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given to the obstacle</p><pb/>
given to the obstacle</p><pb/>


Collect the Tables giving the proportion os expansion in air to the quantity of caloric applied to it As oxygen is but 1/4 of the air no more 'caloric can be ?? applied than is contained in that 1/4 parT: even ??eppering the fewel to be ?? applied as to employ the whole of the air. But the increase in 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
<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 <gap/> 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 <unclear>Lavoisiers</unclear><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>
 
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/>


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Revision as of 20:57, 6 February 2015

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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
cou?inually 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---



Identifier: | JB/106/013/002"JB/" can not be assigned to a declared number type with value 106.

Date_1

1793-12

Marginal Summary Numbering

Box

106

Main Headings

Folio number

013

Info in main headings field

flash-pump

Image

002

Titles

flash & steam engine

Category

text sheet

Number of Pages

2

Recto/Verso

recto

Page Numbering

Penner

jeremy bentham

Watermarks

[[watermarks::[w with crown] [lion motif]]]

Marginals

Paper Producer

Corrections

Paper Produced in Year

Notes public

ID Number

34601

Box Contents

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