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<head>Flash P. Dec:<hi rend="superscript">r</hi> 1793</head> | |||
<head>Flash & Steam<lb/> | |||
Engine</head> | |||
<p>The power of a <lb/> | |||
Steam Engine is <lb/> | |||
limited by the Diameter <lb/> | |||
that can <lb/> | |||
be given to the Piston: <lb/> | |||
that of a Flash <lb/> | |||
Pump has no limitation.</p> | |||
<p>Steam can not <lb/> | |||
act but in proportion <lb/> | |||
as it is compressed <lb/> | |||
and <del>prevented from</del><lb/> | |||
<del>escaping</del> confined.</p> | |||
<p>The pressure is <lb/> | |||
between the surface <lb/> | |||
of the water and <lb/> | |||
the bottom of the piston.</p> | |||
<p>Do what you will <lb/> | |||
with the steam, it <lb/> | |||
can not act but in <lb/> | |||
proportion as it applies <lb/> | |||
itself to an <lb/> | |||
obstacle. moving in <add>reciprocating</add><lb/> | |||
a channel. <unclear>Its</unclear> <lb/> | |||
power will therefore <lb/> | |||
be limited by the <lb/> | |||
diameter that can <lb/> | |||
<unclear>conveniently</unclear> be given <lb/> | |||
to the channel and <lb/> | |||
by the weight or <lb/> | |||
other power of resistance <lb/> | |||
that can be <lb/> | |||
given to the obstacle</p><pb/> | |||
<p>Collect the Tables <lb/> | |||
giving the proportion <lb/> | |||
of expansion in air <lb/> | |||
to the quantity of <lb/> | |||
<unclear>caloric</unclear> applied to <lb/> | |||
it</p> | |||
<p>As the oxygen is <lb/> | |||
but 1/4 of the air <lb/> | |||
no more '<unclear>caloric</unclear><lb/> | |||
can be <del><gap/></del> applied <lb/> | |||
than is contained in <lb/> | |||
that 1/4 part: even <lb/> | |||
supposing the fewel to<lb/> | |||
be applied as to <lb/> | |||
employ the whole of <lb/> | |||
the air.</p> | |||
<p>But the increase <lb/> | |||
of temperature resulting <lb/> | |||
from the decomposition <lb/> | |||
of that quantity <lb/> | |||
of oxygen is <lb/> | |||
known by Lavoisiers<lb/> | |||
experiments: and if <lb/> | |||
the degree of expansion <lb/> | |||
is likewise known <lb/> | |||
this will shew the <lb/> | |||
utmost proportion <lb/> | |||
of air that can be <lb/> | |||
driven out by a <lb/> | |||
flash.</p> | |||
<p>If the first flash <lb/> | |||
has been perfectly <lb/> | |||
performed, nothing <lb/> | |||
can be gained by <lb/> | |||
a second but in proportion <lb/> | |||
as the air <lb/> | |||
has been changed in <add>the</add><lb/><pb/> | |||
the flash-chamber <lb/> | |||
since the first flash.</p> | |||
<p>Apply a Winnowing <lb/> | |||
Machine - <lb/> | |||
Making the Chamber <lb/> | |||
Square the <lb/> | |||
length of the Winnowing <lb/> | |||
machine <lb/> | |||
may be the length <lb/> | |||
of a side of the Square <lb/> | |||
But in this plan <lb/> | |||
in would be better <lb/> | |||
the square should <lb/> | |||
be an oblong Square :<lb/> | |||
that the ventilation <lb/> | |||
may be the more <lb/> | |||
speedily performed: <lb/> | |||
especially if the bulk <lb/> | |||
of the chamber be <lb/> | |||
considerable</p> | |||
<p>How to give admission <lb/> | |||
to the water <lb/> | |||
when the expansion <lb/> | |||
is at its <hi rend="underline">maximum</hi>.</p> | |||
<p>The expansion <lb/> | |||
opens a valve <lb/> | |||
On the ceasing of <lb/> | |||
the expansion the <lb/> | |||
valve closes.</p> | |||
<p>The closing of the <lb/> | |||
valve opens the <lb/> | |||
sluice which lets <lb/> | |||
in the water.</p> | |||
<p> | |||
The valve must be <lb/> | |||
as <hi rend="underline">sensible</hi> as possible.<lb/> | |||
It must consequently <lb/> | |||
be distinct from the <lb/> | |||
great valve for which <lb/> | |||
gives exit to the air.</p> <pb/> | |||
<p>In the Steam Engine <lb/> | |||
the Chamber must <lb/> | |||
be cast all in one <lb/> | |||
place viz: of Cast <lb/> | |||
Iron at the cheapest.</p> | |||
<p>That iron must be <lb/> | |||
of great strength and <lb/> | |||
of a strength increasing <lb/> | |||
in proportion to <lb/> | |||
the power of the steam <lb/> | |||
that is in proportion <lb/> | |||
to the size of the <lb/> | |||
Chamber</p> | |||
<p>In the Steam Engine <lb/> | |||
the whole of the water <lb/> | |||
in the Boiler must<lb/> | |||
be brought to the Boiling<lb/> | |||
Heat before any <lb/> | |||
steam is formed - before <lb/> | |||
any power is <lb/> | |||
produced and then</p> | |||
<p>2 There must be a <lb/> | |||
constant supply of <lb/> | |||
caloric to make up <lb/> | |||
for what is carried <lb/> | |||
off by the containing <add>surrounding</add><lb/> | |||
<add>bodies</add> vessel. Then</p> | |||
<p>3. There must be <lb/> | |||
another supply of <lb/> | |||
caloric to convert <lb/> | |||
the water into steam <lb/> | |||
But the quantity of <lb/> | |||
caloric absorbed by <lb/> | |||
a given weight of <lb/> | |||
water when converted <lb/> | |||
into steam is much <lb/> | |||
greater than the <lb/> | |||
quantity of caloric <lb/> | |||
absorbed by <del>a given</del> <lb/> | |||
the same weight of <lb/> | |||
air when expanded to <lb/> | |||
twice its bulk.</p> <pb/> | |||
<p>In the Flash Pump <lb/> | |||
the Chamber need <lb/> | |||
not be all of a piece <lb/> | |||
it may be of thin <lb/> | |||
lead or copper or it <lb/> | |||
be well supported <lb/> | |||
with brick work.</p> | |||
<p>The strength will <lb/> | |||
only be in proportion <lb/> | |||
to the quantity of <lb/> | |||
water in height: <lb/> | |||
i: if a <del><gap/></del> <unclear>fluid</unclear> in <lb/> | |||
an <gap/> state. <lb/> | |||
it will not increase <lb/> | |||
with the diameter <lb/> | |||
of the flash-chamber</p> | |||
<p>The Chamber <lb/> | |||
must certainly be <lb/> | |||
strong - but this only <lb/> | |||
at bottom: and <lb/> | |||
the strength <unclear>even</unclear><lb/> | |||
be given by arch <lb/> | |||
work, or by the <lb/> | |||
ground where circumstances <lb/> | |||
admitt <lb/> | |||
of its being built <lb/> | |||
low enough</p> | |||
<p><unclear>Nor need</unclear> the strength <lb/> | |||
be for a greater <lb/> | |||
part of the height <lb/> | |||
than that to which <lb/> | |||
the water will be <lb/> | |||
raised</p> | |||
<p>Suppose 1/2 the <lb/> | |||
utmost quantity of <lb/> | |||
the air that can be <lb/> | |||
driven out and <lb/> | |||
32 foot the height <lb/> | |||
to which the water <lb/> | |||
could rise if the <lb/> | |||
whole of the air were <lb/> | |||
driven out: - the <lb/> | |||
<gap/> 16 foot is the <lb/> | |||
utmost of the waters <lb/> | |||
rise by a single <add>flash</add></p><pb/> | |||
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{{Metadata:{{PAGENAME}}}} | {{Metadata:{{PAGENAME}}}}{{Completed}} |
Flash P. Dec:r 1793
Flash & Steam
Engine
The power of a
Steam Engine is
limited by the Diameter
that can
be given to the Piston:
that of a Flash
Pump has no limitation.
Steam can not
act but in proportion
as it is compressed
and prevented from
escaping confined.
The pressure is
between the surface
of the water and
the bottom of the piston.
Do what you will
with the steam, it
can not act but in
proportion as it applies
itself to an
obstacle. moving in reciprocating
a channel. Its
power will therefore
be limited by the
diameter that can
conveniently be given
to the channel and
by the weight or
other power of resistance
that can be
given to the obstacle
---page break---
Collect the Tables
giving the proportion
of expansion in air
to the quantity of
caloric applied to
it
As the oxygen is
but 1/4 of the air
no more 'caloric
can be applied
than is contained in
that 1/4 part: even
supposing the fewel to
be applied as to
employ the whole of
the air.
But the increase
of temperature resulting
from the decomposition
of that quantity
of oxygen is
known by Lavoisiers
experiments: and if
the degree of expansion
is likewise known
this will shew the
utmost proportion
of air that can be
driven out by a
flash.
If the first flash
has been perfectly
performed, nothing
can be gained by
a second but in proportion
as the air
has been changed in the
---page break---
the flash-chamber
since the first flash.
Apply a Winnowing
Machine -
Making the Chamber
Square the
length of the Winnowing
machine
may be the length
of a side of the Square
But in this plan
in would be better
the square should
be an oblong Square :
that the ventilation
may be the more
speedily performed:
especially if the bulk
of the chamber be
considerable
How to give admission
to the water
when the expansion
is at its maximum.
The expansion
opens a valve
On the ceasing of
the expansion the
valve closes.
The closing of the
valve opens the
sluice which lets
in the water.
The valve must be
as sensible as possible.
It must consequently
be distinct from the
great valve for which
gives exit to the air.
---page break---
In the Steam Engine
the Chamber must
be cast all in one
place viz: of Cast
Iron at the cheapest.
That iron must be
of great strength and
of a strength increasing
in proportion to
the power of the steam
that is in proportion
to the size of the
Chamber
In the Steam Engine
the whole of the water
in the Boiler must
be brought to the Boiling
Heat before any
steam is formed - before
any power is
produced and then
2 There must be a
constant supply of
caloric to make up
for what is carried
off by the containing surrounding
bodies vessel. Then
3. There must be
another supply of
caloric to convert
the water into steam
But the quantity of
caloric absorbed by
a given weight of
water when converted
into steam is much
greater than the
quantity of caloric
absorbed by a given
the same weight of
air when expanded to
twice its bulk.
---page break---
In the Flash Pump
the Chamber need
not be all of a piece
it may be of thin
lead or copper or it
be well supported
with brick work.
The strength will
only be in proportion
to the quantity of
water in height:
i: if a fluid in
an state.
it will not increase
with the diameter
of the flash-chamber
The Chamber
must certainly be
strong - but this only
at bottom: and
the strength even
be given by arch
work, or by the
ground where circumstances
admitt
of its being built
low enough
Nor need the strength
be for a greater
part of the height
than that to which
the water will be
raised
Suppose 1/2 the
utmost quantity of
the air that can be
driven out and
32 foot the height
to which the water
could rise if the
whole of the air were
driven out: - the
16 foot is the
utmost of the waters
rise by a single flash
---page break---
Identifier: | JB/106/013/002"JB/" can not be assigned to a declared number type with value 106. |
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1793-12 |
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106 |
|||
013 |
flash-pump |
||
002 |
flash & steam engine |
||
text sheet |
2 |
||
recto |
|||
jeremy bentham |
[[watermarks::[w with crown] [lion motif]]] |
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34601 |
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