/
2 x g x A = A2gLρ(λ/2)
λ L
Modeling waves
• Loss of Ep of this water = mgh= A2gLρ(λ/2)
• # of waves passing per unit time = f = v/λ
λ L
Modeling waves
• Loss of Ep per unit time = A2gLρ(λ/2) x v/λ
• = (1/2)A2Lρgv
λ L
Modeling waves
• The maximum power then available per
unit length is then equal to = (1/2)A2ρgv
λ L
Power per unit length
A water wave of amplitude A carries an amount of power per unit length of its wavefront equal to
P/L = (ρgA2v)/2
Wave power - Advantages
• “Free” once built
• Reasonable energy density • Renewable
Wave power - disadvantages
• Only in areas with large waves • Waves are irregular
• Low frequency waves with high frequency
turbine motion
• Maintainance and installation costs high • Transporting power
Radiation
from the
Sun
Black-body radiation
• Black Body - any object that is a perfect
emitter and a perfect absorber of radiation
• object does not have to appear "black"
• sun and earth's surface behave
Black-body radiation
• http://phet.colorado.edu/sims/blackbody-sp
Wien’s law
Example
• The sun has an approximate black-body
spectrum and most of its energy is radiated at a wavelength of 5.0 x 10-7 m. Find the
surface temperature of the sun.
• From Wien’s law
5.0 x 10-7 x T = 2.9 x 10-3
Stefan-Boltzmann law
The amount of energy per second (power) radiated from a body depends on its surface area and absolute temperature according to
P = eσAT4
where σ is the Stefan-Boltzmann constant
(5.67 x 10-8 W.m-2.K-4) and e is the
Example
• By what factor does the power emitted by a
body increase when its temperature is increased from 100ºC to 200ºC?
• Emitted power is proportional to the fourth
The Sun
The sun emits electromagnetic waves
The earth
Reflected
Around 30% will be reflected by the earth and the atmosphere. This is called the earth’s albedo
(0.30). (The moon’s albedo is 0.12) Albedo is the ratio of reflected light to incident light.
Albedo
• The Albedo of a body is defined as the ratio
of the power of radiation reflected or
Albedo
Absorbed by the earth
Around 70% reaches the ground and is absorbed by the earth’s surface.
Absorbed by the earth
Infrared
Temperature of the earth with no
atmosphere?
• Remember the solar constant is around
1360 W.m-2. This can only shine on one
side of the Earth at a time, and since the
silhouette of the earth is a circle, the power incident = 1360 x πr2
Temperature of the earth with no
atmosphere?
• Power incident on earth = 1.75 x 1017 W
• Since the albedo is 30%, 70% of the
incident power will be absorbed by the Earth
Temperature of the earth with no
atmosphere?
Power absorbed by Earth = 1.23 x 1017 W At equilibrium,
the Power absorbed = Power emitted
Using the Stefan Boltzmann law;
Temperature of the earth with no
atmosphere?
Using the Stefan Boltzmann law;
1.23 x 1017 = eσAT4
1.23 x 1017 = 1 x 5.67 x 10-8 x 4πr2 x T4
Temperature of the earth with no
atmosphere?
T = 255 K (-18°C)
Absorbed by the earth
Infrared
Absorbed
• Various gases in the atmosphere can absorb
radiation at this longer wavelength (resonance)
Greenhouse gases
• These gases are known as “Greenhouse”
gases. They include carbon dioxide, methane, water and N2O.
Re-radiated
• These gases in the atmosphere absorb the
Balance
There exists a balance between the energy absorbed by the earth (and its atmosphere) and the energy emitted.
Balance
This means that normally the earth has a fairly constant average temperature
(although there have been big changes over
thousands of years)
Balance
Without this normal “greenhouse effect” the earth would be too cold to live on.
Greenhouse gases
• Most scientists believe that we are
producing more of the gases that absorb the infra-red radiation, thus upsetting the
balance and producing a higher equilibrium earth temperature. This is called the
What might happen?
What might happen?
• Higher sea levels and flooding of low lying
Coefficient of volume expansion
• Coefficient of volume expansion is defined
Coefficient of volume expansion
Given a volume V0 at temperature θ0, the volume after temperature increase of Δθ will increase by ΔV given byDefinition
Coefficient of volume expansion is the
fractional change in volume per unit temperature change.
Example
The area of the earth’s oceans is about 3.6 x 108 km2 and the average depth is 3.7 km.
Using γ = 2 x 10-4 K-1, estimate the rise in
Example
The area of the earth’s oceans is about 3.6 x 108 km2 and the average
depth is 3.7 km. Using γ = 2 x 10-4 K-1, estimate the rise in sea level
for a temperature increase of 2K. Comment on your answer.
Volume of water = approx depth x area
= 3.6 x 108 x 3.7
= 1.33 x 109 km3 = 1.33 x 1018 m3
ΔV = γV0Δθ
ΔV = 2 x 10-4 x 1.33 x 1018 x 2 = 5.3 x 1014 m3
Δh = ΔV/A = 5.3 x 1014/3.6 x 1014 = 1.5 m
What else might happen?
• More extreme weather (heatwaves,
What might happen?
What might happen?
Evidence?
• Ice core research • Weather records
Other possible causes of global
warming?
• Increase in solar activity
• Volcanic activity increasing CO2
concentrations
Surface heat capacitance C
sSurface heat capacitance is defined as the energy required to increase the temperature of 1 m2 of a surface by 1 K. Cs is measured
in J.m-2.K-1.
Example
• Radiation of intensity 340 W.m-2 is incident on the surface of a lake of
surface heat capacitance Cs = 4.2 x 108 J.m-2.K-1. Calculate the time to
increase the temperature by 2 K. Comment on your answer.
• Each 1m2 of lake receives 340 J.s-1
• Energy needed to raise 1m2 by 2 K = Q =
ACsΔT = 1 x 4.2 x 108 x 2 = 8.4 x 108 J
• Time = Energy/power = 8.4 x 108/340 =
2500000 seconds = 29 days
• Sun only shines approx 12 hours a day so