Discussion
introduction
The word "engine" is a bit old fashioned. At one time, an engine was any kind of mechanical
contrivance. For example …
With the exception of the last example, the original meaning of the word
engine is now pretty much obsolete. This can be traced back to the development
of the steam engine in the middle of the Nineteenth Century. Nowadays, an engine generally refers
to a device that transforms heat into mechanical energy. Technically, such
a device is a heat engine, but in the current era, the adjective "heat" is generally dropped.
Although the two devices are often confused, an engine is not the same as
a motor. An electric motor (often just called a motor) is a device for transforming electrical energy into mechanical energy.
… What about compressed air motors?
This gives rise to several linguistic problems. Why are automobiles sometimes
called "motorcars"? Many cars do have motors in them, but the device responsible for propelling
them isn't a motor. It's an engine. At the dawn of the Twenty First Century
cars use motors to drive the wiper blades, open and close the windows, adjust the seat and
side view mirrors, and spin CDs; but they only use an engine to drive the wheels (although this is likely to change). The largest auto
maker in the US may be called General Motors, but what they really sell
are automobiles driven by engines.
The description of an engine is very simple, but it refers to a wide variety
of different devices. Engines can be found in cars, trucks, motorcycles,
planes, boats, ships, trains, lawnmowers, chain saws, model airplanes,
portable generators, cranes, augers, drills, and rockets (to give but a
few examples). Engines can be classified according to one or more of several
schemes.
- by the motion of its parts
- Reciprocating Engine
pistons going up and down
piston arrangements: V, W, inline/straight, flat, radial
- Rotary Engine
parts that spin like in a wankel, turbine, turbocharger, jet turbine,
turbojet, fanjet
- Rocket Engine
need not have any moving parts, motion is strictly produce by action-reaction,
hot gases are expelled backward, rocket goes forward, also known
as reaction engines
- Unknown
ramjet, scramjet
- by where the fuel is burned
- Internal Combustion
fuel is burned inside the chamber containing the working fluid (air)
- External Combustion
fuel is used to heat the working fluid (air, liquid water, steam,
molten sodium)
- by the manner in which fuel is burned
- Continuous Combustion
a steady flow of fuel burns in a steady flame
- Intermittent Combustion
discrete amounts of fuel are periodically burned
- by the cycle through which the operating gas is run
- Otto Cycle
Nikolaus Otto (1831-1891) Germany, conceived in 1861, built in 1876
gasoline powered cars
- Diesel Cycle
Rudolph Diesel (1858-1916) Germany, patented in 1892, successfully built in 1897
trucks, locomotives; intended to used powdered coal but usually burn diesel oil, but can also run on vegetable oil (biodiesel)
- Rankine Cycle
William Rankine (1820-1872) Scotland, described in 1859
steam turbines, Watt's engine, Newcomb's engine
- Brayton Cycle
George Brayton (1830-1892) US, first proposed the concept in 1873
gas turbines, jets
- Miller Cycle
Ralph Miller (0000–0000) US, 1940s
Mazda, version of the forced induction Otto-cycle, asymmetric valve timing
- Wankel Cycle
Felix Wankel (1902-1988) Germany, designed 1954 tested 1957
Mazda again, very few moving parts
- Stirling Cycle
Robert Stirling (1790-1878) Scotland, invented in 1816
works on any temperature difference, high efficiency, low to no exhaust (OTEC: Ocean Thermal Energy Conversion), high manufacturing cost
otto cycle
Start with piston diagrams.
[magnify]
Describe each part of the cycle
Then move on to PV diagrams (indicator diagrams).
James Watt called them indicator
diagrams rather than pressure-volume graphs since the word graph hadn't
been invented
yet.
A steam-indicator is a device for plotting the pressure in the cylinder of
a steam engine as a function of the phase of the engine's working cycle.
The shape of this diagram reveals possible faults of the machine. With
a planimeter one can determine the mean effective steam pressure in the
engine or, when the stroke and diameter of the cylinder and the number
of revolutions per minute are known, the power of the engine,
A history lesson from The Canadian Museum of Making
Watt & Southern, c. 1796 The indicator was soon adapted to provide a written record of each individual application instead of merely a transient observation. This was a tremendous analytical breakthrough, allowing, as it did, an accurate picture to be formed of the pressure of steam at any time during the movement of the piston. The inspiration was due to John Southern (1758-1815), Watt's draughtsman, who recorded in a letter dated 14th March 1796 that he had 'contrived an instrument that shall tell accurately what power any engine exerts'.
[magnify]
- intake stroke
The piston starts out at the top of the cylinder and moves downward.
The volume above the piston expands, drawing air and fuel into the
combustion chamber. Since the intake valve is open during this stroke,
the pressure inside the cylinder will be constant and roughly equal
to the pressure of the environment. This segment of the cycle is thus
represented by a horizontal line (an isobar) running from left to right (from minimum to maximum volume). Assuming the amount of gas within the
cylinder increases in proportion to its volume, there is effectively
no change in its temperature.
- compression stroke
Both valves are closed and the gas is squeezed rapidly inside the cylinder.
Since the process is rapid, there is essentially no time for heat to
be lost to the environment. This segment of the cycle is thus represented
by an adiabat running from right to left. Since adiabats are steeper than isotherms, this segment crosses a few isotherms;
which is in agreement with our expectation that the temperature should
increase. Since the curve runs "backward", the area under it is negative; that is, work is being done on the gas.
- ignition
Igniting the fuel-air mixture inside the cylinder does two obvious things:
it raises the temperature and it raises the pressure above the piston.
It occurs so rapidly, however, that there isn't a lot of time for the
piston to react and the volume above it is effectively constant. This
segment of the cycle is thus represented by a vertical line (an isochor) running from bottom to top. The curve crosses several isotherms (since the fuel-air mixture's heat
of combustion is dumped into the system), but no work is done on or
by the gas (since the area under a vertical line is zero).
- power stroke
The piston is pushed down by the intense pressure following ignition.
Volume increases but it happens so quickly that the heat lost to the
environment is minimal. This segment of the cycle is thus represented
by an adiabat running from left to right. Since this curve runs "forward" the area under it is positive and work is done on the environment. That's
why it's called the "power stroke". This is the only part of the cycle that results in any useful work being
done. Since the curve of the power stroke is higher than the curve
of the compression stroke, the net work of the gas is positive. Thus
(overall) each cycle does work on the environment. This makes sense
as engines are a devices for doing work. In addition, the curve crosses
several isotherms. Closer inspection of the indicator diagram shows
that more isotherms are crossed during the power stroke than were crossed
during the compression stroke. This is an important observation that
sets us up for the next part of the cycle.
- valve exhaust
The valve is popped open at the end of the power stroke, which reduces
the pressure inside the cylinder to the pressure of the environment.
It occurs so rapidly, however, that the volume above the piston does
not effectively change. This segment of the cycle is thus represented
by a vertical line (an isochor) running from top to bottom. Since the graph is vertical, no work is done on or by the gas at this time.
The line does cross several isotherms, however, which means that internal
energy is decreasing. Since no work is done, this decrease must be
as a result of heat exhausted to the environment. In accordance with
the work-energy theorem, this heat lost is less than the heat gained
during combustion (the difference between them being equal to the net
work done by the gas).
- exhaust stroke
The last part of the cycle returns the system to its initial conditions.
Since the exhaust valve is open during this portion of the cycle, the
pressure inside the cylinder is effectively equal to that of the environment,
but since the piston is moving upward, the volume above it decreases.
This segment of the cycle is thus represented by a horizontal line
(an isobar) running from right to left (from maximum to minimum volume). Assuming the amount of gas within the
cylinder decreases in proportion to its volume, there is effectively
no change in its temperature. In addition, the area under this segment
is equal and opposite the area under the intake stroke. Thus (in the
ideal world, at least) no work is done on or by the gas as it is drawn
into and forced out of the cylinder.
And lastly, the essence of engines.
| The waterwheel heat engine analogy |
| aspect |
waterwheel |
heat engine |
| working fluid |
water |
heat (caloric) |
| gradient |
height difference between high and low water reservoirs |
temperature difference between hot and cold thermal reservoirs |
Add bridge text.
[magnify]
Efficiency in general vs. efficiency in engines. What symbol would you prefer:
η [eta] or ℰ [script capital e] or e [lowercase e]?
| efficiency = |
work out |
= |
Qhot − Qcold |
= 1 − |
Qcold |
| energy in |
Qhot |
Qhot |
Efficiency applies to more than just engines.
| Selected Efficiencies |
| action or device |
peak efficiency (%) |
| human, swimming, surface |
2 |
| human, swimming, underwater |
4 |
| human, shoveling |
3 |
| steam engine |
17 |
| human, cycling |
25 |
| reciprocating gasoline engine |
30 |
| natural gas turbine |
40 |
| Wärtsilä RTA96C |
50 |
| muscle contractions |
50 |
| combined cycle (gas-steam) turbine |
60 |
| fuel cell |
60 |
| electric motor |
80 |
| combined heat and power turbine |
95 |
other cycles
- diesel cycle (turbo-diesel)
- enter turbocharger
- air at atmospheric pressure and temperature
- turbocharger compression
- adiabatic compression by turbine
- open both valves on piston
- air only blown into piston (no risk of blowing unburned fuel out the exhaust valve like a two-stroke engine)
- Win
- compression stroke
- close intake valve
- piston moves up
- adiabatic compression
- higher compression than otto cycle
- temperature increases beyond the ignition point (no fuel - no danger of preignition)
- Win
- fuel injection
- piston moves down
- no spark plug, spontaneous ignition
- exploding fuel keeps pressure constant (idealization)
- isobaric expansion (horizontal line on PV diagram)
- Qhot and Wout
- power stroke
- piston continues moving down
- adiabatic expansion
- one useful stroke out of two
- Wout
- turbocharger expansion
- open both valves
- adiabatic expansion of exhaust continues outside the cylinder
- turbine extracts a portion of the residual energy to power blower
- Wout
- exit turbocharger
- isochoric pressure drop (vertical line on PV diagram)
- pressure and temperature return to atmospheric values
- Qcold
- rankine cycle (steam turbine)
- water in
- water pumped into high pressure boiler
- isochoric pressure increase
- Win
- vaporization
- water heated to boiling point
- isobaric, isothermal expansion
- volume increases due to phase change
- Qhot
- expansion
- superheated dry steam into turbine
- adiabatic expansion
- cooled wet steam exists turbine
- Wout
- condensation
- water condenses (eventually)
- isobaric, isothermal compression
- volume decreases due to phase change
- Qcold
- stirling cycle (two pistons with regenerator baffles)
- compression stroke
- isothermal contraction
- momentum caries cold piston forward
- compression beginning in cold piston (assisted by contraction of cooling gas)
- heat exits to cold reservoir
- hot piston remains stationary
- Qcold and Win
- regeneration
- isochoric (both pistons move equally)
- compression ending in cold piston
- flow of cold gas through regenerator
- heat extracted from regenerator to prewarm gas
- expansion beginning in hot piston
- −Qregenerator
- power stroke
- isothermal expansion
- cold piston remains stationary
- momentum caries hot piston forward
- hot piston continues expanding (assisted by expansion of hot gas)
- Qhot and Wout
- regeneration
- isochoric (both pistons move equally)
- cold piston expands
- hot piston contracts
- flow of hot gas through regenerator
- heat extracted from regenerator to precool gas
- +Qregenerator