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{{About|heat measuring devices|particle detectors|Calorimeter (particle physics)}}
== Nike Air Force  oder indem eine einzigartige ==


[[Image:Ice-calorimeter.jpg|150px|right|thumb|The world’s first '''ice-calorimeter''', used in the winter of 1782-83, by [[Antoine Lavoisier]] and [[Pierre-Simon Laplace]], to determine the [[heat]] evolved in various [[chemical change]]s; calculations which were based on [[Joseph Black]]’s prior discovery of [[latent heat]]. These experiments mark the foundation of [[thermochemistry]].]]
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A '''calorimeter''' (from [[Latin]] ''calor'', meaning [[heat]]) is an object used for [[calorimetry]], or the process of measuring the heat of [[chemical reaction]]s or [[physical change]]s as well as [[heat capacity]]. Differential scanning calorimeters, isothermal microcalorimeters, titration calorimeters and accelerated rate calorimeters are among the most common types. A simple calorimeter just consists of a thermometer attached to a metal container full of water suspended above a combustion chamber.
 
 
  <li>[http://www.bluboo.com.cn/bbs/forum.php?mod=viewthread&tid=263818&fromuid=20099 http://www.bluboo.com.cn/bbs/forum.php?mod=viewthread&tid=263818&fromuid=20099]</li>
To find the [[enthalpy]] change per [[Mole (unit)|mole]] of a substance A in a reaction between two substances A and B, the substances are added to a calorimeter and the initial and final [[temperature]]s (before the reaction started and after it has finished) are noted. Multiplying the temperature change by the mass and [[specific heat capacity|specific heat capacities]] of the substances gives a value for the [[energy]] given off or absorbed during the reaction. Dividing the energy change by how many moles of A were present gives its enthalpy change of reaction. This method is used primarily in academic teaching as it describes the theory of calorimetry. It does not account for the heat loss through the container or the heat capacity of the thermometer and container itself.
 
 
  <li>[http://josh99.egloos.com/1629781/ http://josh99.egloos.com/1629781/]</li>
==History==
 
In 1780, [[Antoine Lavoisier]] used a [[guinea pig]] in his experiments with the calorimeter, a device used to measure heat production. The heat from the guinea pig's respiration melted snow surrounding the calorimeter, showing that respiratory gas exchange is a combustion, similar to a candle burning.<ref>[http://www.ajcn.org/cgi/content/full/79/5/899S Buchholz, Andrea C; Schoeller, Dale A. (2004). "Is a Calorie a Calorie?". American Journal of Clinical Nutrition 79 (5): 899S–906S. PMID 15113737. Retrieved 2007-03-12]</ref>
  <li>[http://www.vlpa.org/Forum/default.aspx?g=posts&t=446664 http://www.vlpa.org/Forum/default.aspx?g=posts&t=446664]</li>
 
 
==Adiabatic calorimeters==
  <li>[http://www.achicourtautrement.fr/spip.php?article451/ http://www.achicourtautrement.fr/spip.php?article451/]</li>
An [[adiabatic process|adiabatic]] calorimeter is a calorimeter used to examine a runaway reaction.  Since the calorimeter runs in an adiabatic environment, any heat generated by the material sample under test causes the sample to increase in temperature, thus fuelling the reaction.
 
 
  <li>[http://www.pierre-le-jeune.info/spip.php?article3 http://www.pierre-le-jeune.info/spip.php?article3]</li>
No adiabatic calorimeter is adiabatic - some heat will be lost by the sample to the sample holder. A mathematical correction factor, known as the phi-factor, can be used to adjust the calorimetric result to account for these heat losses. The phi-factor is the ratio of the thermal mass of the sample and sample holder to the thermal mass of the sample alone.
 
 
</ul>
==Reaction calorimeters==
 
{{Main|Reaction calorimeters}}
A reaction calorimeter is a calorimeter in which a [[chemical reaction]] is initiated within a closed insulated container. Reaction heats are measured and the total heat is obtained by integrating heatflow versus time. This is the standard used in industry to measure heats since industrial processes are engineered to run at constant temperatures. Reaction calorimetry can also be used to determine maximum heat release rate for chemical process engineering and for tracking the global kinetics of reactions. There are four main methods for measuring the heat in reaction calorimeter:
 
===Heat flow calorimetry===
 
The cooling/heating jacket controls either the temperature of the process or the temperature of the jacket. Heat is measured by monitoring the temperature difference between heat transfer fluid and the process fluid. In addition, fill volumes (i.e. wetted area), specific heat, heat transfer coefficient have to be determined to arrive at a correct value. It is possible with this type of calorimeter to do reactions at reflux, although the accuracy is not as good.
 
===Heat balance calorimeter===
 
The cooling/heating jacket controls the temperature of the process. Heat is measured by monitoring the heat gained or lost by the heat transfer fluid.
 
===Power compensation===
Power compensation uses a heater placed within the vessel to maintain a constant temperature. The energy supplied to this heater can be varied as reactions require and the calorimetry signal is purely derived from this electrical power.
 
===Constant flux===
Constant flux calorimetry (or COFLUX as it is often termed) is derived from heat balance calorimetry and uses specialized control mechanisms to maintain a constant heat flow (or flux) across the vessel wall.
 
==Bomb calorimeters==
 
[[File:Bombenkalorimeter mit bombe.jpg|thumb|Bomb calorimeter]]
[[File:Bomb Calorimeter.png|thumb|Bomb calorimeter]]
 
A bomb calorimeter is a type of constant-volume calorimeter used in measuring the heat of combustion of a particular reaction. Bomb calorimeters have to withstand the large pressure within the calorimeter as the reaction is being measured. Electrical energy is used to ignite the fuel; as the fuel is burning, it will heat up the surrounding air, which expands and escapes through a tube that leads the air out of the calorimeter. When the air is escaping through the copper tube it will also heat up the water outside the tube.  The temperature of the water allows for calculating calorie content of the fuel.
 
In more recent calorimeter designs, the whole bomb, pressurized with excess pure oxygen (typically at 30atm) and containing a weighed mass of a sample (typically 1-1.5 g) and a small fixed amount of water (to saturate the internal atmosphere, thus ensuring that all water produced is liquid, and removing the need to include enthalpy of vaporization in calculations), is submerged under a known volume of water (ca.&nbsp;2000 ml) before the charge is electrically ignited. The bomb, with the known mass of the sample and oxygen, form a closed system - no gases escape during the reaction. The weighted reactant put inside the steel container is then ignited. Energy is released by the combustion and heat flow from this crosses the stainless steel wall, thus raising the temperature of the steel bomb, its contents, and the surrounding water jacket. The temperature change in the water is then accurately measured with a thermometer. This reading, along with a bomb factor (which is dependent on the heat capacity of the metal bomb parts), is used to calculate the energy given out by the sample burn. A small correction is made to account for the electrical energy input, the burning fuse, and acid production (by titration of the residual liquid). After the temperature rise has been measured, the excess pressure in the bomb is released.
 
Basically, a bomb calorimeter consists of a small cup to contain the sample, oxygen, a stainless steel bomb, water, a stirrer, a thermometer, the dewar  or insulating container (to prevent heat flow from the calorimeter to the surroundings) and ignition circuit connected to the bomb. By using stainless steel for the bomb, the reaction will occur with no volume change observed.
 
Since there is no heat exchange between the calorimeter and surroundings → Q = 0 (adiabatic) ; no work performed → W = 0
Thus, the total internal energy change  ΔU(total) = Q + W = 0
 
Also, total internal energy change ΔU(total) = ΔU(system) + ΔU(surroundings) = 0
→ ΔU(system) = - ΔU(surroundings) = -C<sub>v</sub> ΔT (constant volume → dV = 0)
 
where C<sub>v</sub> = heat capacity of the bomb
 
Before the bomb can be used to determine heat of combustion of any compound, it must be calibrated.
The value of C<sub>v</sub> can be estimated by
C<sub>v</sub> (calorimeter) = m (water). C<sub>v</sub> (water) + m (steel). C<sub>v</sub> (steel)
 
m (water) and m (steel) can be measured;
 
C<sub>v</sub>(water)= 1 cal/g.K
 
C<sub>v</sub>(steel)= 0.1 cal/g.K
 
In laboratory, C<sub>v</sub> is determined by running a compound with known heat of combustion value: C<sub>v</sub> = H<sub>c</sub>/ΔT
 
Common compounds are [[benzoic acid]] (H<sub>c</sub> = 6318 cal/g) or p-methyl benzoic acid (H<sub>c</sub> = 6957 cal/g).
 
Temperature (T) is recorded every minute and ΔT = T(final) - T(initial)
 
A small factor contributes to the correction of the total heat of combustion is the fuse wire. Nickel fuse wire is often used and has heat of combustion = 981.3 cal/g
 
In order to calibrate the bomb, a small amount (~ 1 g) of benzoic acid, or p-methyl benzoic acid is weighed.  
A length of Nickel fuse wire (~10&nbsp;cm) is weighed both before and after the combustion process. Mass of fuse wire burned Δm = m(before) - m(after)
 
The combustion of sample (benzoic acid) inside the bomb ΔH<sub>c</sub> = ΔH<sub>c</sub> (benzoic acid) x m (benzoic acid) + ΔH<sub>c</sub> (Ni fuse wire) x Δm (Ni fuse wire)
 
ΔH<sub>c</sub> = C<sub>v</sub>. ΔT → C<sub>v</sub> = ΔH<sub>c</sub>/ΔT
 
Once C<sub>v</sub> value of the bomb is determined, the bomb is ready to use to calculate heat of combustion of any compounds by ΔH<sub>c</sub> = C<sub>v</sub>. ΔT
 
<ref>Polik, W. (1997). Bomb Calorimetery.  Retrieved from http://www.chem.hope.edu/~polik/Chem345-2000/bombcalorimetry.htm</ref>
<ref>Bozzelli, J. (2010). Heat of Combustion via Calorimetry: Detailed Procedures. Chem 339-Physical Chemistry Lab for Chemical Engineers –Lab Manual.</ref>
 
==Calvet-type calorimeters==
The detection is based on a three-dimensional fluxmeter sensor. The fluxmeter element consists of a ring of several thermocouples in series. The corresponding thermopile of high thermal conductivity surrounds the experimental space within the calorimetric block. The radial arrangement of the thermopiles guarantees an almost complete integration of the heat. This is verified by the calculation of the efficiency ratio that indicates that an average value of 94% +/- 1% of heat is transmitted through the sensor on the full range of temperature of the Calvet-type calorimeter. In this setup, the sensitivity of the calorimeter is not affected by the crucible, the type of purgegas, or the flow rate. The main advantage of the setup is the increase of the experimental vessel's size and consequently the size of the sample, without affecting the accuracy of the calorimetric measurement.
 
The calibration of the calorimetric detectors is a key parameter and has to be performed very carefully. For Calvet-type calorimeters, a specific calibration, so called [[Joule heating|Joule effect]] or electrical calibration, has been developed to overcome all the problems encountered by a calibration done with standard materials.
The main advantages of this type of calibration are as follows:
*It is an absolute calibration.
*The use of standard materials for calibration is not necessary. The calibration can be performed at a constant temperature, in the heating mode and in the cooling mode.
*It can be applied to any experimental vessel volume.
*It is a very accurate calibration.
 
An example of Calvet-type calorimeter is the C80 Calorimeter (reaction, isothermal and scanning calorimeter).<ref name="Calvet-type calorimeter">[http://www.setaram.com/C80.htm C80 Calorimeter from Setaram Instrumentation]</ref>
 
==Constant-pressure calorimeter==
 
A '''constant-pressure calorimeter''' measures the change in [[enthalpy]] of a reaction occurring in [[solution]] during which the [[atmospheric pressure]] remains constant.
 
An example is a coffee-cup calorimeter, which is constructed from two nested [[Styrofoam]] cups and a lid with two holes, allowing insertion of a thermometer and a stirring rod. The inner cup holds a known amount of a solute, usually water, that absorbs the heat from the reaction. When the reaction occurs, the outer cup provides [[Thermal insulation|insulation]]. Then             
 
<math>Cp = \frac {W\Delta H}{M\Delta T}</math>
 
where
 
:<math>Cp</math> = Specific heat at constant pressure
:<math>\Delta H</math> = Enthalpy of solution
:<math>\Delta T</math> = Change in temperature
:<math>W</math> = mass of solute
:<math>M</math> = molecular mass of solute
 
The measurement of heat using a simple calorimeter, like the coffee cup calorimeter, is an example of constant-pressure calorimetry, since the pressure (atmospheric pressure) remains constant during the process. Constant-pressure calorimetry is used in determining the changes in enthalpy occurring in solution. Under these conditions the change in enthalpy equals the heat.
 
==Differential scanning calorimeter==
{{main|Differential scanning calorimetry}}
In a '''differential scanning calorimeter''' (DSC), [[heat flow]] into a sample—usually contained in a small [[aluminium]] capsule or 'pan'—is measured differentially, i.e., by comparing it to the flow into an empty reference pan.
 
In a '''[[heat flux]] DSC''', both pans sit on a small slab of material with a known (calibrated) heat resistance K. The temperature of the calorimeter is raised linearly with time (scanned), i.e., the heating rate
dT/dt = β
is kept constant. This time linearity requires good design and good (computerized) temperature control. Of course, controlled cooling and isothermal experiments are also possible.
 
Heat flows into the two pans by conduction. The flow of heat into the sample is larger because of its [[heat capacity]] ''C<sub>p</sub>''. The difference in flow ''dq''/''dt'' induces a small temperature difference Δ''T'' across the slab. This temperature difference is measured using a [[thermocouple]]. The heat capacity can in principle be determined from this signal:
 
<math>\Delta T = K {dq\over dt} = K C_p\, \beta</math>
 
Note that this formula (equivalent to [[Law of heat conduction|Newton's law of heat flow]]) is analogous to, and much older than, [[Ohm's law]] of electric flow:
ΔV = R dQ/dt = R I.
 
When suddenly heat is absorbed by the sample (e.g., when the sample melts), the signal will respond and exhibit a peak.
 
<math>{dq\over dt} = C_p \beta + f(t,T) </math>
 
From the [[integral]] of this peak the enthalpy of melting can be determined, and from its onset the melting temperature.
 
Differential scanning calorimetry is a workhorse technique in many fields, particularly in [[polymer]] characterization.
 
A '''modulated temperature differential scanning calorimeter''' (MTDSC) is a type of DSC in which a small oscillation is imposed upon the otherwise linear heating rate.
 
This has a number of advantages. It facilitates the direct measurement of the heat capacity in one measurement, even in (quasi-)isothermal conditions. It permits the simultaneous measurement of heat effects that are reversible and not reversible at the timescale of the oscillation (reversing and non-reversing heat flow, respectively). It increases the sensitivity of the heat capacity measurement, allowing for scans at a slow underlying heating rate.
 
'''Safety Screening''':- DSC may also be used as an initial safety screening tool.  In this mode the sample will be housed in a non-reactive crucible (often [[Gold]], or Gold plated steel), and which will be able to withstand [[pressure]] (typically up to 100 [[bar (unit)|bar]]). The presence of an [[exothermic]] event can then be used to assess the [[chemical stability|stability]] of a substance to heat. However, due to a combination of relatively poor sensitivity, slower than normal scan rates (typically 2-3°/min - due to much heavier crucible) and unknonwn [[activation energy]], it is necessary to deduct about 75-100°C from the initial start of the observed exotherm to '''suggest''' a maximum temperature for the material. A much more accurate data set can be obtained from an adiabatic calorimeter, but such a test may take 2–3 days from [[ambient temperature|ambient]] at a rate of 3°C increment per half hour.
 
==Isothermal titration calorimeter==<!-- This section is linked from [[Titration]] -->
{{main|Isothermal Titration Calorimetry}}
In an '''isothermal [[titration]] calorimeter''', the heat of reaction is used to follow a titration experiment. This permits determination of the midpoint ([[stoichiometry]]) (N) of a reaction as well as its enthalpy (delta H), entropy (delta S) and of primary concern the binding affinity (Ka)
 
The technique is gaining in importance particularly in the field of [[biochemistry]], because it facilitates determination of substrate binding to [[enzyme]]s. The technique is commonly used in the pharmaceutical industry to characterize potential drug candidates.
 
==See also==
{{commons category|Calorimeters}}
*[[Enthalpy]]
*[[Heat]]
*[[Calorie]]
*[[Heat of combustion]]
*[[Calorimeter constant]]
 
==References==
{{reflist}}
 
{{Laboratory equipment}}
 
[[Category:Measuring instruments]]
[[Category:Laboratory equipment]]
 
[[ja:熱#熱量計]]

Latest revision as of 00:11, 2 January 2015

Nike Air Force oder indem eine einzigartige

In A Friend in Deed, sie, Drops Sweetie und andere Ponys auf Dächer hüpfen während der Song-Lächeln. In der Marktszene der Umsetzung Ihrer Hoof unten, sie auf einem Tisch zusammengesunken ist. "Ich denke, das wird mir viel bessere Gesamt Trainer zu machen, weil es Ihnen eine ganz andere Perspektive", sagte Mangini. "Das ist auf jeden Fall ein Ziel von mir.

Wie zu verbringen tagelang in der Stadt zu rauben, können zu einer Rolle, dass der D20 für eine info sammeln Prüfung, ein paar BS Rollen der Perzentile für gute Effekthascherei kondensiert und dann soll er den Laden Nike Air Force ausrauben, anstatt ihn zu verbringen Alle Spiel nichts zu tun, ist, dass ganze Stück in 10 Minuten kondensiert. Wenn Sie wollen, dass es danach zu stoppen, entweder ihn gefangen, schwer traumatisiert oder getötet / ausgeführt.

Text-Lese-Software können Sie den Text auf dem Bildschirm, um als Sound-Datei ausgegeben werden. Louis Vuitton Tasche So können Menschen, die nicht lesen können, zu hören, was auf dem Text. Wer weiß, was passiert, wenn eine Webseite angezeigt wird. Sind Sie einfach Kollision mit einem Link, der auf eine Verbindung, zum Beispiel in diesem Fall MSN.

In der Zwischenzeit jedoch entdeckte ich eine Online-Drucker namens Zazzle, die meine Entwürfe zu nehmen und sie auf thier Produkte würden, so dass ich eine Website, um sie zu verkaufen auf zu bauen. Ich war intreged und schnell meine eigene Zazzle Galerie eingestellt.

Wir haben nur Platz, um ein paar der mehr als 80 Produkte Nike Schweiz mit diesem Entwurf auf ihnen zur Verfügung zu zeigen. Macht große Raum-oder Bürozubehör, Spaß Gefälligkeiten für Geburtstagsfeiern, Hochzeits-oder Baby-Dusche Ornamente, oder indem eine einzigartige, besondere Note zu verpackte.

Alligator Adventure verkündet über 800 Alligatoren. Die Gäste finden zahlreiche Alligatoren in einer Größe von nur acht Zentimeter bis zum reifen 15 Fuß Exemplare, die in von 500 1000 Pfund wiegen, und alle Größen dazwischen zu sehen. Lächeln begeistert sein. Sie würden, wie viele Menschen nicht gerechnet werden begeistert sein.

Über Jungs, die ich treffen wollen: Ich freue mich auf Jungs, die eine solide Herz, Geist und Körper und die Persönlichkeit zu entsprechen haben, zu erfüllen. Ich bin auch auf der Suche nach Jungs, die mir helfen können, Dinge herauszufinden, auf dem Weg, und mir helfen, meine Ziele zu erreichen, während den Aufbau einer Nike Shoes Freundschaft.

Dieser Artikel war ein weiterer anti Nintendo Troll Versuch einer Website, die offensichtlich in der Liebe mit Microsoft. Verstehen Sie mich nicht falsch, es war die Wahl in MS-System zuletzt gen und könnte dieses Mal sein, aber nur die Zeit zeigen.