Return-Path: Received: from [24.25.9.100] (HELO ms-smtp-01-eri0.southeast.rr.com) by logan.com (CommuniGate Pro SMTP 4.3c3) with ESMTP id 854150 for flyrotary@lancaironline.net; Mon, 04 Apr 2005 10:19:35 -0400 Received-SPF: pass receiver=logan.com; client-ip=24.25.9.100; envelope-from=eanderson@carolina.rr.com Received: from edward2 (cpe-024-074-185-127.carolina.res.rr.com [24.74.185.127]) by ms-smtp-01-eri0.southeast.rr.com (8.12.10/8.12.7) with SMTP id j34EIjLw008438 for ; Mon, 4 Apr 2005 10:18:46 -0400 (EDT) Message-ID: <003901c53921$36bac140$2402a8c0@edward2> From: "Ed Anderson" To: "Rotary motors in aircraft" References: Subject: molecular movemen translational velocity Date: Mon, 4 Apr 2005 10:18:46 -0400 MIME-Version: 1.0 Content-Type: multipart/related; type="multipart/alternative"; boundary="----=_NextPart_000_0035_01C538FF.AF7259D0" X-Priority: 3 X-MSMail-Priority: Normal X-Mailer: Microsoft Outlook Express 6.00.2800.1106 X-MIMEOLE: Produced By Microsoft MimeOLE V6.00.2800.1106 X-Virus-Scanned: Symantec AntiVirus Scan Engine This is a multi-part message in MIME format. ------=_NextPart_000_0035_01C538FF.AF7259D0 Content-Type: multipart/alternative; boundary="----=_NextPart_001_0036_01C538FF.AF7259D0" ------=_NextPart_001_0036_01C538FF.AF7259D0 Content-Type: text/plain; charset="iso-8859-1" Content-Transfer-Encoding: quoted-printable I agree with your explanation, Bernie - but not totally with your first = assertion. I agree that the pressure is due to the average number of molecules = striking a surface per unit time. A clearer explanation than I had = given. However, when an airmass is moving there is a small = translational velocity component (small compared to the molecule's = nominal velocity), imparted to the molecule (else it would not move in = that direction). This translational velocity component increases where = the duct narrows which as you stated, reduces the time available for = molecules to impact the wall resulting in fewer impacts per unit time = =3D> less pressure. The opposite when the duct widens. So the molecules total velocity magnitude IS affected (even if minutely) = by the translational velocity of the air. This, of course, also = explains what happens in the Bernoulli tube where the air density is = considered "incompressible" or non changing. Below is an explanation I found which explains (I believe) , that = although often ignored for simplicity, air movement does impart a = translational component to the molecules velocity. Mean Free Path=20 The mean free path or average distance between collisions for a gas = molecule may be estimated from kinetic theory. Serway's approach is a = good visualization - if the molecules have diameter d, then the = effective cross-section for collision can be modeled by=20 using a circle of diameter 2d to represent a molecule's effective = collision area while treating the "target" molecules as point masses. In = time t, the circle would sweep out the volume shown and the number of = collisions can be estimated from the number of gas molecules that were = in that volume. The mean free path could then be taken as the length of the path divided = by the number of collisions.=20 The problem with this expression is that the average molecular velocity = is used, but the target molecules are also moving. The frequency of = collisions depends upon the average relative velocity of the randomly = moving molecules.=20 I highlighted the words for emphasis but they are as presented on the = webpage which you can check at. http://hyperphysics.phy-astr.gsu.edu/hbase/kinetic/menfre.html#c1 This shows (in my opinion) that pressure is indeed affected by the = average relative velocity component of the molecules velocity as well as = its velocity attributed to temperature. While the translational = component is quite small compared to the molecules velocity, it does = have an effect on pressure. No translational velocity component =3D> no = change in pressure. Since as you point out there is negligible = temperature change and therefore negligible change in the molecules = "inherent" velocity, the changes in pressure must be due to the = difference in the translational velocity component affects on the = molecule.=20 Whew, I think I want to get back to work on my digital flow meter. Boy, isn't this fun. I wonder how we can use it to abate Bernie's noise = problem. It appears simply, Bernie, if you can get your translational = speed up past the average molecular velocity the noise should no longer = be a problem {:>) Best Regards Ed ----- Original Message -----=20 From: To: "Rotary motors in aircraft" Sent: Monday, April 04, 2005 8:26 AM Subject: [FlyRotary] Re: molecular movement Re: Cooling -Learned a lot >=20 > OK, I can't keep my blabber mouth shut on this subject any longer. >=20 > molecular velocity is only a function of the temperature which is not = changing in the diffuser. colder air has less molecular velocity. >=20 > The stagnation, pitot, total, dynamic pressure (Pt) does not change if = we have a friction free wall. Why does the static pressure (P) along = the wall go up as we slow the air down? If Pt is not changing and = velocity is decreasing then the Bernoulli equation lets us calculate the = P value. We can ignore the small density change in our low velocity = arena. One way to think of this is that the P is proportional to the = number of molecules striking the surface per unit time. If they are = going by the surface at a slower average forward velocity, they strike = the surface more frequently and we see a higher pressure. >=20 > Bernie >=20 >=20 >=20 > >> Homepage: http://www.flyrotary.com/ > >> Archive: http://lancaironline.net/lists/flyrotary/List.html ------=_NextPart_001_0036_01C538FF.AF7259D0 Content-Type: text/html; charset="iso-8859-1" Content-Transfer-Encoding: quoted-printable
I agree with your explanation, Bernie = - but=20 not totally with your first assertion.
 
I agree that the pressure is due to the = average=20 number of molecules striking a surface per unit time. A clearer = explanation=20 than I had given.   However, when an airmass is moving = there is a=20 small translational velocity component (small compared to the molecule's = nominal=20 velocity),  imparted to the molecule (else it would not move in = that=20 direction).  This translational velocity component increases where = the duct=20 narrows which as you stated,  reduces the time available for = molecules to=20 impact the wall resulting in fewer impacts per unit time =3D> less=20 pressure.  The opposite when the duct widens.
 
So the molecules total velocity = magnitude IS=20 affected (even if minutely) by the translational velocity of the = air. =20 This, of course, also explains what happens in the Bernoulli tube where = the air=20 density is considered "incompressible" or non changing.
 
Below is an explanation I found which = explains (I=20 believe) , that although often ignored for simplicity, air movement does = impart=20 a translational component to the molecules velocity.

Mean Free Path =

The mean free path or average distance = between=20 collisions for a gas molecule may be estimated from kinetic theory. Serway's = approach is a good=20 visualization - if the molecules have diameter d, then the effective=20 cross-section for collision can be modeled by

using a circle of diameter 2d to = represent a=20 molecule's effective collision area while treating the "target" = molecules as=20 point masses. In time t, the circle would sweep out the volume shown and = the=20 number of collisions can be estimated from the number of gas molecules = that were=20 in that volume.

The mean free path could then be taken as = the length=20 of the path divided by the number of collisions.

The problem with this expression is = that the=20 average molecular velocity is used, but the = target=20 molecules are also moving. The frequency of = collisions=20 depends upon the average = relative velocity of the randomly moving molecules. =

I highlighted the words for emphasis = but they are=20 as presented on the webpage which you can check at.
http://hyperphysics.phy-astr.gsu.edu/hbase/kinetic/menfre.html#c1
 
This shows (in my opinion)  that = pressure is=20 indeed affected by the average relative velocity component of the = molecules=20 velocity as well as its velocity attributed to temperature. While the=20 translational component is quite small compared to the molecules = velocity, it=20 does have an effect on pressure.  No translational velocity = component =3D>=20 no change in pressure.  Since as you point out there is negligible=20 temperature change and therefore negligible change in the molecules = "inherent"=20 velocity, the changes in pressure must be due to the difference in the=20 translational velocity component affects on the = molecule. 
 
 Whew, I think I want to get back = to work on=20 my digital flow meter.
 
Boy, isn't this fun.  I wonder how = we can use=20 it to abate Bernie's noise problem.  It appears simply, Bernie, if = you can=20 get your translational speed up past the average molecular velocity the = noise=20 should no longer be a problem {:>)
 
Best Regards
 
Ed
 
 
 
----- Original Message ----- =
From: <jbker@juno.com>
To: "Rotary motors in aircraft" = <flyrotary@lancaironline.net>
Sent: Monday, April 04, 2005 8:26 = AM
Subject: [FlyRotary] Re: molecular = movement Re:=20 Cooling -Learned a lot

>
> OK, I can't keep my blabber mouth shut on this = subject any=20 longer.
>
> molecular velocity is only a function of the=20 temperature which is not changing in the diffuser. colder air has less = molecular=20 velocity.
>
> The stagnation, pitot, total, dynamic = pressure (Pt)=20 does not change if we have a friction free wall.  Why does the = static=20 pressure (P) along the wall go up as we slow the air down? If Pt is not = changing=20 and velocity is decreasing then the Bernoulli equation lets us calculate = the P=20 value. We can ignore the small density change in our low velocity arena. = One way=20 to think of this is that the P is proportional to the number of = molecules=20 striking the surface per unit time. If they are going by the surface at = a slower=20 average forward velocity, they strike the surface more frequently and we = see a=20 higher pressure.
>
> Bernie
>
>
> =
>=20 >>  Homepage: 
http://www.flyrotary.com/

> >>  Archive:   http://lancaironline.net/lists/flyrotary/List.html ------=_NextPart_001_0036_01C538FF.AF7259D0-- ------=_NextPart_000_0035_01C538FF.AF7259D0 Content-Type: image/gif; name="mfree1.gif" Content-Transfer-Encoding: base64 Content-Location: http://hyperphysics.phy-astr.gsu.edu/hbase/kinetic/imgkin/mfree1.gif R0lGODlhmwFXAPcAAP7rxp+TfH92Y97Ore7cuk9JPkA7Mr+wlf6wof92ff6Tj/9nc/8dRf87WP8P PP8AM/9JYSAdGV9YSgAAAK+iiM6/oW9nV93KrMq0m66ahbCah7OciLmljtjDp/biv/8sT/7OtP9Y av6Ehv6/qv8aRv9NbP9zif+Zpv+/wv/MzP+Elv8mUP7cvY+EbzAsJZJ9b2JMSGJJR21SUHZZV31f XIRjYYZlY4BhXpN3b8Srlv6imP+zuRAPDNzJqnViWFU/PmNKSHlbWYJiX41raZRwbpl0cp13daN7 eKF6d5FubL2nkf+mr6OQfU05OFlCQGRLSXBUUnxeW4dmZJJubJ94dqZ+e6yDgLCGg7KHhKF6eJp6 c+fTs4x5akw4N3tdWodmY5p1c6qBfraLh7uOi76Qjb+Sjr2QjLiMiZZxb/8zWUs3NmFIRmxRT3da V4NjYI9saqB5d6mAfb6RjsSVkceYlMqalsmZlcWWkv9mgJeDc0g0M1E7OltEQmZMSnFVU35hXYlo Za2Egc2dmdCfm9GgnM6emsycmKN9ev8NPUc0M1Q+PV5HRWtQTo5raZhzcbOJhcGTj9SintekoNil odWjn9OhnbWKhqODel5LRU45OHlcWZBta7SJhryPjNmmotqno6uCf0g1NFpDQZx2dKZ9esaXk0k2 NVI8O4lnZd2ppd+qplM+PKR8ecGTkKaIfcOUkIVkYqh/fNzGqv9AY4xpZ6V9etOinpl0cea3t9aq qcWcm7yUlPnHx086OVdBP2pPTXRXVbaLiK6EgcienoxtbGRLSoFiX5Jxb7mRj/LCwV1GRIRkYYtp Z6+JiEw3NnVYVvXExHVaWad/fN2wr3RYVevYt7mNilA6OayCf2VMSunVtUo2NVM9PFxFQ2lOTPPg vV5HRpdycNGmpmRNSZx2c6+FguHNr2lWT3NWVKSAf/9ZdoRtY9TApHRfVpV2cJV0cmtXUKuOgVhB P6J+fVRBPWpRUJl2ccmalpl4dnJVU+/auWBJSGNLSoFkY5h3dldDQCH5BAEAAAAALAAAAACbAVcA Bwj9AAEIHEiwoMGDCBMqXMiwocOHECNKnEixosWLGDNq3Mixo8ePIEOKHEmypMmTKFOqXMmypcuX MGPKnEmzps2bOHPq3Mmzp8+fQIMKHUq0qNGjSJMqXcq0qdOnUKNKnUq1qtWrWLNq3cq1q9evYMOK HUu2rFmFAQSoXTtAgEUCBQIACGAA4gC5Jw+s3ct3L16MCBIoEBh4MIDChAUnNoz4sGLHjB83niy5 cuTLizND1kwZ8+bPnTlXTmBwAYMGCxo4eNAgAYIFCxDUDAyhwYPbuG83gOCaZFoBESSoHTDBooAC AwBMoNDwQN0KFlDq5Wug79q/CS9gyKBhA4cOHv0MhgZtWbTn8ejLkz+vPj379+ZFk1bwAQKIBQ4Y hHCNIHAIBreJIJACI7ikAAQOkFCCCSegkMKDEKJwggolrPAABAqwMJIBBww0AQEtBEDAQBQI0KFB JXZIgAQSDFDBBCemOFBbzAHQggsVEFABAAeMCICLAFQgAHYg1SXRBS/AEIMMM9BQgw023IBDDuGd 1VKBhymQwAMhYHnQCCFwyUIIDuig0n0OrGDCDhC26WabO5iwggMhgBAShx4WcJwEAklQnQvREeSn AIBWEEEEAVgwQV2DAhpkBBYUUJcLPFjgHAAFtNBniBEc54JIBEyQ3EM9+PADEDIEIcQQRBRh/cQR RyBRRBJKVGnlSSAwwIBAI5xmJ0MgICibQCAYNhIIYZawxJvMNpvCDiVw+WtHeAoEo7VBGknApwNV oO2namHrrUDbYnoicpdeGsCnBPBAQAQ+FrAjSBRMQKRCTDThxBNQRCHFFEVQUYUVV2BhsBVZaLHF rSgZNoIDAkKkwAOMnTZSAg6UwKazHL8J7QOkUXuich4CAJwBKPMwr8kRoGyAyuGSfHLKLxaUbl3t 3lXAATy4HIGmIEkwQQEOcdHFvlB48UUSYCARxhVijEFGGWWYccYVaGDAsEgiLEDQw8ZCBPZAXno0 wgcrLNvx2m8ukcYHZWNULcnYtiDBAXj+9ziQ3Xn3GHNxfOfdbrcE3LxpARRU4ELfo37EwwQfMsSF Gj+swUYbbrxRBBxxXHGGHHPQUUcddtxRhhhUrLw1R/R5yYIDYUekgwNlBzttRgo4gAfbvDOLB8Ub zV2cuPAC0K6Pj454/N/JG+9upj9+aDiPLwukskAG1OhRvZDfW1AeeuzBRx9+/AEIEUZUEYgYZsxh hyCDEDJIIYbMccYhC6/ekYYDNRDCRQn4QEH+s5EFIOIEvUugm5aAiP9lRHglA4AFWsYDIk3wZXJh ngQpKBdDYfBHlbqUQCAlkAC0LDghKQDkFqUQDCRCDYpYBCPaIIRGOAIJcXjEGCBBB0H9ECISkpgE JSpRP0tcwlb6q8gIvFYQHTCAfxb5QOxuZ5EQpE2BWIzQChxIkgHozSBeRN5BwkiQL/5IdQYpXOM+ grJFGUCMBcFEIjLhBFRpwgabAMMRrMCJTszBEIOIhCc+QUhJEBESoMhBEi0CAtgZRIoZQcCuDDKC uEXEig7KoiZRsMVFMmR4CeFAIkKxB1HwKwpfmMIoSBEIS5ChFIb44SAJ+QlJEIIOZ6ACEj0JkWF9 zQEbgWQTaUcRTGrymCngJBeTSAED3AuUCJGjKU4xPj/QABWqZKUr7wDISBAyFapIxSeISIY4KJKX GYHNRkSwzIEowEwSUQAiNobMTf2SIGJJDNXIIoiQHiTihauo5jWnAAZWWMESfqxDIAmpClV8whNE bMUVXBERDCUxBPgsyAfgmZGHbWQED1BbPY/JQF+url4HgaZBMvBPNVCTfKhMQhGyAAodvqIOhQAi LT8xiUgI4hWP2EREbuOABViSLLODYkEeoFSMMBUhIOAoQ1jAABOMdKQqeGISI5VShXChpdTklyZg YUM4xMJzZYBlICnhibYO0RCQeIQjZAGR3DyAAQuQKlmoOBAWPKAjDTDp1x5w1IMsIA1Xveos2vnA DhVHhAWZm07SQgEXAK0gKi2ID/5pilKiioa0IMIoanHQMbSCDoC0RSRWW4lC/dihDFi4hdZS04Da 2va2trVrblqjA76aBQENAKxgCSKC4X7pAfTEIi5yoYtd5CIXvEDmDhBhXIvgqTg6OkiOeCIBuRxg AmjEVkI2O8pe+CIGvwDGH7BZBBxeIRhmeIUdDFEIQsivEHWYwxiE4QgOAIC2uA2wbXR7mw+EQAHV xcoIQoYQ4AoXIw3YHRaHQYxiPIFJNBCCMWhwDGQkQ5N4CC5EDMUDCYxIcUMb0XWDFB0UG2BHFtgR XCaAoyCxiMZrnIsLhrYj6FigLiacgImzRWPtQUQCgTpABBCSWYKQd46KUAb5NLGMIaBhFKwABRbO YIZWlMIOdTAE6e4gBzH9xIEI/n2IXemUIbLwRiF+fbBCfEsQBCAik73TRTFEAVMbvIEIjjACHKhQ BGY048NYJEGC0xiBDunpXR1qQV1WfKkI7KgFRMOTATSl5MItR4J8Gsi7koNpHk1AABU4gAuSg2QA LC5IPJBIANwlEAGE2iBNHsiTnUFNILDhGTdAxSYcQQXSYiEYY5BDK+bA7FfI4QzCOMIQlFDXB9BJ r2MRQVMN8tSNdDshDFg0BCTMO2hE4xTKYASwmUEEMGQhFoG4grwDUYUi6AKLJhBxQxJFrgoE4NYR GACl6xLCgXBoAEvuUwBULRDIGi9HeqkLwwEgnLx9qkMHQGlEUCgQF/14j24I+cM/y+uLRZAvCG5g BsDgUAVQXMESZxhDJ8hghjGI4QrSAIMQOgARKW6blxv9KDAXkgAIJAQED8Dz2qahCHT/ghp/YMaV SfuImE/NalhAQjAUiAJE0NkgMau1W7DnHMdSz8aU0hSHIKsWETp8Wy5gkcSNZAAXuIxREdBTrhNC nBrVC478PAgTRp6IJgQUCOmNAixCCwYqsCIO8X7EIzjxCCwEIhZUmMIzqoFOODdEnRph51R/LhAR lKB301hFL/hsTVSI1qCcGEMZ7iA6OpQCEtaIAzIUWAImMoQCoS4RBYhmPQIM/C4CqRmHBicQxLnd SAJpQaCaeXYJ/uIFRIoj194R8l0VFcAFBPDe9itAeFNco+R9YNIfbEALgBkhC6SIRRywQf9Y1IIK aLDBHzqfEB3oWyEepRHCVBEfoALltgqUYzmYozlOgwXWAAmwVAiDMD+GUApmEAa7kEBLMEkM0S4t QAERwBwuYCIFEB0DBwA80AIRBwB4Eil6cXFG4nDrcgB0sWpuxwMUcAAlOAA4OHzXAxEuMIIlwgNj h2sLsQqE1wWnIApr0AdQMAN/AAvMsAloAAaChgSwkgVwMApEAAhtwAT8hxD74RADaBGS5BAsgG0A AAKI0DvRoAfXYEr98i/psz5kMAc4VQlAJAm2UAilMAasMA0J/kQChQVGEoA45PJjQBMAyeEWyFcB fmIBI8KI0WcAkvgjeIF8BCFpkog4msgjkgI0wycBQlKEDlE4yhNegSd4hKcHvRBQMeCETeIGUtB+ aFAEYJCLRYAGSYAKUZAN2hCGBwECpGcQTlSMD1GGc/ZXBqEAs8A7u5AI28AN3eANwHADUkcF0uA5 PCQIlSAJtOQJfVgKwVAFCVQCGbU6xmcAbgR4AvENSDhyptALP9ANsSgDwKAJNwALUsAMQ7AJADkE zLAMXsAGeSCMEMZYERFAENEAlhQCVsU24JAIXfADMjQDqxIOOOSAkGAHOQWO4WgLhlAGYSAOvaMC RudJKgQ5/dDHioS3DdfwA0z4BIzgB8+gCX8gBLDwBV9gA0JAA23ABuMQjAhJECzwdQfxOrEDEbNT iMmIQGujC//UBJXDBig3BDcUBxzpkbYwCQzlUJJQCHdgCUbQOxvIS9xjLwvxZP+0Db2gCE6gDEDQ B2zgB8DQBkGQl0HwDFDQB6JAbUVJEAngew4xNhJhmBfxALxDDP9kXpZzleHAORzZQ5XgleAEloNQ CmdADrjQO8zoSY8TawvxDXJEeKGQCacgk4swl97wCzLwmr/QB2vwA1wQmAWxAAz2EA+TjgwxMUsJ LFPUhmwTj455OauCBtpYDmeQVoZQCWy1U5EwCHTQCbX+kIG8swKLdhZCQ3wLYQ7nQHiJoAfO0Aup KQp8oAxrAARAsAbK4ATXUJu22VG+0hDB4gDZ2WD/dxiItTa4MHL0uAa/sG7tRloIJV+FoIdeyVPR +YfScAi9kwb3+YlgEQBq2RDfwJb/FArjuQer8AMe+gOrsAfbkAHxuREssCVdkhBgIiYUASYFgQD7 2THiMHJUuQjegA408C/tFQZbNnt5uFqrRQiGcAfWIA3p8KD3CR1jESo5thAZEI/gGQpqMKVTGgo+ 0AMlWhAjgIzAYhr6wR/+wQB0gpQTAaNsI5X/1AWr0A1OOFZDEA51GHsQaAg+ZF+DYAh0AAmWUAvG 0Dv96sCbaTQvMuIVLekQ38AEpQmeI7cOqigV38AOGZABG7ABSgAeIRFYuAMgdpWbHGGma4MMI6cG nsUGM3ADgAAwSBAL5WAJO0R7YSZmdPAKY3AFcPAHvYMHnHoQlxIphGKKUzEde1Ed1jEkC9EDGcAF PpCsPsAEHPANWPENG9AO1YgOXiAEXwAIUeIKWuMRmFoR96Er+9EfYTqmFnGiLxqjHDOjGeqYN+oF sGBlo3AEcbCqUgMJc1AKpXAHkNAJnBAGYLAMD/qbNlMXkSOhvzqsw/pxZMEEojCtOboJ4QAGcMAK sRIO7sAOM3GiXFKIKxoCXJoQDlZn6Oos6jqVa/76BKR6A1IAsa8yr1U3BmZANZ1gDZxgBUcwBe+A pAxxKUKzae6YpU+xBfBwChdpDLRwZUcQBuWABZJ3BdgwCvGwSyvRKw1ApsQiLBOxRC9KAmzDCy95 DfLQhH6gKsIWaEcgDQQzeZZgCZWHDawABlIwDzq7ECI0AMOXcEArFT1AD05HDTdAC3BKddbQCWUA CWXQCcEACpdAlBgBAlZLSRATEb6pEYrJNvVAeJlweL9ArW4gbOEwChMbC2GADVZgBaAQC0cABpug CffGOw9gtc6BcMojmnkLFT2geqw3UFjGRzv0ZaNjB3NgBldgD1I7EQcSEYgpNo6EEQ4gUhyTDv3l d37KgLLAEAWd2wjtJmhZcASswApZQGhJ4AbeAA28gwKfqRA8y0G1CxXwCEMyhDmNsKMcGYHxQwiF cA+QgAUUhRG9AhFKWRFNKTF81QAGyJ/g2QV74ASLQL2aYK20sAmtAgajMApgUARE8Aaw8Az4cJL5 yRBktL5PsVmrxy9Ko0oEmlAHSgmTIESEUAdlYAXnhBL+A0ACpGbblgDqsJitiJoKTJPoEAR/QIuA 8I9JkASbMASAYAxtsAa5cKuECcJe4ULbQE3ekA/mQwTJuZyUSQk7RQmDYAdjgAT6gBLHiBHKeHQK iQBcyza4AKXhSZ4KjHhQQA1ArJM82ZNC/hAFwNAHOds7K6CGUKwV36kGq6AMAfq3yLmND7jFO/UJ lPBTWLABGMECAvtIldxLHFgRDpBcHBONpomavmCPfcAIUHCXQeAFUaAJQUANMkCT5Ms7O/BtgcwV /lR4lcMIM2AMVqaNV2ANZcDIn9BQPJWZZ4AGxQsRSPexAZgRZ3xJ5LY2jNmKTbAHMqkMMfAE3sAI MgAFUCADsbkI3SCIvWMCKTnLXZEHU3nLbWC0iaycv+yN4JgK8lxLhGAHnXAI22oREOCUAgF6GSF6 C/EaILvGOgyeakCeP+AEfLAIMaCeQBAD3eALTiDOvUMCl2zOL4EAIXCfFvGdtgygfstu/aOgPmIg B2oVCQlKSJRQz50ACvFgEkGnEcucEA0AqAPBAAXMO9ALnnqgBpmwB9zgoU7gBCDaC/tA0bxzApmM 0TLxrbfB0RVBoz9gyOiwXgR1BKAgp6j1Q5LQVj0lnZ2ADe5gErLsVFzaZgmhACO7NuIwkYoqpV3Q BE3gDGoQCsfwygmUBrnqEwNQAAXwswzzGh9gV1A9EbVMkWtKPl7gZ45gVuUQDHfokT8EpEJ6B2MQ BoDQUTWMEHHGEd1qEQwAlQm0C/ygqOBJDJ2JRSfgAB+LE3Lxb/oDAoExYAT2AQJ227gtYAVCfmDF B58lBKGFZTXly3cQZvVFgXlajjb+oBEMUMkhuxGfTUmPqwAErUDT0Az9EA1OkAj1EA3+oAt4jUUr sNc+ES/6MwI6kBoEVmC53d65vdvyeA1OgF7A8LDEpj6xRwav4LukQwetMKtH4AYy/XXPrRHRbZTN TYbPnFiaZAJLfRG++hEg8mLdorC3kt6aihuFLRG83ZhT7YQox25NEwvC8AiDWwavwGxzAAlj0K9g QAMl0dnQXV0IUM4MAVLOy+AKNF0bvhAUWhIaF33CuESr8QA9HhGEx2uigHj1bQPwmgVoiwViYA0y 1wljcAaPYLNTsA6sI7BlnZit3RAJsAJKp+N+/MRv8ThN6hE/tjfKg5AKcOAdkaj9oUCPJicDbaCy jXBlSFAFYRAITCt5j3AFoPC2qHCQH0VYBxHTHTV0Wvq4BtEAp2fm57jZGaEW12IRJcIX++RqQGMB FqAWgM3UC/FVI6eEohAD3uAHeS4F2Nt4R1AF8kd/YSANqfsGXpBmG6EDP+fPGAHQRvkB5L0QLPAB k07pa2MCrL0RA0CKp2YRQrNCK8QcIGIi4NVweNOopM4QLjRyrliPQHCjQXADX9B+jtB4cICFWYAE RlAEm+AGv8C4IzHTF3HG6a1EDpDTyN4sKkBMG4EcynFr3XJ3dxcoA4E3oTIikWM8FC4AtLvtGJGo 0hiTcnmjeQ4LQzwFt5iLYP7gCEQwBBnM5R/xMHHTzBJxhmaTMfveLMrOzxGhFx1XqMbTN32DRpNI NNRnPC5QI7YG8RohSkm4B75Q8U8YBcZgA6hAC/+4CY0wBKhwAzOwBhgLEiJg6QBQxvUeNiNg4xZx NiVQ5vteAv6+EZCiFhGwfQ0RFxQ3dn5icBbu8xDh0acu9KIsA+jQBl5wAzoJJW5wA5qADtkAnzKs kBDBkAPRSDY9EcW+Apxs5juwAh8Q5g8RIgMhAKJSEG1hHfeS8CjYIcRxfZcP9xhxuwdMzQsd7jKQ D6aclzOADmwQA+fgrCQBXL/yvxQRwAQB6RBhQBFJ6SqACGiOEeUyEBTa6f2Z3xf3chxBMjyW7yMW wC2ijxFAT3gHvQq+cPp98AuuKQOM4A1P0A18gKUxbhpks7zIu7xVLxKSlAaifVVuE24fYQHY8V2X FREU6l0T0AKYnnyF0ukAAUDgQIIFDR5EmFDhQoYNHT6EGDEhh0QVLYZqsmeVL1HdlK2JsUYZnx// ekhEeVAHixEORERU8ECBwBENEKSEmMBBmhMpfP4EGlTozyUlHCRggVNhiwkCCAgcYGGCiwoop0Kd MIHCAB4FBFQwEIGCUrJlzZ5Fq7THKosWTXXpdWrVD7qKTnWBdzItxAYORoxg0ABEQxAQXC64uXch C51pVKAYGvknChVp/Y4mVZwZQIWnUDsPOAB1gGbSpU2fBvCNS9u2ptS8VmNqFRPUC0EkHfHgQYgR CUeE2M0CQojBtQmyUNDgwSwTSyQTNTHrwQcFmI1fx55d+3aBW7iwZW0RE5NvBhEkmAngfPr1Atur R+8+Pnz2888nGMi4wQIGDEIkQECBBBIIgQHd8OOuIBAUKPCBFdLAI0IJ00jjAQYgUKC4BDfksEMP I6qAiTx8IJGJDPQ66D0V7WOxPhflqw9B62gSYYEGblwAwBk/FIgFBHQYMMgEdEBgRx6PRDJJJZdk skknn4QySimnpLJKK6/EMkstt+SySy+/BDNMMccks0wzz0QzTTUc12SzTTffhDNOOeeks04778Qz Tz335LNPP7kMCAAh/h1jbGlwMmdpZiAwLjcuMiBieSBZdmVzIFBpZ3VldAA7 ------=_NextPart_000_0035_01C538FF.AF7259D0 Content-Type: image/gif; name="mfree1b.gif" Content-Transfer-Encoding: base64 Content-Location: http://hyperphysics.phy-astr.gsu.edu/hbase/kinetic/imgkin/mfree1b.gif R0lGODlhfgGUAPcAAP7rxs6/oe7cup+TfN7OrUA7Mr+wlX92YxAPDCAdGQAAAF9YSm9nVzAsJU9J Pq+iiI+Eb/7OtP6/qv6wof8sT/8PPP6Tj/9nc/87WP8dRf6imAoKCiYmJjMzMxoaGg0NDTYmKY8A Hf9Yav8AM/7cvf9JYUxMTJiYmIWFhb+/v8zMzJmZmc+/wvUmUO9AY01NTVZWVjAwMICAgN+Ak/92 fY+PjxMTE3Nzc3JycrOzs9KzuexNbKampmZmZkBAQOZmgNmZpv6Ehl9fX/wNPdyMnOlZdllZWR0d HYyMjENDQ2lpabJyf/kaRtamr+Jziat8hewdRp6PkvIzWcVWbNg5WXx8fMxMZuUmTPITQL9fcvkK ObhpeNJDX6WFi98wUzk5OXAAFqJyfM8wTwAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAACH5BAEAAAAALAAAAAB+AZQA Bwj9AAEIHEiwoMGDCBMqXMiwocOHECNKnEixosWLGDNq3Mixo8ePIEOKHEmypMmTKFOqXMmypcuX MGPKnEmzps2bOHPq3Mmzp8+fQIMKHUq0qNGjSJMqXdoygICLAgIwnUq1KscBBB4WMEDRAFcDBayK HUuW4VatXCceOFC2rduhAxAgYAtgQIJ/C54yOHCXbdwGUhnIpcvAbloAZwU4+AdYYIC7ees2+Ocg wOMEAwIwECgYs8ACB+Q+eEu6dEoDDQgISOA1NYAFmwsUEEAAAQECDSAIOJBXQIPRBX4//cy1AAQA BhIIWM3VwYHVWSE4ELBgAQGwAHjTbsD13+YHCf1Mix8PcsFoALcXHPCKGvH5s2cTPPAKIfb5gVsJ hBe4YMCAzQBEJaABB4S1FnJhJZBVXQsA8M9w/5An4YQXnYVfA7LJhlha8HWXYQGxHUYcdgKtdeBA vjVQnYFsYRehQC4O9CKFNNbIUGElPoBjgMdZ2CEArgEQAHAibigAAgM58MADDQLwwAH1CfQAiwgC KRUAUc44o41cdgkjAg/EdR2YBjgQInGI6XYAdw/8tmFBZzHgAIENBIgABOCFyd0AwRHA23VhtRmm gg7K6OWhXZa5wJVlGicQVo9mBZZUfCoZaUGQYgnicAQsYKmmDCj2AAEOYDWAlA4sWuJAdCHq/eqr sMYq66y01mrrrbjmquuuvPbq669JBTCXTZpRVCywyNZ0AID4FUnRiRORKJG0yVabkgADQJAVddYN hJtuQkIwwHBOQTrAAQQ4JeV6AVa3IIwCiIscu44dcB6JBEAALoz0HvZVWAGe+661BHvkG2wJWJaA Z48iABh4yyLwVHCAMdDAmqy9BloDDFx2qowXYwgaAlzZVWCD2D3GgGBZmXxxoQJFiN3Bod1X8M0Z RemkA9m1iuYBV8LH1pFPHWlAAAD71nNB/3y1314ASCwQYNjNKZC+ACiHHs9aVgkBXQHwjPPYFR4W IbRo7uZAAU2/Ke1WfGWIQABow0ziWtL+4h3WPxk2MCfAhsZcZXByk204RZ8euTRBQhfnuJCAbwXB AuwZsJvPdgO8VgB1cgYBdiSzZxng3Rla9efsHa46RAOIPfnizTr4VG2PZy0V7Y8VLXHdL97NVsIB Knh6iZvNLVnUT0Egc1jSwdj56tAvtEACDTTwVN0LVJxAcNm/6eT2C3PFwPYInGrXx4JXubSwBZRf 5WMUP2VX+4Ftv8DyARJufPT8J5TuQpZDj1SiUhDLWS5I1xmOkAbGkAAa5GgEEYCILIOQADirf7uy WJNekoDPrQmDIDzJA55SGZh0alMhTKFJ0KXCFqrEXiR5jNg4cxID2MyFGDwS5kDSwYH9jOskdsFh Cu83w5AQ4B9XesDtTpIxIfaPbsG5SAAW8CHZXOlR+0mObG4oEt44sScRiIBAJDABMSJlOvezCG4m Exy+aQ5KqaLIdSpHxzra0SsD+Md87sjHPvrxj4AMpCAHSchCApKBKwmjQChQAQsI5AIYcCQAMoAB DcDlOAdAokEy+Y9OevIfmDMfzx4ww/7EDH0PEUABNsABDnSyA7CMpSxnScsOeOADtcylLnfJy176 8pfADKYwhwlLEIQglh+IDEtEMAJJKoQEZRRICSxAgp6oEkZ6vEipXnOc14hNAA+KiLBMcIJyoqCV KVCBOtfJzna2cwUecKc850nPev3a8574zKc+98lPfLKgBS5ggTpT8ALroSQCkoxANSNigRKYcSe8 WQsDQGkRcD7FeAb4x4LaFJHVwKCcID1BDF7Qz3V6QAYlTalKV8rSlq50Bu4s6Ek0MAIRaEQDNFio TUhFEMoYhE9VlA0qH8UzAyAJAA54HmwQwkWBOCAGIQVpDWxwg5TKoAMuzapWt8rVlnJghyF5KEYi gIES4IRyBMGQQeZYRwau5lQFEtKwkNO04RgArQ/4x1CRs4EaRBWkOPhAOvuZgg/koKuITaxiVaqD HdCTBxoNKwYuQJr2MG5LEPGN1DLJAAggYDP5elA3/bSwyegVTh/9K0g50IOU/b7gtT5YrGxnS9t1 7uAH9XzBBj1CAxHo9CMSyIAEZEKqEqLKOAp8SABOixwETCeP5lkuswaiPE9u0AAbUG1IAzvYfV71 lbUNL0uB8AMgiFedOxAoPXMQ2aIEAQNe4qQnXeMAcmp3tSjdZwpcCd7z+lefQBiBgHXwX3u+YLoZ sQBlMXiutVCxAXf6BwruC1IhcICw/MVqgTdMzx8IeATm5bA8V3BUjUygAsNNiQWciagDQJXC5azB Pw7Lzxx84B/xFLGO16mDIYxgCASuLRFckE8PNLUiYp3pCFKMKAcIAcYgjUFV+wnZf+z4yirQARDU W9sdFCGfRkAwRZKsEg39kJlLEoZyOYWg4X7KYMZYjnN4gRDke65gPxYhQQYs+cUHHEHNMbZySn2A BDkbOs4fQCRD4QsTDQThUAdIAqDLeYQVpDQFUz60pjnsg72mZAKgBvVvIyKBEZx5QgVQgmqXsATV JqG1JZ3BEJjQhE3buqU7cII8gRDidvZgtyeJQBAoMAIKYODYGBhBBkQwgYmY2UtpDukToEBtKEQh qkKIbUl9PAIp3PrbKW1Br9X5zxa0gNbvfJ5ELGDTiESAmSLQwKgBIIELZGDPvQpAdkMaBShMoZxU gEJUq5DjfnKbyOBOOIDdKQXHqsAJTOCyOjELkQywuCFBqIAITk0QC/1UoATzXgifa/QADkTVClcI KRayEFVB95MIUnBBrRV+a1kPgQj9nAET2CkF3LLTA1dkaEREkIFmO4QEJRAuRCpgdBodwL4g1UKr QZoFLES10jTPOj+ZIGBvbx2m6wTCECTegSN3RAQUCPlCaIDih1yABjZaQGrLuQWrR1ULTwhpDAqt 9b7fk+vdtucPfK7OJgzBnS0Auzp7ANaFkIDjB7lA2ikShAyoHVYFwEFIqfDvqHKBCyE1Aaz9Tnp5 NkEKUpg5PXPNzh84nJ1OQLg6byBmhgSh3Q3RQAUgzxARmPVWCaiCyvMe1S0IHKQwMEKByVvn0p+3 CRKXAs7baXh2/q4AcA+J5NErMHKK6Ln7ChF2jf4R0i6MQLVROD9g2yzeAP+4+c4v8Agkvk4gr/P6 IqEBoy9igQw4JLjjF1JLkHKqBQVTdwI4wH7h5WECNm7x519NsHPyJH3sRHEcUXQagW8NsX8SEgB/ BlJWAHqq5QVbAFIoUHDtJ2Bjl1jM94DtNALsBARe506DV4EREU25538acXu1YgAmB4JWoF1WEIQg 5XLnpWX0p1XuZ38uqE4wuE41KE9O8GXrZIEK8XYOcQELlhERUAE9+IPldAUHeHJEWE5G2IQMCGJN qE7jFoXuJIPsxAHJxRAY0HQLUYcc0XYMMQGPNiE+GFJiqF0D/hhSZ+iCTaCC8LeGKrAD0/eGM6gC HXBBGWFqHIGHe8iB4/GHIBWIq0aAZqiIPEZn4mUEHEBS4SUFDhh2jxiJIDECHVECfbgQEhCL5PEA XwCIYyiAnngChQiKtYUE6eQDPKBYcLhOqEhPqyiJCGGHC+GKHEEDcDcrT4eLgriLveiL4dUDNIZY xahOxzhPT6hOrPgQztgQ5agR00Qr07iJuQhSg1iE2FhbOeADH8BOyqdYLKB6KvCN7hSB7DSODqF0 DbF7lciMCDGLFPIAksaO1UiIOmYE2qZOPnCP7NQDoxdnLxCRMjBYOWCRHmmR+aVV/NhO3QiJyngR lZSHvCcQ/ROAieKhiWHYjnTnBQ4pYpA1WCnwD8PoaxeJZR4wZUgwjNtYTzywkyu1A4pHkskIEjSw hRgBgA0xAdEoITB5AiQohGXIizt2UuokA/GUAkbQAVNmkSoweq2VAzKABB3QAwTVAXwHlmvZXfrE Ay9AS0apAux1WPAES3xXTzIgWP1Ukm6olP94kgYRAQZ5kDqYEReAe7JSlUOIlTUpYjegbT5QVay1 AhNZlq3lcla2Av/wAivAASeFBHCWmRlZY630Dx3gSrCkTkhgBDdgBChofXWpTpBlaWX5AR7Alvwk mFRIg8GpAhwQdAzRWw+hgRjBdF8YUlMggn91BSUIjzr+xl4pkJM5gAQRKVhk6ZkqAE+Ld48dsAJI YIrEWZGf9A89qQIoJQOxpZ3rJAOm2AHm6U6muU4+EJIf0Je/GYOPyE5FQHgqYIUJMQG/1xAWQAEZ 8V4PcaAdCIYn8I5/hQXEdwI1UJsbxgFpeWFkKY4r0J1V+J0a1qHj2QPpqZv7lJ8q8AJT5pWDxQH8 2U55qU5GMFg36VLVN4HjRqAZSIsT0YWJeRBdGIAglX7op37llIBXJp8v0J7m6QEd2ZkD9ZkjCmvj KQMUyQPd9aEfiaLslJPp9AHDWFj5Bab19A+WlgOZJgMXllUjkIgq8KY2KBInxmQTMVkPEQFTOSHk hwP9OCAEJgAGYfBXW7CLSrpjhQWYKeABlnYDWEWWHjCML0Cli2elK2Bjw7gC9Xh/H9kDXhqfsaWp s/cPg8Wm9rSfZclOL0CR/YRuxpiUhSeB6rQC6uYQCAURGbeSCIF2l4co95OeSSAG0AlSVJCVMFCf ImYEWepKPpBOMtCeH/ABV6UCPHCPz0qjw4gEHvAPHHCX+LSoKNUDWMUDPqBhheWb9LSW6KpOMCqX +zSSTvB661QE8op/7uaFECECepivk2crGeVJG6BqdRdVUYB3obee8ahfHACYJiqbPnBhKYAEH7AC N+Cu/xipXzpjMapP0MdOPUZ/TNCIKnADwOYQG/4XEWzno+FHAf3qEE1JIQTwAAjQSUcwYeWEBdNZ TllwfFEWkglLZf+QX5rarDyAS1WFSxbLTsLYTpCVaS4lBboWdrK6eI33ERNASUE6ECRAAyOwpwGZ tW2xJFyhPEfgV1RndycQBTgbVRzwqT+LjWLHZS0QtfjpaSGxtRVAAUFgpwCAUPCmqwZxcW9BAAMw QijSABAahlSQtl5Aky2XtG9bekDQAu60Ay0gUJbrThxgmAmhAS75EOyWAcqGAcQ2AhgQBIBLcvNx EAFgA38VBVeABVrgBdcWUiiwqbSlZXAauVwVjuy0A7MmBUnIo46nnBVBRhPQq7mXuklBuIabEP3/ YLZR1QVdoFpKoIDEqIJJyLtblYrqpANwSqsWoVAyAaRtIQBhYpwIkWqTdgKvJk8swGtblYbey70F RrJKgVNlEQCFCxEMAHVqdgQbu48CJqDjhYj2m1j5mKLdZBE0ILjJgr6ZAhF+NmkylrQf9p/j9QO7 m8At5Y/69AHqKxEnxrwdkbxiEbNmxxDgJL0wpgRtynAF7MH4JIOpx2FDoI9EWWIXgcIrIQHc9yoN 8GRq9gUIqwIs4ASwSsPzBHgarGm/hhQrBisQ8GJQtgHeysQG13UJZ2QccbV8W1n/0MBRg32Mw7nr i8beEr1QpgQYqsX8JGuuumEz0MHrxAM8/qwRF+CgImEBn+sSGfU8eWXGsTMRFqIVc3dfUgbHD+hl 96RbRdGF4AcTYGEbnLE2juEp75EWEFAA3SIkDmA1XgEjj7MbIJIVzitmA+C6FIYCpMrI8dcEBuxO hTXCGuHHJuxuNgEWC9BN8hEW+lG4bhInc+JZ6IEZMusndHEgZ+EcBgAB4WFUBeBpCUDE2vUFyArL 2NgDhMwRJLDHHfHNCooTYNEeYYMdneUYdbIVqzEQDGAAOzIfJ8LMXEEX4IQcePZTNuDCIVUFhqXN D8gC24uXH6DGCaa8DqEBDpUT2KEghYEdhxwhW/GvnlQgIjLPbHEWfIIAbKM+67uQf3UE/UcM0FlX BLLXTj5QeyGBAft6gyIQxjeBznYhQWFhSse8IbjhLZ1yHvJMGBltAPqxIPjjPwhgzSD1BTFM0qXH AnO8TjdgUCiRYvU2yYdpRpOVyyuRMglQVGGBGqqhHm/iGfrBv9ZTG/zLM8Ly07kjABPl0RWEAHNX A0gNuUodfz2wP4lEA7+n0HBnATRgdCwNwTtxLJZyLHbxWZwhFUjzDwwTGp6hSnwjLx0DAJ3ROpWh 0gTBOUdgAklgA9xKTKAd2qI92qRd2qHtAx/pAQWgaCyBUI7k12CbLE+yHoZU27Z927id27qN2w22 OV/028Ad3MI93CGhLsR9Ebdx3CX+ccjKrRZVezjGDRPM3dwRUTfRM90tgd3UXRAH4GnWvd0bod1K ocwmshZ2uxRsgwDmQRDfjTOcwzeBIRVVJCRsZMseYSEStNv6TUgTQRsFkd/7HeCAZFqeBBoE8twE AzzNcxbsoSLMcTzLbdBTwTmsbRRsU+Ds0t4381mHcchUVBdz0hpzCBLinRQEAiAEsNolMrPPMRVs UyrJpeEFM0UQ1iNpMQAGFTcZYt8cUeJJERcC4RsNzDBTMSoHIePWQriOIdFckcxSskH7MhI+jhTL NRwMsCBHVOFVgeTWcicEEhb54VwmciQeVKshMeVI0Ta7MRDgURpcXi1ThEJYQd79B3JCoQIsbRPl DFCy4N3ny20vQTfNfj7oJxEcQ6VRK0zoio4Rgk4QGdXiix7pHaFoEi7pln7pmJ7pmr7pnN7pnv7p oB7qoj7qpF7qpt4Qkz0RqR4T3dwQx3Lq44HmaTwTdEG8D9TqsE4Ut0EgqqEvw4Et2oImQtLdKOLr 6IHlWWEhdIM+y/5A8bIv2MJCxz7KQX4lBFQu0s4Vy3UYEjQQAZAVdHMvwIzsyBEvp0Igh9Hsue4Q 8TInKS41HcEXZsLRchIWBzM+8l0yCXAASRUgKiIYl1MiP10X+97vbcLvZszY/F4nNAMm2dEARE4i EJ0Ae74fETJR2Lc/CWMynv5cJRjtICEjG6Gh7wu/7g6RVwSwGW3DEOn5SQgRV4hxKvesM6QU1sNR GV+TIx8fHzePNOeBOStfAA+Q86CcHWYs8WBOF9wBM5i1VO0B71RDJUvTNsnBGb/T8ybPEPx+HMv1 ESdiIUxuKBPN0bLRQcy9815B9gXQQXnEMQw0I2tBOLKBJHWD9N5zFi+CWVXfy3mzHlJ/IL3zRtJc 9mSc9QdRPdGB6xbx9WkRIYmDJFvBOZVDKmlxG2gv+eyxLfDcXumTHdKBOqNc9wAD0RxSOjBDEAkj MZzjzp/z92wR+AKP+V6h5VkPTnQB1g0RVBny8nQB9iB+NQ1yFvsj9M2TNf1DvxmrMfDDDx5X0hgy MhrQUfztUTerj1RgXvpMv0kFIDbAAx3YESXJnzkCHzVBk+gmn1fDIR+04QDdtCOOfke8L+wvMj3V MzH6vvYNokoQ3yC1ERwA4eAAgAIGAAxIUCDBgoMIFDIEEBHAvwYKBwAQUKAiggAADgyUGLHByAUF CBo8OTFiwpAACPx7EDGAQwQXDZgk4LCBQJUAbkb8eDDhwpZFjR5FmlTpUqZNnT6FGlXq1KILHER8 SQACAAcoGVB1SqBjUQEGCIQMcDZiWQFGy6rFaLboP59wAQRAmVTu0rJLDbRtybbpW7CFDR9GnFjx YokLLt79t9XjQAN5VRlfjkoX82bOnT1/Bh0a6YCvkkWfBnla9WrWrV1fvvkA8GvatW3fxp07cQLT un3/Bh5cOGiTw40fR55ceeDlzZ0/hx5d+nTq1a1fx55d+3bu3b13DggAIf4dY2xpcDJnaWYgMC43 LjIgYnkgWXZlcyBQaWd1ZXQAOw== ------=_NextPart_000_0035_01C538FF.AF7259D0 Content-Type: image/gif; name="mfree2.gif" Content-Transfer-Encoding: base64 Content-Location: http://hyperphysics.phy-astr.gsu.edu/hbase/kinetic/imgkin/mfree2.gif R0lGODlhXQGXAPcAAP7rxr+wlc6/od7Ore7cukA7Mk9JPp+TfG9nVwAAAH92Y4+EbyAdGV9YShAP DK+iiDAsJQAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAACH5BAEAAAAALAAAAABdAZcA Bwj9AAEIHEiwoMGDCBMqXMiwocOHECNKnEixosWLGDNq3Mixo8ePIEOKHEmypMmTKFOqXMmypcuX MGPKnEmzps2bOHPq3Mmzp8+fQIMKHUrUYAABBQUEAClgAIGlRaNGLEC1gIEDAxFgPRiAgMiuGg8g aCj25b9/XgUSOAuygIIA/xCWlUp34L8FAQIcYNBA4AGoBv8B/ihYo4ICDQ+bdbAVwAEHcT+6Vai4 bt3Cah0sbSpQgIIFXuGCBkDggIIHA7uaBlxaAdLOCg6kTX2XwFMCCwYAeBA7tO7Oulu/rrz7NEHe AYiz/NfAwEADDSILMPCPwdbp/xyMddwAQfbGA/33/kPgVgBiAAoY/CsgYK92ANjfA0BwuPpr7NYF pv9nYLbllJgJ1B0AkyHAgAINODBAAf9AIAABDjSQ3nbVdfcPagNEiIADqG14GAQFMeggXBCwR9WH AECn1j9NOWDAhqhVBgEEEwp4YAElmvUAWqRdGBkDYwWgYIpjDZCfAnc5xmNqmqH3z1tx7aVbegM0 4CCRABiJVQFNWikQAwsAANcAez3YQF//qRQgeohNhplWABQWAJpwCfSkQAg4N6BjBQzwz28QgBfn UnBhRUABaQn2mF8gninQAwyw6VikPQ4gwJIMnNeSYFc5ZkCdAVAKgIRipkUjeiDaOZijAjkA/SUA CzCA1FOSlirQqQVsB6qoByy4lZ9pqjmYYpMVACRqqqoVwALUJSspA4MdAEFec6JpF6GRCaSXd0s1 aUCYYFL7p2JnUhsoceSZpZdzV9WpgANVZSqmARA44GqtgxI0mUBu1Xlodg0gVVkA9NqrAIEHixmX cnGWSNWawZK0JqmT4WaAvUjJCa8CSDqr2JrvVpVrQXJGRgADEGhVWHd+etWgyJ61mWlVpmnKsLBr tezutNQ+6EBuCOM7ccII16nWAxcToBiEQBebcJ0LaPrgXdSCFbFJAWaIlFsDEG2Ac4W9qG1kmCkW qLZapZrla9cqLNACassJJpoMIFsqudv+wTdAqAM1oOlySxlgldsCOJAWAniZfKDQ0VK61qt7xhmz 26Qtvm+dl3oF4XQJm+ff1SJRrRdf/B78M2kGHHzhqM4NAAHZUCmmAARO0cg0fBySjJrRe9kWHVQM 5I6qbl4qJuRSj+m2uJB/r1TYAf9gZXQDB9LrFQOpO9y1phCXmJ6roDJ3GGILMAYA9rNTteDTkVE/ e1+FS2g+6CWJ3CmeWD3weoRe/b5ggwLAHoFeM5cNjaczr8tPQX5nnr5V5wAJeptzsgKZ/jhmO+K5 EnwYlKu8sQQstyENYHgjG7UsIDddI4ClUvM5xyjAUk6BygAWYJy3GeqEA0ghZ0Q4EBL9DmSGrqGf EIdIxCIa8YhITKISl8jEJjbxN06MohR7cqopWvGKNCmcoLAYEb04BnmD+SHRuEjGzsyvjBAh1sHg ZJAGohGNWkTIdKyyxaEIgG2dwWNnPhfCgdxxIGo0ih5TA0WB7K2Fbyxi4cY4kH7Fij1EgQtVSAcf lKEsNMxZ04YYhBUBzGhGAmvTwSbzGGMhymgPgBf2XGYAlDlgkIkkYgAb8LkloeeMQBFN5ba0ndQp zFraYkBoHBC0+SAmkJMRHgQSR5omHUp1E1RRLJNIAFASpEk9nB8icQKXw/VnSfqjHEEQkLcA+Ok3 50TmwbD3gLTUaS/hiVTZmjdNI/2+i2gFCKMWU1lInRiNTXA5i0DF2cgx/nNQ6oTPxfjzlIVpqk7z rOcSzQOmVA4Semex207+Sc5LEQSTBoncC/9kyHGJEmG0gg8EGvBOXskzdvSUqBHntK/jQOYsHvRn kiC0FDAJyDkH9YswYRWpfcnupG5Zy2sQwNK48LR0+cKXTK1YPoGqbaMvi5AZPwnSkMLrlZWckawk 5TQn4YgBe4tMKTPlMphOlYueFGg/uRkXcxbkKA05JEH+yJCnwFJMc30rGgkQnej1JKiCTWxMFrCe nrhRsZCNCfQCG9nKlnEuls3sG/+q2c569rOgDa1oRwtZCJL2tKnhmGpVS9mf/SQHXqiNLUPwOhSq yPa2B1kUUWyL29DyZjsDMMBvCFsdBWxzJ7ztLWjfZch7lVSjQUmucj37zyD6JVu1jel0K7sWqADT b1GR7nY1+7zBLK4o4h2vZX+GG4L4KYzR1a56FesWYO4mLq3lSXrnC1mqfI48B+CsfuXL37caYJAw IgqZqPKA/LrWurCBb0WmU0eRdG0jXizwEpH03Ttp5GsO3ojxsEuR5+X0IRDTMFC+d83zZimMT+mn XkM0xhzmsSB95EohYwxIxGBOwtrqJ22jetfgWM2QRw5QjlW8kw8hS38VM1a9hvNVNPHHlXhk0J0y 6RpLQuBw8DIsQdJTovn9hUyrSFoPXKw0o8+VUquOUSWiBJqcY6KMQenh0mtMaVg6zyfMFWYyTQ6z ADQ1IGoHO4xXoman4LAoTtG0774a5JWRpehgQtJN4fyDJKRcSjckVaqkdHk+8EAINSfrFrKWmS/Z PXpDxAMqpVKZrEzjzj9KqRqQ6XIAkfk60FI8TIZatT4AQABZa7GNIXe0lIjqK2GFSfajQETOgRx7 zGpbZloGwOxRZ6umu1Fbtdk5m8IcVT/nWRpsYDefvF07K74mcFT2pmtqhbiJZntAON0k0LMsJTor LYyzC1rrfrNFywIdI3EmA/DfeZvggDQ4YqZTwbZKqjIYR8z/rMJuhP2fhZESWa3IR07ykpv85ChX bUVSzvKWm3zQ5DtTmJI5mNIMNV8Dh2q+PDoQr/iy52PW1LF7l6wRQ/xtf7MNVDzZF3MfM91QZ93Y kvVztRDENCIX9EsUk6EhMXyCi4LbdZvt1mc7y6dSJ3rh8NhpMRlO7EpaitF1XtJZafvR82m63J+O 7r6LbVTsVjtYwzNykpjm3hxJs8E/3pHD10VGqaoYBDIF1pPNiM1RZdikl+4Argroq4JKT6YMa/mV zui+CPgnuJVkLDQh6ay6mfzkMt535oHpgLIfFehfkrqLIT4ovR+SLMNoVwIIeLZ6nHHQl1z8+xxf WTse8pIXEkIb/vdR+SzpFb/CFCztE4j7sb2ZYmfzmYiRH/yoxWxnhStE9mu9jAR4gKVhY5n4zx8+ IH//FeFCtPZ2pt55kUseRhrop39cBD1Q4X+2kWv15l47gYAmpBbHZYBMFB0FxTEndhDTsRMWWDoY SIFGZB6LN4A9dR6eoVqAwTZ4JCQZaEja8hEiuHhEU4KwgYIOCB8TCIJBcTJcUiIMMDNIUWjJkSQI oT+pUiidER2IkxTUcRQXY18YwYOdZyxACCsshSQF6F4eQlg/qIOWYVw5kyKNwSptlxA78hyNkR4I AWtjMTiJZxskdT+j4np4V4QsQkvM5YWWAU/Shh43tyEL8Wl4/jIbBQCFt0IqcZKFGcGHS5IeYLYQ BjIabqiHdCE20lJSjbFSDFEYF2YXdeQniKIwzzcRlpgqfpKJhkgQP/gaREiJURGGexIdaXEpwGYn MTIbY5JbYpaHHQGL2yGLnSFmCOEndFKHrkgUs/MlB5MhmkIdIUYjATZmorJAoqKJT2FXe/N7B5GM 57OMsCUQzqgQk4UnlJJr2rJrx0gT0LMV/EEwjbUbxiImC0FHBQEdfHVN27EWB9BgCKA2oUgR62gn n0Id5yF/kbJr9GJtDcBta4EsB6CI6ZhF2ZEW6vFKSqgVxmJc8whyG9NGmLFmu3MeAUgRl2I4X5Id AnCRvXYg/cflXHFSANyXT/oRkTUBST0HYZ4RHA+paRBZEND1KMiikUhGEHhRUm9jEUqjgi9EGjsJ Hz0pQrPxAGOIaaNIkyfxGFXpEQmCeGjRYDyhAGPxlFa5ElipEgmSlQXwAGIpEwEAkzk4lipRSvE2 l1WRUwB4l9RylhDRHG8ZE1oClzbBgHipa5poI3R5mDb5EDVERYBJF9XUF1bSlxchmTJBmY2ZE9V0 SSXRTpeJW4RlmRaRkp05mgWBS6R5mZx0mqOZZlmpmjK1NyqxI9nxk64JWXADmhlxKQIFbErRmrWp RAHwOugYOv32V2+WmL9pRW15FhPkPGchfAbhJ7PyLrX+mJxG1Gv9po0dsVJMJxfN6XbVaZ1CVE39 loomkRbVNC0hVYBxJJ5XkxyxkRAnI1czETKcCSsmmRQp5p5FoTQOwBeHUWEb8jrmyRK48TpngZxX 9538WRT22UMgRwD08iDq2aDbFSoyOWaMlEoWZKHqRZ3bWE5cQpseeluHQjtyNB796Cq4WaKd9ZgL 0TWLKVFH5qIZ8QAt6BPvSHdpJG8SYSy+aaNCdBbgt3oOIX4WsZ9CykRPkp+kJEOYdgC9hodGVQBT OhsH8DXIohfylxR+w30cpp1LCjqcgiZl5TYcFpzaESqJxhxzkirpIZVN8i5VpC2M0ZbHxBxiOqYR Ixj9T3Wm7kIp3Cg7xNQqqIFNzOKHn/N3oqakrqk0hbQsuTWcG0FhLlEYsRI0l+NQfXdxmlIeT8Ix EXQzAeImlEqaQEIQhUljJgFilwoVbgGonFor57Z9/LdaUuUsQeOormkgP7Q68ME2RlpkUPlRNWqs hJh/KIEZhWM5CQM9tBp1athMU/MbAhAmN8Ooj8arqimdbxMpnvRJWzNK7OOHJfIklLdUgGYQZzZK jLcpgIEkiVY34hGtfZemgoMnx5ZKWHEzQvIX+Upk/Jkyt9KGCZMusuokSAFrUmdrm0YQQuIVGbIU w4oSS6kWb0EahxEwUaotW+FFenEYCDAbUWMAW/5aRzQ1Guixp3CZqdJ5TiVVbJtqr5JSbbeiUawy h8XEp1akVGJ3UIKRsLRHVgY3RjUVSDx7RS/CajCbJX8itFEnKVVHGgSRs45SsUm7ROLxG1UaNNLU LEOrGIK3gib5p8qatUvkIn6EMrk3GUIyeRYYtueRIFyyRZskH1iLtlJ0j8aqjdiHrFFxrBGxQ3rb Wdy6kYXrWYerEHmbuE5kHu/CGN4xVllCHWgXbQkiH37IUAPkFwarH+phQYQFGbS0V25hL1sxuvJh Ho9xqo5LE2sGKwc0rYsTQFixMojiOlghLU6hIhFFSrJCWJDZHxIKTLFbOP+Wu2dDIoL7ujrVVf11 QmtvAyIC9xu9RiC/crtuVSy/EheuukK08RuOQlJ8ojAtqmFsZBAppRFgoX42YTTwO6tuIxiSRBWv I7CZd1Iv8zBHoR5A4h/VlU/rYb91RWLH+BcIgVhJSijh2RLxO3VwtxvERL/0Sy0AgE3Gl7+7ihfU sm3S8jfV1VS6RlDpyBlNkRw3hBnCoSy4oRskNBszBDSioUKvscJQSUMsixEP7DZNO77dAhWm9XcK ADbIYluT8XOeUzd2CrGYkR/YZFoKTInFkinvggBxpXEukmAkYiKxmiqpxFQKIiKTYyTyg2kNkifQ iRI7bDQGgiBD8jzasSGepiFg5T44clLx/gOiVZweBlVcOOIXcQxWUayHxVKQxDQ9aAIpCmMo/1gY SjwqqrN3Ouu0aQUVrKYSKZXJKdgb2jKLnwFFQARFq7FCOwRESglhY9M1JQQbQMNDVpmwRhMuefEn B7UtggEsJCPJwmNszMSjZDTIownLZOMwVKEUipMyCIhYTkdk/fJtZztFwNyZwvwldtMVRhPBfkq+ C6C9knLJF/wAqvfMzpsmwuwVs0M8IMI7wkRcFEtLyBsnMYIYUuKH4tS442wZcMJGDUSeeFJxG+RA 1hFBEvodAqIo27EfB/bP+HPPDH2xFOHQDC1YkGTPB7G4EW1FSmEQFJ1jvFp9YQSbF03O4OUKF/Si mUH7rveVFmLXrqoSzgTySa7CtpojZYMX0nQxs7p0Mty8evMTKBGbJU1CwQRnLF5RIteDraHIaDZ9 0yPtzPmyennitMLbN3rn0vty1Qfzbn241OjV1ARXGKtXOOjRF0eLGEINVVgNVYvnulyNEzjt1GAN cnUDLZOss2etqQmT1thkdW1NFF9bwF9NsSAHN5Ty008lGIJ4KeSqc18HyH1dFG/LF4Ct1kuxIYLi J0RztxQSOPAyI4tdTJKXro/dn3blEKWtENP3f4PL1qPd2q792rAd27I927T9fgEBACH+HWNsaXAy Z2lmIDAuNy4yIGJ5IFl2ZXMgUGlndWV0ADs= ------=_NextPart_000_0035_01C538FF.AF7259D0--