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      <title>Period 1 Thermodynamics #3 by Thomas E Clark</title>
      <link>https://padlet.com/tec430/stpnrhtx9sdz</link>
      <description>Please use the handout and answer the following questions listed on the board
p358 2 key pts, p359 practice Ques, p360 2 key pts, p361 2 key pts, p362 practice ques, p363-364 2 key pts, p364 question, p365-366 2 key pts, p367 questions.</description>
      <language>en-us</language>
      <pubDate>2017-02-08 16:26:18 UTC</pubDate>
      <lastBuildDate>2017-02-10 16:33:54 UTC</lastBuildDate>
      <webMaster>hello@padlet.com</webMaster>
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      <item>
         <title>Nicky Castillo</title>
         <author></author>
         <link>https://padlet.com/tec430/stpnrhtx9sdz/wish/152525205</link>
         <description><![CDATA[<div>Pg. 358<br>1. The first law of Thermodynamics states that energy is neither created nor destroyed. <br>2. Internal energy can change by doing work or a change in heat.<br><br>Pg. 359<br>1. 3,000J -2,000J=<strong>1,000J<br></strong>2. 2,500 - 1,700J=<strong>800J<br><br></strong>Pg. 360-361<br>1. Work is dependent on volume and pressure for a gas.<br>2. You can find the change in volume through the area and displacement of the piston.<br>3. An isobaric process involves work done by a gas without a change in pressure. <br>4. Pressure can remain constant in a piston if the weight on top is constant.<br><br>Pg. 362<br>1. Delta P=300 m^3 - 50 m^3<br>Delta P=250m^3<br>W=(1,000.0Pa)(250m^3)<br>W=<strong>250,000 J<br></strong>2. 6,000.0J=(300Pa)(P2-100m^3)<br>20m^3=P2-100m^3<br>P=<strong>120 m^3</strong><br><br>Pg. 363-364<br>1. An isochoric process involves the pressure of a gas increasing, but not the volume.<br>2. This means there is no work, as volume does not change, and delta V=0<br><br>Pg. 364 <br>1. <strong>No work</strong>, as Delta V=0<br>2.<strong> No work</strong>, since Delta V=0<br><br>Pg. 365-366<br>1. In an isothermal process, the temperature is always constant<br>2. The product of pressure and volume remains constant.<br><br>Pg. 367<br>1. W=(1.0mol)(8.31J/K)(303.15K)ln(3.0/2.0)<br>W=<strong>1020J</strong><br>2. W=(0.60mol)(298.15K)(8.13J/K)ln(3.0)<br>W=<strong>1,630J</strong></div>]]></description>
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         <pubDate>2017-02-08 16:41:52 UTC</pubDate>
         <guid>https://padlet.com/tec430/stpnrhtx9sdz/wish/152525205</guid>
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      <item>
         <title>Cori, Kayla, and Noah</title>
         <author></author>
         <link>https://padlet.com/tec430/stpnrhtx9sdz/wish/152528908</link>
         <description><![CDATA[<div>P358<br>-The initial internal energy in a system, Ui, changes to a final internal energy, Uf, when heat, Q, is absorbed or released by the system and the system does work, -W, on its surroundings (or surroundings do work on the system) Uf-Ui=Change U= Q-W<br>- The quantity Q (Heat transfer) is positive when the system absorbs heat and negative when the system releases heat. The quantity W (work) is positive when the system does work on its surroundings and negative when the surroundings do work on the system.<br><br>P359<br>1) ΔU = 3000J-2000J= 1000J<br>2)ΔU = 2500J - 1700J = 800J<br>P360<br>Work = Force*time = Fs<br>Work = Pressure*Area*time = PAs<br>Work = PΔV =Pressure*Change in Velocity<br><br>P361<br><em>isobaric </em>= constant pressure<br>W= PΔV<br>Work increases with an increase in volume when pressure is constant<br><br>P362<br>1.) W = (1000.0 Pa)(300.0m^3-50m^3) = 250,000J<br>2.) W = (6000.0J/300.0Pa) = 100.0m^3 = 120m^3<br><br>P363-364<br>- Volume is constant in an isochoric process, no work is done.<br>-The volume is constant, so Fs (force times distance) equals 0. No work is being done- the area under the graph is 0.<br><br>P364<br>1.<br>W=PΔV<br>P= 3000<br>ΔV= 0<br>W=3000*0=0<br>2.<br>ΔV=0<br>P=6000<br>W=6000*0=0<br><br>P365-6<br>- In an isothermal system, the temperature remains constant as other quantities change.<br>- P=(nRT)/V<br>- W=nRTln(Vf/vi)<br>- ΔU= Q-W<br>0=Q-W<br>Q=W<br><br>P367<br>1.) (1.0mol)(8.31 J/k)(273.15K+30.0K)(ln(3.0m^3)/(2.0m^3))<br>= 1,020J<br>2.) (.60mol)(8.31J/k)(273.15K+25.0K)(ln(3.0m^3)/(1.0m^3)) =1,630J</div>]]></description>
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         <pubDate>2017-02-08 16:50:19 UTC</pubDate>
         <guid>https://padlet.com/tec430/stpnrhtx9sdz/wish/152528908</guid>
      </item>
      <item>
         <title>Uriah Aldaco</title>
         <author></author>
         <link>https://padlet.com/tec430/stpnrhtx9sdz/wish/152531126</link>
         <description><![CDATA[<div>Pg. 358<br>1) Heat, work, and the internal energy make up all of our energy<br>2) A system can lose energy by doing work on their surroundings.<br><br>Pg. 359 - Practice Questions<br>1)&nbsp; 3000J - 2000J = <strong>1000J<br></strong>2) 2500J - 1700J = <strong>800J<br></strong><br>Pg 360<br>1) W = P*(triangle)V<br>2) Graphing pressure versus volume graph compares them and the area under gives you work.<br><br>pg 361<br>1) With constant pressure, temperature change can change volume. <strong>Isobaric</strong><br>2) In a graph, this relationship forms a rectangle.<br><br>Pg 362<br>1) W = (1000 Pa)(300 m^3 - 50 m^3) = 250000 J = <strong>250 kJ<br></strong>2) 6000 J = (300 Pa)(Vfin - 100)<br>20 = Vfin - 100; Vfin = <strong>120 m^3</strong><br><br>Pg 363<br>1) With constant volume, temperature can change pressure.&nbsp;<strong>Isochoric</strong><br>2) Since volume stays the same, work done on the system equals zero.<br><br>Pg 364<br>1) W = 0 b/c (chg)V = 0; <strong>isochoric</strong> process<br>2) W = 0 b/c (chg)V = 0;&nbsp;<strong>isochoric</strong> process<br><br>Pg 365-366<br>1) With constant temperature, pressure and volume change. <strong>Isothermal</strong> <br>2) P = nRT/V; In a P vs V graph, curved top. W = nRT[ln(Vf/Vi)]<br><br>Pg 367<br>1) W = (1mol)(8.31J/K)(273.15K + 30K)ln(3/2) = <strong>1020 J</strong><br>2) Q = W = (0.6mol)(8.31J/K)(273.15K + 25K)ln(3/1) = <strong>1630 J</strong></div>]]></description>
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         <pubDate>2017-02-08 16:55:19 UTC</pubDate>
         <guid>https://padlet.com/tec430/stpnrhtx9sdz/wish/152531126</guid>
      </item>
      <item>
         <title>James Holan</title>
         <author></author>
         <link>https://padlet.com/tec430/stpnrhtx9sdz/wish/152532049</link>
         <description><![CDATA[<div>pg.358<br>1. Uf-Ui=deltaU=Q-W<br>2. Heat, work, and internal energy make up the energy in a system.<br><br></div>]]></description>
         <enclosure url="" />
         <pubDate>2017-02-08 16:57:53 UTC</pubDate>
         <guid>https://padlet.com/tec430/stpnrhtx9sdz/wish/152532049</guid>
      </item>
      <item>
         <title>Cynthia Jackson</title>
         <author></author>
         <link>https://padlet.com/tec430/stpnrhtx9sdz/wish/152536561</link>
         <description><![CDATA[<div>Pg.358<br>1)For mechanincal energy to be conserved, the system can not have energy lost to heat.&nbsp;<br>2)Heat, work and internal energy make up all of our energy.&nbsp;<br>&nbsp;Pg.359<br>1)3,000J-2,000 J= 1,000J&nbsp;<br>2)2500J-1700J= 800J&nbsp;<br><br>Pg.360<br>1)A gas only performs work if the gas expands<br>2)F= Pressure*area&nbsp;<br><br>Pg.361<br>1)Isobaric: process where the pressure stays constant<br>2) W=P delta V<br><br>Pg.362&nbsp;<br>1)(1,000)(300m^3-50m^3)=250000J<br>2)<br><br>Pg.363-364<br>1)isochoric: everything else changes as volume stays constant<br>2) If there is no work then V=0 since nothing is changing<br><br>Pg.364<br>1)No work done: V=0<br>2)No change in volume<br><br>Pg.365-366<br>1)In a isothermal system, temperature remains the same as everything else changes<br>2)P=nRT/V<br><br>Pg.367<br>1)<br>2)<br><br></div>]]></description>
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         <pubDate>2017-02-08 17:09:42 UTC</pubDate>
         <guid>https://padlet.com/tec430/stpnrhtx9sdz/wish/152536561</guid>
      </item>
      <item>
         <title>Brie Scott</title>
         <author></author>
         <link>https://padlet.com/tec430/stpnrhtx9sdz/wish/152542421</link>
         <description><![CDATA[<div>pg.358<br>1)The first law of thermodynamics deals with energy conservation.<br>2) These three quantities-heat, work, and internal energy.<br>pg.359<br>1) 3,000 J of heat<br>2,000 J of work<br>3,000-2,000= 1000 J<br>2) 2,500 J of heat<br>1,700 J of work<br>2500-1700= 800 J<br>pg.360<br>1) Force= Pressure*area* distance<br>W= P*(triangle)V<br><br></div>]]></description>
         <enclosure url="" />
         <pubDate>2017-02-08 17:25:38 UTC</pubDate>
         <guid>https://padlet.com/tec430/stpnrhtx9sdz/wish/152542421</guid>
      </item>
      <item>
         <title>Joy Montes de Oca</title>
         <author></author>
         <link>https://padlet.com/tec430/stpnrhtx9sdz/wish/152545615</link>
         <description><![CDATA[<div>358<br>1. <strong>First Law of Thermodynamics</strong> deals with conservation of energy. -internal energy persists in situations of motion of atoms and molecules. <br>2. <strong>Work</strong> is the transfer of mechanical energy-for work in a gas, it must be compressed. Mechanical energy-work with systems where no energy lost in heat.&nbsp;<br>359<br>1. Change of U- 3000J-2000J=1000J<br>2. 2500J-1700J=800J&nbsp;<br>360<br>1. </div>]]></description>
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         <pubDate>2017-02-08 17:34:03 UTC</pubDate>
         <guid>https://padlet.com/tec430/stpnrhtx9sdz/wish/152545615</guid>
      </item>
      <item>
         <title>Daisy Adin</title>
         <author></author>
         <link>https://padlet.com/tec430/stpnrhtx9sdz/wish/152653328</link>
         <description><![CDATA[<div>Page 358<br>1. The first law of Thermodynamics states that energy can neither be created nor destroyed. <br>2. Internal energy can change by doing work or a change in heat.<br>Page 359<br>1. 3,000J -2,000J=1,000J<strong><br></strong>2. 2,500 - 1,700J=800J<strong><br></strong>Page 360 and 361<br>1. Work depends&nbsp; on volume and pressure for a gas.<br>2 .F= (pressure)(area)<br>3. An isobaric process involves work done by a gas without a change in pressure. <br>4. Pressure can remain constant in a piston if the weight on top is constant.<br>Page 362<br>1. Delta P=300 m^3 - 50 m^3<br>Delta P=250m^3<br>W=(1,000.0Pa)(250m^3)<br>W=250,000 J<strong><br></strong>2. 6,000.0J=(300Pa)(P2-100m^3)<br>20m^3=P2-100m^3<br>P=120 m^3<br>Page 363 and 364<br>1. An isochoric process: the pressure of a gas increasing but not the volume.<br>2. No work means V=0&nbsp;<br>Page 364&nbsp;<br>1. No work, as Delta V=0<br>2. No work, since Delta V=0<br>Page 365 and 366<br>1. In an isothermal process, the temperature is always constant<br>2. The product of pressure and volume remains constant.<br>Page 367<br>1. W=(1.0mol)(8.31J/K)(303.15K)ln(3.0/2.0)<br>W=1020J<br>2. W=(0.60mol)(298.15K)(8.13J/K)ln(3.0)<br>W=1,630J</div>]]></description>
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         <pubDate>2017-02-09 00:45:27 UTC</pubDate>
         <guid>https://padlet.com/tec430/stpnrhtx9sdz/wish/152653328</guid>
      </item>
      <item>
         <title>Bryson Leshkiw</title>
         <author></author>
         <link>https://padlet.com/tec430/stpnrhtx9sdz/wish/152656564</link>
         <description><![CDATA[<div>p358<br>1. Heat is the transfer of thermal energy. This energy is conserved.&nbsp;<br>2. Work is the transfer of mechanical energy. The first law of thermodynamics states that these energies, together, are conserved.&nbsp;<br>p359 internal energy<br>1. f-i 3000j-2000j= 1000J<br>2. 2500J-1700J= 800J<br>p360<br>1.&nbsp; Force is equal to pressure<br>2. Work is dependent on volume and pressure for a gas.<br>p361<br>1. In an isobaric process pressure is constant.&nbsp;<br>2. For an isobaric process the volume of gas changes, but the weighted piston keeps pressure constant.&nbsp; &nbsp;<br>p362<br>1. (1000pa)(300m3-50m3)=250000J<br>2. w/p+vi 6000J/300pa+100m3=120m^3<br>p363-364<br>1. As gas increases pressure also increases while volume is constant.<br>2.&nbsp; No work is done as volume stays the same&nbsp;<br>p364<br>1. no work V=0<br>2. no work v=0<br>p365-366<br>1. In an isothermal system temperature remains constant while everything else changes.<br>2. In an isothermal process internal energy doesn't change and heat remains the same as work.<br>p367&nbsp;<br>1. W=nRTIn(Vf/Vi)= (1.0)(8.31J/K)(273.15k+30 k) ln(3/2)=1020J<br>2. (.60)(8.31J/K)(273.15K+25K)(3/1)<br>1630J</div>]]></description>
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         <pubDate>2017-02-09 01:23:00 UTC</pubDate>
         <guid>https://padlet.com/tec430/stpnrhtx9sdz/wish/152656564</guid>
      </item>
      <item>
         <title>Biren Rama</title>
         <author></author>
         <link>https://padlet.com/tec430/stpnrhtx9sdz/wish/152657680</link>
         <description><![CDATA[<div>358<br>1.) Energy can neither be created nor destroyed.<br>2.) If you have two of heat, work, or internal energy, you can solve for the third and they all interact proportionally. Their sum is also finite.<br>359<br>1.)deltaU = <strong>1000 J</strong><br>2.)deltaU =<strong> 800J</strong><br>360<br>1.) W = PdeltaV<br>2.)When you hold temperature constant, and change the pressure, the resultant change in volume of a gas is all that really matters in terms of it's work done.<br>361<br>1.)When you hold pressure constant, and change the temperature, the resultant change in volume of a gas is all that really matters in terms of it's work done.<br>2.) The amount of heat added to change the temperature is equivalent to the amount of work done by the gas. (ideally)<br>362 (Isobaric reactions)<br>1.)1000Pa*250m^3 = <strong>250,000 J</strong><br>2.)6000 J= (Vf-100)m^3 *300Pa<br>&nbsp; &nbsp; &nbsp; &nbsp;20 = Vf-100<br>&nbsp; &nbsp; &nbsp; &nbsp;Vf = <strong>120 m^3</strong><br>363-364 (Isochoric reactions)<br>1.) If volume is constant, as you change the temperature, the pressure changes, but no work is done. <br>2.) What changes is the internal energy.<br>364<br>1.) <strong>0J</strong> Simpson<br>2.) <strong>0J</strong> was innocent<br>365-366 (Isothermal reaction)<br>1.) In an isothermal reaction, the work done is equivalent to the amount of heat added to a system.<br>2.) W= nRTln(Vf/Vi)<br>367<br>1.) 1mol*(30+273)K*8.314 J/molK * ln(3/2) = <strong>1,021 J</strong><br>2.) .6mol * (25+273)K *8.314 J/molK * ln(3) = <strong>1,633 J</strong></div>]]></description>
         <enclosure url="" />
         <pubDate>2017-02-09 01:33:23 UTC</pubDate>
         <guid>https://padlet.com/tec430/stpnrhtx9sdz/wish/152657680</guid>
      </item>
      <item>
         <title>Joy Montes de Oca </title>
         <author></author>
         <link>https://padlet.com/tec430/stpnrhtx9sdz/wish/152950590</link>
         <description><![CDATA[<div>358<br>1. <strong>First Law of Thermodynamics</strong> deals with conservation of energy. -internal energy persists in situations of motion of atoms and molecules. <br>2. <strong>Work</strong> is the transfer of mechanical energy-for work in a gas, it must be compressed. Mechanical energy-work with systems where no energy lost in heat. <br><br>359<br>1. Change of U- 3000J-2000J=1000J<br>2. 2500J-1700J=800J <br>360 and 361<br>1. The packet relates how Force=Pressure<br><strong>W=P*(Change of V)</strong><br>Work depends on the changes or consistency of volume as well as the pressure for a gas.<br>2. <strong>F=Pressure*Area</strong><br>The graph builds the connection between the two, but the area underneath explains the amount of work in that current scenario.<br> 3. An <strong>isobaric process </strong>is a thermodynamic process in which pressure stays constant meaning the change of P is equivalent to zero. The volume of the gas can change but the weighted piston maintains the continuity of the pressure.&nbsp;<br>4. Heat added to change the temp is represented by an equivalent value of work which was done by the gas.&nbsp;<br><br>362<br>1. W=(1000)*[(300M^s)-(50m^s)]=250000J or 250kj<br>2. 6kj-6000J=(300Pa)(Vf-100)=20<br>Vf-100=120m^3<br><br>363 and 364<br>1.&nbsp; An isothermal process is measured as a changing system, but temperature remains constant. In other words, internal energy doesn't change while heat stays constant.<br>2. Volume a constant number, so work is zero.&nbsp;<br><br>364<br>1. V=0 therefore no work is done in this scenario. 3000*0=0<br>2. There is no change in volume.&nbsp;<br><br>365 and 366<br>1.W=nRT*ln(Vf/Vi) isothermal temp-constant_(P and V are constant)<br>2.P=nRT/V<br><br>367<br>1.W=(1mol)*(8.31J/K)*(273K+30K)*[ln(3/2)]=1020J<br>2. W=(.6mol)*(8.31J/K)*(273K+25K)*[ln93/1)]=1630J</div>]]></description>
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         <pubDate>2017-02-10 00:33:45 UTC</pubDate>
         <guid>https://padlet.com/tec430/stpnrhtx9sdz/wish/152950590</guid>
      </item>
      <item>
         <title>Max Mok</title>
         <author></author>
         <link>https://padlet.com/tec430/stpnrhtx9sdz/wish/152972499</link>
         <description><![CDATA[<div>358<br>1) Energy can't be created or destroyed.<br>2) Work is the transfer of mechanical energy. Internal energy can change by doing work or a change in heat.<br><br>359<br>1) 3000J-2000J=1000J<br>2) 2500J-1700J=800J<br><br>360<br>1) W = PdeltaV<br><br>361<br>2) With constant pressure, temperature change can change volume.<br>2) isobaric = constant pressure<br><br>362<br>1) W = (1000 Pa)(300 m^3 - 50 m^3) = 250000 J<br>2) 6000 J = (300 Pa)(Vfin - 100)<br>20 = Vfin - 100; Vfin=120m^3<br><br>363-364<br>1) An isochoric process involves the pressure of a gas increasing, but not the volume.<br>2) Volume is constant in an isochoric process, no work is done.<br><br>364<br>1) No work, deltav=0<br>2) No work, deltav=0<br><br>365-366<br>1) Temperature is always constant in an isothermal process.<br>2) P=(nRT)/V<br><br>367<br>1) W=(1.0mol)(8.31J/K)(303.15K)ln(3/2)<br>W=1020J<br>2) W = (0.6mol)(8.31J/K)(273.15K + 25K)ln(3/1) =16</div>]]></description>
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         <pubDate>2017-02-10 05:03:05 UTC</pubDate>
         <guid>https://padlet.com/tec430/stpnrhtx9sdz/wish/152972499</guid>
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      <item>
         <title>Brie Scott p.2</title>
         <author></author>
         <link>https://padlet.com/tec430/stpnrhtx9sdz/wish/153097430</link>
         <description><![CDATA[<div>2) Graphing pressure versus volume graph compares them and the area under gives you work.<br>pg.361<br>1) An <strong>isobaric process </strong>is a thermodynamic process in which pressure stays constant meaning the change of P is equivalent to zero. The volume of the gas can change but the weighted piston maintains the continuity of the pressure.&nbsp;<br>2) Constant pressure, temperature change can change volume.<br>pg.362<br>1) W=(1000)*[(300M^s)-(50m^s)]=250000J or 250kj<br>2. 6kj-6000J=(300Pa)(Vf-100)=20<br>Vf-100=120m^3<br>pg.363-364<br>1) When volume is constant while there is a change in temperature then the pressure changes but there isn't any work performed.<br>2)&nbsp; An isochoric process involves the pressure of a gas increasing, but not the volume.&nbsp;<br>pg.364<br>1)W= 3000*0=0<br>2) W= 6000*0=0<br>pg.365-366<br>&nbsp;1) In an isothermal system, the temperature remains constant as other quantities change.<br>2)P=nRT/V<br>pg.367<br>1.W=(1mol)*(8.31J/K)*(273K+30K)*[ln(3/2)]=1020J<br>2. W=(.6mol)*(8.31J/K)*(273K+25K)*[ln93/1)]=1630J<br><br></div>]]></description>
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         <pubDate>2017-02-10 16:09:58 UTC</pubDate>
         <guid>https://padlet.com/tec430/stpnrhtx9sdz/wish/153097430</guid>
      </item>
      <item>
         <title>Gareth Usac</title>
         <author></author>
         <link>https://padlet.com/tec430/stpnrhtx9sdz/wish/153098758</link>
         <description><![CDATA[<div>Pg.358 2 Key Points<br>1. Energy can neither be created nor destroyed.<br>2.Heat is a transfer of thermal energy. Work is the transfer of mechanical energy.<br>Pg.359<br>1. 3000J - 2000J= 1000J<br>2. 2500J - 1700J= 800J<br>Pg.360 2 Key Points<br>1. Work = force * distance<br>or W=F * s<br>2. Work = change in volume * pressure<br>Pg.361 2 Key Points<br>1. Isobaric process is a thermodynamic process where pressure stays constant.<br>2. The pressure of the piston stays constant, but the volume of a gas can change.&nbsp;<br>Pg. 362<br>1. W=Pressure * change in volume<br>(1000 Pa)(300m^3 -50m^3)= 250000J<br>2. 6000J = (300 Pa) (final volume - 100) = 120m^3<br>Pg.363 2 Key Points<br>1. Isochoric process is a process where pressure is not constant but volume is constant.<br>2. An example of an isochoric process is if a spray can was tossed into a fire.<br>Pg.364&nbsp;<br>1. Since change in volume is 0, there is no work.<br>2. Since change in volume is 0, there is no work.<br>Pg.365-366 2 Key Points<br>1. In an isothermal system, temperature remains constant.&nbsp;<br>2. The relation between pressure and volume is&nbsp;<br>P= nRT/V<br>Pg.367<br>1. W= (1)(8.31J/K)(303.15K)ln(3/2)<br>= 1020 J<br>2. W= (.6)(8.31 J/K)(273+15)(ln 3) =1633 J</div>]]></description>
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         <pubDate>2017-02-10 16:13:57 UTC</pubDate>
         <guid>https://padlet.com/tec430/stpnrhtx9sdz/wish/153098758</guid>
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