JB/106/067/001: Difference between revisions

Transcribe Bentham: A Collaborative Initiative

From Transcribe Bentham: Transcription Desk

Find a new page on our Untranscribed Manuscripts list.

JB/106/067/001: Difference between revisions

Keithompson (talk | contribs)
No edit summary
Keithompson (talk | contribs)
No edit summary
Line 10: Line 10:
or else by machanical agitation.</p>
or else by machanical agitation.</p>
<p>Steadiness within a certain range by a successive gradation of<lb/>
<p>Steadiness within a certain range by a successive gradation of<lb/>
temperattures as before explained.- But this will require the perfect<lb/>
temperatures as before explained.- But this will require the perfect<lb/>
steadiness of the two extreme point: <add>with respect to</add> <del>of</del> the lowermost we have<lb/>
steadiness of the two extreme points: <add>with respect to</add> <del>of</del> the lowermost we have<lb/>
a sufficiently perfect means of obtaining it by ice. The highest<lb/>
a sufficiently perfect means of obtaining it by ice. The highest<lb/>
may be obtained by making the supply of heat from a lamp<lb/>
may be obtained by making the supply of heat from a lamp<lb/>
for instance precisely <del>equivalent</del><add>equal</add> to the expendditure: which might<lb/>
for instance precisely <del>equivalent</del><add>equal</add> to the expenditure: which might<lb/>
easily be done after a few trials, were it not that the exxpendditure<lb/>
easily be done after a few trials, were it not that the expenditure<lb/>
<del>viz,</del> (depending of the lower temperature of the air) is variable.<lb/>
<del>viz(,</del> depending of the lower temperature of the air) is variable.<lb/>
this however might also be adjusted by repeated trials.</p>
this however might also be adjusted by repeated trials.</p>
<p>A more perfect method would be by employing a regulator<lb/>
<p>A more perfect method would be by employing a regulator<lb/>
Line 26: Line 26:
The whole <del>quanti</del> expansion should be made in the<lb/>
The whole <del>quanti</del> expansion should be made in the<lb/>
descending arch.</p>
descending arch.</p>
<p>{Plan of Frigidarium showing position of 40<hi rend="superscript">o</hi> 50<hi rend="superscript">o</hi> and 60<hi rend="superscript">o</hi> chamber}</p>
<p>{Plan of Contrivances showing position of 40<hi rend="superscript">o</hi> 50<hi rend="superscript">o</hi> and 60<hi rend="superscript">o</hi> chamber}</p>
<p>Air would be improper on account<lb/>
<p>Air would be improper on account<lb/>
of its <del>being in</del> bulk depending<lb/>
of its <del>being in</del> bulk depending<lb/>
Line 35: Line 35:
cold water or air</p>
cold water or air</p>
<p>h, pipe for admitting<lb/>
<p>h, pipe for admitting<lb/>
hot water or air
hot water or air<lb/>
or an instrument on the<lb/>
or an instrument on the<lb/>
hydrometer principle.</p>  
hydrometer principle.</p>  

Revision as of 12:02, 15 November 2015

Click Here To Edit |4
4o. Preservation of Uniformity & Steadiness of
Temperature

Uniformity preserved in fluids (with exception before mentioned)
applying heat at the topbottom & cold at the bottom top.
or else by machanical agitation.

Steadiness within a certain range by a successive gradation of
temperatures as before explained.- But this will require the perfect
steadiness of the two extreme points: with respect to of the lowermost we have
a sufficiently perfect means of obtaining it by ice. The highest
may be obtained by making the supply of heat from a lamp
for instance precisely equivalentequal to the expenditure: which might
easily be done after a few trials, were it not that the expenditure
viz(, depending of the lower temperature of the air) is variable.
this however might also be adjusted by repeated trials.

A more perfect method would be by employing a regulator
admitting hot water or air as it cooled: & letting out theas much cold water
as much colder water, or air: as by the following contrivances
Two thermometers filled with oil & rendered just boy
buoyant at 30o when immersed in water at 50o
but sinkingrising in higher heats and risingsinking in lower.
The whole quanti expansion should be made in the
descending arch.

{Plan of Contrivances showing position of 40o 50o and 60o chamber}

Air would be improper on account
of its being in bulk depending
on the pressure of the atmosphere
which is very variable.

{Sketch showing oil and water apparatus}

c, pipe for admitting
cold water or air

h, pipe for admitting
hot water or air
or an instrument on the
hydrometer principle.

{Two sketches of equipment showing position of cold and hot water inlets and valve for admitting hot water}


---page break---





Identifier: | JB/106/067/001"JB/" can not be assigned to a declared number type with value 106.

Date_1

Marginal Summary Numbering

Box

106

Main Headings

frigidarium

Folio number

067

Info in main headings field

Image

001

Titles

preservation of uniformity & steadiness of temperature

Category

copy/fair copy sheet

Number of Pages

4

Recto/Verso

recto

Page Numbering

f4 / / /

Penner

fr4

Watermarks

pot 1796

Marginals

Paper Producer

fc6

Corrections

Paper Produced in Year

1796

Notes public

includes drawings

ID Number

34655

Box Contents

UCL Home » Transcribe Bentham » Transcription Desk
  • Create account
  • Log in