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      The Geomagnetic Field Decay / Solar Radiance Increase
  </h1>
  <p id="description">[PLEASE USE CONTROL (+) FOR ZOOMS AND CONTROL (0) FOR NORMAL VIEW]. To see other BSMRA sites the BSM Research Associates Integrated Websites Selection.   Also please use included PDFs and WORD files for higher resolution if desired.[PLEASE USE THE ASSOCIATED PDF FILES TO ZOOM GRAPHS AND PICTURES]. The Maxwell-Lorentz Force protects the Earth from lethal, high energy, charged
particle incidence.  GLOBAL WARMING IS PRIMARILY A FUNCTION OF WATER VAPOR GENERATED FROM THE 
330 MILLION CUBIC MILES OF OCEAN, NOT PREDOMINANTLY CARBON DIOXIDE (click on frame below addressing global heating). As the Earth continues to decelerate in its angular velocity
through the Sun's interplanetary magnetic field, the electrical currents generated
within the Earth's Geo-Core commensurately decreases.  As these currents decrease
the geomagnetic field, generated by these induced currents as Earth's conductive core rotates
through the Sun's interplanetary magnetic field, likewise decreases. This is again confirmed by
the International Geomagnetic Reference Field (IGRF-11) for 2010. The value drop is even more severe
than that predicted by the 2005 value of 48,288.6 nT.  The new five year value is in fact 48,238.6 nT; down
by 50 nT.
As the geomagnetic field (GMF) dies, this planet becomes increasingly exposed
to lethal charged particle radiation.  The Maxwell-Lorentz Force is F=qE + qvxB; where F is the 
protective deflection force; q is the charge on the high energy particles streaming from
the Sun and interstellar (and intergalactic) space; E is the electric field of the 
Geo-Core, and B is the Geo-Core's current-induced geomagnetic field.  The first
appearance of the so-called Maxwell-Lorentz force appeared in 1861 by Professor James
Clerk Maxwell: On Physical Lines of Force; London, Edinburgh Journal
of Science; ;March 1861; p. 342; Equation 77, which is vxB in scalar form (see enclosed PDF).  As the induced
Geomagnetic flux density decreases due to deceleration and magnetic diffusion
processes in the Geo-Core, so does the deflection force disintegrate.  
Geomagnetic polarity changes are not associated not associated with this 
Maxwell-Lorentz deflection force equation.  Neither is assumed polarity change
involved in INCREASE of the the B-field.  All spontaneous changes in polarity
will, in accord with the Second Law of Thermodynamics, result in further decay of the
primary geomagnetic field (GMF).  This is assuming of course that the so-called geomagnetic
field reversals could occur at all. So-called  "paleo"-magnetic data assumes the utility
of potassium-argon (K-Ar) reliability for dating the basalt basins of the Global Fracture System.
Very foolish approach since NO radiometric dating method yields time past
5740 years (approximately radio carbon).  K-40 and Ar-40 leach very readily through
rocks. Also the orientation of so-called "paleo"
magnetic rocks are not reliable due to seismic reorientation. The assumed orientation of the the indigeneous
magnetic fields of such rocks are altered continually since the lithospheric
destruction some 4,500 years ago.  In reality, paleomagnetic assurances are
integral to evolutionary dogma and certainly NOT geophysical science.  (See the 
appropriate PDFs).  Global heating results in vastly increased evaporation rates 
over the oceans and large rivers system.  Condensation and precipitation of
the water vapor results in rain-generated floods and increased snow flux rates.
The new half-life values for the decay of the geomagnetic field has been calculated 
to be 684.18 years.  This value is not constant and in fact varies as input values of 
to the geomagnetic field induced intensity varies, as well as time of measurement.  
Notwithstanding, the overall value of the GMF's half-life continues in reduction. In
effect the time required for the field to reduce one half of its effective deflective force
(EDF) is becoming less; even as the primary geomagnetic field continues to 
disintegrate. Current frames address the global temperature increase as a function
of decrease in planetary rotation; data obtained from the International Earth Rotation
System (IERS) for 2010. FULL TRANSLATION OF THIS PAPGE [http://www.freetranslation.com/]

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     <h2 class="date-header">Friday, 02 July 2010</h2>
      
   <div class="post"><a name=21></a>
    <h3 class="post-title">Geomagnetic Field Rates of Decay for 2010: International Geomagnetic Reference Field (IGRF); BSMRA Confirms General Decay Trend Since 1835</h3>
    <div class="post-body">
      <p><p align="left"><strong>Geomagnetic Field (GMF) Decay 2010: International Geomagnetic Reference Field (IGRF-11); BSMRA Confirms General Accelerated Decay Trend Since 1835; GMF Decay Energy Conversion Into Geo-Core Electrical Power, Induced Magnetic Fields and Heat; Half-Life of Geo-Core Power Increase: 50% Every 544.74 years.</strong></p><p align="left"><br>Current <strong>Geomagnetic Field Decay (GMF)</strong> data are presented in this section. The <strong><a href="http://www.ngdc.noaa.gov/geomagmodels/IGRFWMM.jsp">International Geomagnetic Reference Field (IGRF) 2010</a></strong> data indicate a continued 6th order polynomial intensity general decrease with respect to the primary dipole field. The 2005 IGRF predicted value for 2010 was <strong>48, 288.6 nT</strong> which decreased from the 2000 value of <strong>49070.6 nT</strong>. The 2005 prediction for 2010 by <a href="http://www.ngdc.noaa.gov/geomagmodels/IGRFWMM.jsp"><strong>IGRF </strong></a>proved incorrect, since the new empirically-based <strong><a href="http://www.ngdc.noaa.gov/geomagmodels/IGRFWMM.jsp">IGRF</a></strong> value is <strong>48,238.6 nT</strong>, a 50 nT drop from even the predicted geomagnetic decrease for 2010. This states that the exponential rates for decay of the Earth's geomagnetic field is increasing. This requires an adjusted (and more severe) half-life calculation by BSMRA which is: <strong>t(half-life)=[(t2-t1)/(ln H1/H2)]ln2; H1=53,984 nT (1900)</strong>; <strong>H2=48238.6 nT (2010)</strong>. With these input values using the <strong><a href="http://www.ngdc.noaa.gov/geomagmodels/IGRFWMM.jsp">IGRF</a></strong> empirical model, the new half-life is <strong><u>677.57 years</u></strong><strong> </strong>(down from 683 years for 2005).<br><br>Hoping that the Earth's protective (<strong>F </strong>=<strong> qE </strong><strong>+</strong> <strong>qv</strong>x<strong>B</strong>) deflective barrier against very high charged particles (protons and gamma rays) is going to: (1.) somehow reverse in polarity; and (2.) somehow increase in intensity; is real only for the evolution-trained types. The former has no real scientifically confirmed basis processes functioning on this planet, since assumed geomagnetic field reversals rely on potassium (<strong>K-40</strong>)-argon (<strong>Ar-40</strong>) dating, which is very questionable as both <strong>K-40 </strong>and <strong>Ar-40</strong> leach in and out of all core samples taken along the <strong><a href="http://smtp.antelecom.net/blogs/bsmaCIA/index_09_05.htm">Global Fracture System (GFS)</a></strong>. Also increasing field intensity requires (a.) increasing the conductive geocore's rotation rate; and thereby, (b.) increasing the core's electrical current density as the Earth rotates in the interplanetary solar magnetic field. Increasing the Earth's rotation angular velocity isn't likely to occur as tidal forces tend to slow (not speed up) rotation rates. Also the <strong><a href="http://smtp.antelecom.net/blogs/bsmasolar/">Sun's equatorial angular velocity is decreasing </a></strong>which requires the planets to decrease their rotation rates, in commensurate with the conservation of angular momentum for the Solar System. The Solar System is a machine which functions under the Second Law of Thermodynamics and entropy increases.</p><p align="left"><br>[<strong>Oh...I should point out that the very last place anyone should obtain so-called "paleo"-magnetic cores is along the Global Fracture System's primary and nth order transform seismic fault zones. Temperatures (i.e. hydrothermal vent complexes, etc.) and "paleo"-magnetic core tectonic displacements are guaranteed to generate extracted core's indigenous magnetic polarity variations, none of which have the slightest connection to the Earth's primary dipole magnetic field. Also water scavenges potassium very nicely from rocks, including ocean bed basalts. Argon is pushed up as a result of mantle pressure into the Earth's crust, both processes adjusting the imagined potassium-argon "clock". &#65533;Radiometric dating belongs with other pseudo-science types...primarily evolutionists...of course.]</strong></p><p align="left"><strong><br></strong><strong><a href="http://creationwiki.org/Radiometric_dating_problems">Potassium-Argon radiometric dating further include problems of branching ratios values which are required for K-40 to decay to Ar-40 and to Ca-40.</a></strong>The branching ratios are adjusted (cheated) to meet one's age requirements. Added to this challenge are the variable nuclear decay rates. <br><br>Finally, alternating geomagnetic field polarity does not increase field<u> <strong><em>intensity</em></strong></u>, as this requires an input energy source into the Earth's geocore's electrical current; in effect increasing the geocore's current density via an increase in this planet's angular velocity.<br><br>The Earth's orbital decay as a function of the <strong><a href="http://en.wikipedia.org/wiki/Kutta–Joukowski_theorem">Kutta-Joukowski Effect </a></strong>applied to planetary orbital physics will be presented in an upcoming paper from BSM Rearch Associates.</p><p><img src="a_21_GMF_a_out_1.jpg"></p><p><img src="a_21_GMF_a_out_2.jpg"></p><p><img src="a_21_GMF_a_out_3.jpg"><br></p><p><a href="a_21_a_12_C.A._Paiva_BSMRA_Javaraiah_Solar_Equatorial_Deceleration.pdf"><strong>a_12_C.A._Paiva_BSMRA_Javaraiah_Solar_Equatorial_Deceleration.pdf</strong></a></p><p><a href="http://smtp.antelecom.net/blogs/bsmaGMF/a_21_a_12_C.A._Paiva_BSMRA_Javaraiah_Solar_Equatorial_Deceleration.pdf"><img src="a_21_Javariah_out_1.jpg"></a></p><p><a href="http://smtp.antelecom.net/blogs/bsmaGMF/a_21_a_12_C.A._Paiva_BSMRA_Javaraiah_Solar_Equatorial_Deceleration.pdf"><img src="a_21_Javariah_out_2.jpg"></a></p><p><strong>Total Solar Radiance Increase (TSI-Solanki)</strong></p><p><a href="a_21_Solar_Irradiance_Since_1874.pdf"><strong>Solar Irradiance Since 1874.pdf</strong></a>
</p><p><strong>Geomagnetic Field (GMF) Pole (CGM/IGRF-11) In Restoration to Geocentric North: <u>Exactly Opposite of Geomagnetic Reversal Models</u>. The GMF Pole should be moving south, NOT back to the north position in alignment with the Earth's North Pole if geomagnetic field reversals were true.  </strong></p><p><img src="a_21_GMF_CGM_out_1.jpg"></p><p><img src="a_21_GMF_CGM_out_2.jpg"></p><p><a href="a_21_Clifford_A._Paiva_Resume__Vita__2010.pdf"><strong>Clifford A. Paiva Resume (Vita) 2010.pdf</strong></a><strong><br></strong></p><p><img src="a_21_Conductivity.jpg"></p><p><img src="a_21_Resistivity.jpg"></p><p><strong>Geomagnetic Field (GMF) Decay Energy Conversion Into Geo-Core Induced Electromagnetic Power; Induced Magnetic Fields (Lenz's Law: Spatial Differential Changing of induced Electric Field Generating Associated Magnetic Field Working Against the Initial GMF Decay).  See GMF Decay and Geo-Core Power Conversion Correlation frames for inclusion of half-life increase for Geo-Core power (heat): 544.74 years.   This means that if the exponential rate of increase of geomagnetic power to electrical power, induced magnetic fields, plus heat remains at the present conversion values, the Earth's core will increase in heat energy by 50% in 544.74 years.</strong></p><p><img src="a_21_Correlation_1.jpg"></p><p><img src="a_21_Correlation_2.jpg"></p><p><strong>Negative Science (Special and General Relativity): Research Revealing the Fallacy of Relativity </strong><strong><br></strong></p><p><a href="a_21_Herbert_Ives_Biography.pdf"><strong>Herbert Ives Biography.pdf</strong></a><strong><br></strong></p><a href="a_21_HerbertIves1937c.pdf"><strong>HerbertIves1937c.pdf</strong></a>
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   		    <p class="post-footer">
      <em> @ 14:40 PM</em>
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		  			<div class="comment-body"><a name=21_1></a>
			  <p><b>Cliff:</b> The correlations are presented for the geomagnetic field decay, the half-life of which is 677 years approximately.  The half-life for the power increase (thermal joule heat generation in the Earth&#39;s core) is 544.74 years.  The is not good news for this planet since the increased heat in the core will diffuse radially outward through the mantle (aesthenosphere), crust (lithosphere); oceans (hydrosphere) and atmosphere.  Further the induced currents generated within the Earth&#39;s core generates associated magnetic fields which work against the initial collapsing primary geomagnetic signal field.  The is process results in a body force, or torque deceleration of the Geo-Core, plus gravitational tidal friction.  This is yet more heat and a further slowing of the Earth&#39;s angular rotational velocity. <small>(08/26/10)</small></p>
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     <h2 class="date-header">Wednesday, 14 April 2010</h2>
      
   <div class="post"><a name=20></a>
    <h3 class="post-title">Global Fracture System: Earthquake Frequency, Intensity;  Correlation to Global Temperature Increase and Solar Storm Increase</h3>
    <div class="post-body">
      <p><P>This section addresses the global distribution of earthquakes in terms of frequency, intensity and spatial distribution since 1900.  Net increases are directly apparent.<BR><IMG src="a_20_Global_EQ_Mag_Increase.jpg">  <A href="a_20_Since_1900_Most_Intense_Earthquake.xls"><STRONG>Since 1900 Most Intense Earthquake.xls</STRONG></A> </P>
<P><IMG src="a_20_Greater_8.jpg"> <A href="a_20_Earthquake_Temporal_Function_1990-2010.xls"><STRONG>Earthquake Temporal Function 1990-2010.xls</STRONG></A> </P>
<P><STRONG>Earthquake Intensity and Frequency Corrleated to Global Temperature and Solar Storm Increase: 11 Year Moving Average</STRONG></P>
<P><STRONG>[Control (+) = Zoom; Control (0) = Normal View]</STRONG></P>
<P><IMG src="a_20_EQ_Frequency_out_1.jpg"></P><P><IMG src="a_20_EQ_Frequency_out_2.jpg"></P><P><IMG src="a_20_EQ_Frequency_out_3.jpg"></P><P><IMG src="a_20_EQ_Frequency_out_4.jpg"> </P></p>
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   		    <p class="post-footer">
      <em> @ 10:45 AM</em>
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		  			<div class="comment-body"><a name=20_1></a>
			  <p><b>Cliff:</b> Correlation is checked for earthquake intensity and frequency increase, to global temperature increase, and solar storm intensity and frequency increase. 11 year moving averages (general solar storm cycle) is applied. <small>(04/19/10)</small></p>
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     <h2 class="date-header">Friday, 25 December 2009</h2>
      
   <div class="post"><a name=18></a>
    <h3 class="post-title">Thomas G. Barnes, BSMRA, and IGRF Data Leading to Half-Life Calculations of the Geomagnetic Field Decay; Dr. Harold S. Slusher; Clifford A. Paiva; International Geomagnetic Reference Field (IGRF) 2010 Geomagnetic Field Intensity Decay</h3>
    <div class="post-body">
      <p><P><STRONG><A href="http://smtp.antelecom.net/blogs/BSMRAMainsite/">BSM Main Site</A></STRONG></P>
<P><STRONG><A href="http://www.google.com/search?q=Clifford+A.+Paiva+BSMRA&amp;hl=en&amp;filter=0">All BSMRA Sites</A></STRONG></P>
<P><STRONG>CONTROL (+) TO ZOOM; CONTROL (0) BACK TO NORMAL</STRONG></P>
<P>Included in this section: <A href="http://www.ngdc.noaa.gov/geomagmodels/IGRFWMM.jsp"><STRONG>International Geomagnetic Reference Field Data (IGRF)</STRONG></A> of the <A href="http://www.ngdc.noaa.gov/geomag/geomag.shtml"><STRONG>National Geophysics and Data Center (NGDC)</STRONG></A>. This is analysis which is ongoing at BSM Research Associates (BSMRA) as we track the decline of the Earth's geomagnetic field and its protective deflective force capability.  The Earth's geomagnetic field (GMF) continues to decay in accordance with the geomagnetic diffusion and intensity decay equations formulated in this section; and commensurate with the reduction of the rotation of the Earth's conductive geo-core through the Sun's interplanetary magnetic field. The 1900-2010 IGRF half-life value (time required for the geomagnetic field to reduce in cosmic ray deflective force by 50%: 684.18 years.<BR><A href="a_18_New_2010_Barnes_Slusher_Paiva_IGRF_Geomagnetic_Field_Intensity_Decay_Values.pdf"><STRONG>New 2010 Barnes Slusher Paiva IGRF Geomagnetic Field Intensity Decay Values.pdf</STRONG></A> </P>
<P><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_18_Conversion_of_Barnes_ESSA_Slusher_Paiva_to_Geomagnetic_IGRF_Model.pdf"><IMG src="a_18_Barnes_ESSA_IRGF_Intensity_Convergence_.jpg"></A> <BR><A href="a_18_Conversion_of_Barnes_ESSA_Slusher_Paiva_to_Geomagnetic_IGRF_Model.pdf"><STRONG>Conversion of Barnes ESSA Slusher Paiva to Geomagnetic IGRF Model.pdf</STRONG></A>  <BR><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_18_Barnes_IGRF_Convergen_t_DataF.xls"><IMG src="a_18_Barnes_Slusher_Paiva_2.jpg"></A> </P>
<P><STRONG>T.G</STRONG>. <A href="a_18_Barnes_IGRF_Convergen_t_DataF.xls"><STRONG>Barnes/ C.A. Paiva_BSMRA:IGRF Convergent DataF.xls</STRONG></A> </P>
<P><A href="http://solarscience.msfc.nasa.gov/greenwch.shtml"><STRONG>http://solarscience.msfc.nasa.gov/greenwch.shtml</STRONG></A></P>
<P><STRONG>Clifford A. Paiva_BSMRA: <A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_18_1882-2007_Global_Temp_Function_of_Earth_Rotation_and_GMF.xls">Earth Temperature Variance Increase As A Function of Planetary Angular Rotation Velocity Decrease: High Correlation</A></STRONG></P>
<P><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_18_1880-2010_MASTER_Global_Temp_Function_of_Earth_Rotation_and_GMF_Decrease.xls"><IMG src="a_18_Earth_Temp_Increase_Function_of_Rotation_Decrease.jpg"></A> <BR><STRONG>Clifford A. Paiva_BSMRA</STRONG>: <A href="a_18_1880-2010_MASTER_Global_Temp_Function_of_Earth_Rotation_and_GMF_Decrease.xls"><STRONG>1880-2010 MASTER Global Temp Function of Earth Rotation and GMF Decrease.xls</STRONG></A> </P>
<P><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_18_Barnes_in_nano_teslas_1.xls"><IMG src="a_18_Barnes_Primary_IGRF_Format_Version_2.jpg"></A></P><P> <A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_18_Barnes_in_nT_B.xls"><IMG src="a_18_Barnes_Primary_IGRF_Format_Version.jpg"></A> </P>
<P><STRONG>T.G</STRONG>.<A href="a_18_Barnes_in_nano_teslas_1.xls"><STRONG>Barnes/C.A. Paiva in nano-teslas.xls</STRONG></A> </P>
<P><A href="a_18_Barnes_in_nT_B.xls"><STRONG>Barnes in nT_B.xls</STRONG></A> </P>
<P><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_18_IGRF_Half_Life_1900_2010.xls"><IMG src="a_18_IGRF_2010_New_REDUCED_GMF_Half_Life_684_Years.jpg"></A></P><P> <A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_18_IGRF_Geomagnetic_Field_Reduced_Half_Life_Values.doc"><IMG src="a_18_IGRF_GMF_Data_File_1900-2010.jpg"></A> <BR><A href="a_18_IGRF_Geomagnetic_Field_Reduced_Half_Life_Values.doc"><STRONG>IGRF Geomagnetic Field Reduced Half Life Values.doc</STRONG></A> </P>
<P><A href="a_18_IGRF_Half_Life_1900_2010.xls"><STRONG>IGRF Half Life 1900 2010.xls</STRONG></A> </P>
<P><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_18_1880-2010_MASTER_Global_Temp_Function_of_Earth_Rotation_and_GMF.xls"><IMG src="a_18_GMF_Function_of_Earth_Temp_Increase.jpg"></A> </P>
<P><A href="a_18_1880-2010_MASTER_Global_Temp_Function_of_Earth_Rotation_and_GMF.xls"><STRONG>1880-2010 MASTER Global Temp Function of Earth Rotation and GMF.xls</STRONG></A> </P>
<P><A href="a_18_MASTER_Earth_Rotation_Excess_Seconds_and_Earth_Temp_2.xls"><STRONG>MASTER Earth Rotation Excess Seconds and Earth Temp_2.xls</STRONG></A> </P>
<P><A href="a_18_Earth_Temperature_Increase_Function_Rotation_Decrease.pdf"><STRONG>Earth Temperature Increase Function Rotation Decrease.pdf</STRONG></A> </P>
<P><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_18_Earth_Temperature_Increase_Function_Rotation_Decrease.pdf"><IMG src="a_18_Earth_Temp_and_Period_Function_Year.jpg"></A> <BR><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_18_Earth_Temperature_Increase_Function_Rotation_Decrease.pdf"><IMG src="a_18_Earth_Temp_Increase_and_Rot_Decrease.jpg"></A> </P>
<P><A href="a_18_Earth_Rotation_Excess_Seconds.xls"><STRONG>Earth Rotation Excess Seconds.xls</STRONG></A> </P>
<P><A href="a_18_Excess_Seconds_Function_of_Rot_and_Temp.xls"><STRONG>Excess Seconds Function of Rot and Temp.xls</STRONG></A> </P>
<P><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_18_Earth_Rotation_Excess_Seconds.xls"><IMG src="a_18_Earth_Period__Increase_Function_of_Time.jpg"></A></P><P> <A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_18_Excess_Seconds_Function_of_Rot_and_Temp.xls"><IMG src="a_18_Earth_Period_and_SS_Increase_Function_of_Time.jpg"></A></P><P><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_18_1835-2010__GMF_Function_Rotation.xls"><IMG src="a_18_Solar_Cycle_24.jpg"></A> </P>
<P><A href="a_18_1835-2010__GMF_Function_Rotation.xls"><STRONG>1835-2010 GMF Function Rotation.xls</STRONG></A> </P>
<P><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_18_Earth_s_Angular_Velocity_Decrease.pdf"><IMG src="a_18_GME_Induction_Intensity_and_Planetary_Rotation.jpg"></A> </P>
<P><A href="a_18_Earth_s_Angular_Velocity_Decrease.pdf"><STRONG>Earth's Angular Velocity Decrease.pdf</STRONG></A> </P>
<P><STRONG><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_18_GeoCore_Conductivity.xls">Clifford A. Paiva_BSMR: Geomagnetic Field Half-Life Decrease</A></STRONG></P>
<P><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_18_GeoCore_Conductivity.xls"><IMG src="a_18_GMF_Half-Life.jpg"></A> </P>
<P><STRONG>CONTROL (+) FOR ZOOM; CONTROL (0) FOR ZOOM OUT</STRONG></P>
<P><A href="a_18_GeoCore_Conductivity.xls"><STRONG>GeoCore Conductivity.xls</STRONG></A> <BR><A href="a_18_IGRF_GeoCore_Conductivity_Power.xls"><STRONG>IGRF GeoCore Conductivity Power.xls</STRONG></A> <BR><IMG src="a_18_GeoCore_Electrical_Energy.jpg"> </P>
<P><STRONG>GeoCore Future Projections: Electrical Energy Decrease (joules)</STRONG> </P>
<P><IMG src="a_18_Projected_Drop.jpg"> <A href="a_18_BMSRA_Projected_GeoCore_Conductivity_Power.xls"><STRONG>BMSRA Projected GeoCore Conductivity Power.xls</STRONG></A> </P>
<P><A href="a_18_Correlation_Check_Earthquake_to_Global_Warming.xls"><STRONG>Correlation Check Earthquake to Global Warming.xls</STRONG></A> </P>
<P><IMG src="a_18_Best_out_1.jpg"> </P></p>
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      <em> @ 10:18 AM</em>
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			  <p><b>Cliff:</b> As the earth&#39;s electrically conductive geocore&#39;s angular velocity decreases (spinning through the sun&#39;s interplanetary magnetic field), the induced geomagnetic field commensurately decreases; as the graph indicates. <small>(02/15/10)</small></p>
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		  			<div class="comment-body"><a name=18_5></a>
			  <p><b>Cliff:</b> The GeoCore projections are from the solution of the Clerk-Maxwell field equation, in particular the diffusion form of Curl Curl B =Curl J (current density). <small>(04/13/10)</small></p>
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     <h2 class="date-header">Friday, 18 December 2009</h2>
      
   <div class="post"><a name=17></a>
    <h3 class="post-title">Clifford A. Paiva_BSMRA: Global Warming on Mars</h3>
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      <p><BR><A href="http://news.nationalgeographic.com/news/2007/02/070228-mars-warming_2.html"><IMG src="a_17_Mars_Polar_Cap.jpg"></A> <BR><A href="a_17_Clifford_Paiva_BSMRA_Global_Warming_on_Mars.pdf"><STRONG>Clifford Paiva_BSMRA Global Warming on Mars.pdf</STRONG></A> </p>
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      <em> @ 08:50 AM</em>
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     <h2 class="date-header">Tuesday, 08 December 2009</h2>
      
   <div class="post"><a name=16></a>
    <h3 class="post-title">Clifford A. Paiva BSMRA: Dr Thomas G. Barnes and Dr. Harold S. Slusher: Geomagnetic Field Decay and Ramifications of Earth's GeoCore and Biosphere</h3>
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      <p><P>The decay of the <A href="http://www.ngdc.noaa.gov/IAGA/vmod/igrf.html"><STRONG>Earth's geomagnetic field</STRONG> </A>is exceedingly dangerous to this planet as it exposes the planet's biosphere to high energy, charged particle (protons and electrons) penetrations.&nbsp; The geocore's joule heating flux increases as the geomagnetic field decays.&nbsp; The field itself is induced by circulating currents generated from the geocore's rotation through the Sun's interplanetary stellar magnetic field (<A href="http://en.wikipedia.org/wiki/Michael_Faraday"><STRONG>Faraday Effect</STRONG></A>).&nbsp; As the sun slows in its rotation the <A href="http://smtp.antelecom.net/blogs/bsmaGMF/item_2.htm"><STRONG>Earth's induced geomagnetic field decays</STRONG></A>. The changing (decreasing) geomagnetic field induces a <A href="http://en.wikipedia.org/wiki/Lenz's_law"><STRONG>Lenz current</STRONG> </A>in the opposite direction which further slows (through a geocore <STRONG>Stress Force =</STRONG>&nbsp;<STRONG>J</STRONG>x<STRONG>B, <A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_15_Clifford_Anthony_Paiva_BSMRA_Geomagnetic_Field_Mathematics.doc">see electromagnetic&nbsp;physics&nbsp;included</A>).&nbsp; Values are determined by the <A href="http://www.ngdc.noaa.gov/geomagmodels/IGRFWMM.jsp">International Geomagnetic Reference Field (IGRF) of the International Union of Geodesy and Geophysics&nbsp; (IUGG)</A></STRONG><BR><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_16_2010_International_Geomagnetic_Reference_Field_Decay_Data.pdf"><STRONG>Clifford A. Paiva_BSMRA</STRONG></A><STRONG>:</STRONG> <A href="http://www.ngdc.noaa.gov/geomagmodels/IGRFWMM.jsp"><STRONG>New International Geomagnetic Reference Field (IGRF)</STRONG></A></P>
<P><A href="https://smtp.antelecom.net/cgi/a_16_2010_International_Geomagnetic_Reference_Field_Decay_Data.pdf"><STRONG>2010 International Geomagnetic Reference Field Decay Data.pdf</STRONG></A> </P>
<P><STRONG>Clifford A. Paiva_BSMRA:</STRONG><A href="http://smtp.antelecom.net/blogs/BSMRAMainsite/a_1_Global_Earthquake_Intensity_Increase_1990-2010.pdf"><STRONG>Global Earthquake Intensity Increase 1990-2010.pdf</STRONG></A>&nbsp;&nbsp;<BR><STRONG>Clifford A. Paiva_BSMRA:</STRONG><A href="https://smtp.antelecom.net/cgi/a_16_Earthquake_Temporal_Function_1990-2010.xls"><STRONG>Earthquake Temporal Function 1990-2010.xls</STRONG></A> </P>
<P><STRONG><A href="http://www.foxnews.com/story/0,2933,468268,00.html">Clifford A. Paiva_BSMRA: Perforations (Rupture) in the Disintegrating Geomagnetic Field (GMF)</A></STRONG></P>
<P><IMG src="a_16_Rupture_of_GMF_IPM_alignement_2.jpg"> </P>
<P><STRONG><A href="http://www.google.com/search?q=Clifford+A.+Paiva+BSMRA&amp;hl=en&amp;filter=0">All BSMRA Sites</A></STRONG></P></p>
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      <em> @ 08:21 AM</em>
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			  <p><b>Cliff:</b> The new values for the IGRF (International Geomagnetic Reference Field) has been added. The current value continues the decrease. <small>(12/23/09)</small></p>
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     <h2 class="date-header">Thursday, 03 September 2009</h2>
      
   <div class="post"><a name=15></a>
    <h3 class="post-title">Clifford Anthony Paiva_BSMRA_Paleomagnetism  Requirements: Unsubstantied Assumptions Under the Guise of "Science"</h3>
    <div class="post-body">
      <p><P><STRONG><A href="http://smtp.antelecom.net/blogs/BSMRAMainsite/">Back to BSMRA Main Site</A></STRONG></P>
<P><STRONG><A href="http://www.google.com/search?q=Clifford+A.+Paiva+BSMRA&amp;hl=en&amp;filter=0">All BSMRA Sites</A></STRONG></P>
<P>Note that usage of so-called <EM>paleo</EM>magnetic extracted cores require&nbsp;for<STRONG>&nbsp;</STRONG><A href="http://smtp.antelecom.net/blogs/bsmaastrophysics/a_11_H.S._Slusher_Radiometric_Dating_p_26_thru_40_out.PDF"><STRONG>potassium-argon radiometric dating</STRONG>:</A> &nbsp;[<STRONG>Ar-40</STRONG> (argon final)] = [<STRONG>K-40 </STRONG>(potassium initial)][(<A href="http://www.halos.com/"><STRONG>Transmutation Rate</STRONG></A>)][(time]):</P>
<P><STRONG>a</STRONG>. <STRONG><U>Critical:</U></STRONG> applications of <A href="http://smtp.antelecom.net/blogs/bsmaastrophysics/a_11_Dr._H.S._Slusher_Critique_of_Radiometric_Dating__p._1-26.PDF">radiometric dating<STRONG><EM> <U>assumptions</U></EM></STRONG> </A>for age determination; <A href="http://www.halos.com/"><EM><U><STRONG>transmutation rates must be constant</STRONG></U></EM>;</A> in fact the initial <STRONG>potassium (K-40) </STRONG>is <EM><U><STRONG>not known</STRONG></U></EM>, the transmutation of disintegration of<STRONG> potassium K-40</STRONG> into <STRONG>argon</STRONG> <STRONG>Ar-40</STRONG> is also <U><STRONG>NOT</STRONG></U> constant. Futher the generation of <STRONG>argon</STRONG> <STRONG>Ar-40</STRONG> independent of <STRONG>potassium K-40</STRONG> <STRONG><EM><U>does</U></EM></STRONG> occur. Unfortunately for paleomagnetism enthusiasts, <STRONG>K-40</STRONG> to <STRONG>Ar-40</STRONG> is used <STRONG><U>extensively</U></STRONG> in attempted dating of assumed <EM>paleo-</EM>magnetic core extractions along the <STRONG>Mid-Atlantic Ridge</STRONG> [part of the <STRONG>Global Fracture System (GFS)</STRONG>];</P>
<P><STRONG>b</STRONG>. <STRONG><U>Critical:</U></STRONG> core specimens&nbsp;temperatures must not&nbsp;rise above&nbsp;the curie temperature, otherwise a GMF re-alignment in the rock will occur after re-lithification, resulting in the destruction of the <EM><U>initial</U></EM> <STRONG>natural remanent GMF magnetization (NRM)</STRONG> and original primary GMF direction;&nbsp;futher resulting in a "new" <STRONG>NRM</STRONG>.&nbsp;&nbsp;In otherwords no volcanic <EM>thermal </EM>activity along the Global Fracture Zone (GFS) areas where the cores are extracted may be permitted.&nbsp; <STRONG><U>This problem alone eliminates the use of <EM>paleo</EM>magnetic data.</U></STRONG></P>
<P><STRONG>c</STRONG>. <STRONG><U>Critical:</U></STRONG> core extraction immediate region must be geophysically (seismically) stable over time; in otherwords no&nbsp;<STRONG>SEISMIC</STRONG> activity along the GFS areas where the cores are extracted&nbsp;may be permitted. <STRONG><U>This is another problem which eliminates the use of the <EM>paleo</EM>magnetic paradigm</U></STRONG>.</P>
<P><STRONG>d</STRONG>. <STRONG><U>Critical:</U></STRONG> <STRONG>natural </STRONG>geomagnetic <STRONG>remanent magnetization (NRM)</STRONG> must have been acquired aligned <STRONG><EM><U>parallel</U></EM></STRONG> to the <STRONG><EM><U>initial </U></EM></STRONG>primary GMF, otherwise incorrect geomagnetic field directions intrinsic to the extracted cores exist. This cannot be assured.</P>
<P><STRONG>e</STRONG>. <STRONG><U>Critical: </U></STRONG>Time of <EM><U><STRONG>initial</STRONG></U></EM> and <STRONG><EM><U>properly aligned</U></EM></STRONG> natural remanent magnetization must be obtained; the use of potassium-agron (or any other radiometric dating method)&nbsp;destroys this critical requirement.</P>
<P><STRONG><U>NOTE</U></STRONG>: <STRONG>BSM Research</STRONG> <STRONG>Associates (BSMRA) </STRONG>completely endorses <STRONG>Dr. Harold S. Slusher's</STRONG> (University of Texas at El Paso, Physics Department)&nbsp;<STRONG><EM>Critique of Radiometric Dating Methods</EM></STRONG> published in 1970 which addresses all of the above critial paleomagnetic issues; copies&nbsp;of which are in residence here&nbsp;(<STRONG><A href="http://smtp.antelecom.net/blogs/bsmasolar/a_2_HTV_Greenhouse_Gases.pdf">BSMRA</A></STRONG>) &nbsp;if folks are interested.&nbsp;This is an excellent small text for the general reading public and addresses the very significant problems of radiometridc dating assumptions. If you are interested please call [(760)&nbsp;373-1518 or (661) 373-1518], or use this site's comment-email. [Futher Data see <STRONG><EM><A href="http://www.icr.org/article/438/">Snelling</A></EM></STRONG> or <A href="http://www.detectingdesign.com/carbon14.html#Difficult"><STRONG>http://www.detectingdesign.com/carbon14.html#Difficult</STRONG></A><STRONG>; </STRONG><A href="http://www.detectingdesign.com/carbon14.html#Problems"><STRONG>http://www.detectingdesign.com/carbon14.html#Problems</STRONG></A><STRONG>; </STRONG><A href="http://www.icr.org/article/438/"><STRONG>http://www.icr.org/article/438/</STRONG></A><STRONG>; </STRONG><A href="http://www.answersingenesis.org/articles/am/v1/n1/radioactive-http://www.angelfire.com/mi/dinosaurs/carbondating.htmldating"><STRONG>http://www.answersingenesis.org/articles/am/v1/n1/radioactive-http://www.angelfire.com/mi/dinosaurs/carbondating.htmldating</STRONG></A><STRONG>; </STRONG><A href="a_15_Paleomagnetism_Assumption_Restriction.doc"><STRONG>Paleomagnetism Assumption Restriction.doc</STRONG></A><STRONG>]</STRONG><BR><A href="http://www.halos.com/"><IMG src="a_15_Matsushita_and_Campbell_out_1a.jpg"></A>&nbsp;<BR><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_15_BSMRA-HTV_Greenhouse_Gases.pdf"><IMG src="a_15_Matsushita_and_Campbell_out_2.jpg"></A>&nbsp;<BR><A href="http://smtp.antelecom.net/blogs/bsmasolar/a_2_HTV_Greenhouse_Gases.pdf"><IMG src="a_15_Noname.jpg"></A> <BR><A href="http://www.halos.com/reports/ex-nihilo-1998-fingerprints-of-creation.htm"><IMG src="a_15_Noname2.jpg"></A> <BR><A href="http://www.halos.com/reports/ex-nihilo-1998-fingerprints-of-creation.htm"><IMG src="a_15_Noname3.jpg"></A>&nbsp;<BR><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_15_Cliff_PRIMARY_Prime_Military__RESUME__2009.doc"><STRONG>BSMRA</STRONG></A><STRONG>_</STRONG><A href="a_15_Cliff_PRIMARY_Prime_Military__RESUME__2009.doc"><STRONG>Clifford Anthony Paiva Military RESUME 2009.doc</STRONG></A><STRONG> </STRONG></P>
<P><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_2_TSI_INCREASE_26_September_1991000.pdf"><IMG src="a_15_Fracture_Zone.jpg"></A> <BR><STRONG>C.A.Paiva_</STRONG><A href="http://smtp.antelecom.net/blogs/bsmasolar/a_2_HTV_Greenhouse_Gases.pdf"><STRONG>BSMRA-Hydrothermal (HTV)&nbsp;Complexes&nbsp;Greenhouse Gases.pdf</STRONG></A> <BR><STRONG>C.A. Paiva_</STRONG><A href="a_15_BSMRA_Where_Not_To_Drill_Is_Precisely_Where_They_Do.doc"><STRONG>BSMRA_Where_Not_To_Drill_Is_Precisely_Where_They_Do.doc</STRONG></A> </P>
<P><STRONG>C.A. Paiva_<A href="http://smtp.antelecom.net/blogs/bsmasolar/a_8_Solar_Rotation_Decrease_From_1956_up_to_present.doc">BSMRA Earth Rotation Decrease</A></STRONG></P>
<P><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_15_Clifford_Anthony_Paiva_BSMRA_Geomagnetic_Field_Mathematics.doc"><STRONG>Clifford Anthony Paiva_BSMRA_Geomagnetic Field Mathematics.doc</STRONG></A> </P></p>
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      <em> @ 12:54 PM</em>
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			  <p><b>Cliff:</b> Hydrothermal vent zones are positioned along the primary fracture and along transform fault zones.  Of course the worse area for selection of deep-sea core drilling for paleomagnetic specimens would be those areas of seismic and thermal instabilities...in other words...the Global Fracture System (GFS) and its transform fault zones. <small>(09/03/09)</small></p>
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     <h2 class="date-header">Monday, 27 July 2009</h2>
      
   <div class="post"><a name=14></a>
    <h3 class="post-title">Clifford Anthony Paiva_BSMRA_Correlation of Apparent Temperature Decrease With Historical Solar Storm Frequency; Solar Equatorial Deceleration; Canadian Geophysicist Ken Allen Research; Water Vapor Absorption Increasing As H2Ov Concentration Increases</h3>
    <div class="post-body">
      <p><p><a href="http://smtp.antelecom.net/blogs/bsmaGMF/a_14_BSMRA_Paiva_and_Increased_solar_brightness_and_warming_of_the_Earth_since_1979.doc"><strong>Back to BSMRA Main Site</strong></a></p>
<p><a href="http://www.geocraft.com/WVFossils/greenhouse_data.html"><strong>Solar storm (solar storm) frequency</strong> </a>decreases during 2000-2009 correlate well to historical solar storm activity and the <a href="http://physicsworld.com/cws/article/print/17402"><strong>increase of H2O vapor global concentrations for the Earth</strong></a>.  Increases in solar storms should commence in 2010.  The <a href="http://www.tmgnow.com/repository/solar/lassen1.html"><strong>net solar storm</strong> <strong>and earth temperature increases</strong> </a>remain very highly correlated, especially when comparing <a href="http://smtp.antelecom.net/blogs/bsmaGMF/a_14_Friis_Christensen_Primary_Paper.pdf"><strong>Friis Christensen</strong></a>; Javarriah, Hanssen, Solanki and Lassen solar physics data. As the Sun (and Earth's) angular velocities decrease, solar storm activity increase (see Javarriah: <em><strong>Long Term Variations in Solar Differential Rotation and Sunspot Activity</strong></em>; University of California Post Prints).<br><a href="http://www.geocraft.com/WVFossils/greenhouse_data.html"><img src="a_14_Solar_Storm_Low_Activity.jpg"></a> <a href="http://www.tmgnow.com/repository/solar/lassen1.html"><img src="a_14_Solar_Storm_Low_Activity2.jpg"></a> <a href="http://www.geocraft.com/WVFossils/greenhouse_data.html"><img src="a_14_Angular_Vel_decrease_1.jpg"></a> <a href="http://www.tmgnow.com/repository/solar/lassen1.html"><img src="a_14_Angular_Vel_decrease_2.jpg"></a> <br><strong>C.A. Paiva_</strong><a href="http://smtp.antelecom.net/blogs/bsmaGMF/a_14_Correlation_of_Apparent_Temperature_Decrease_With_Historical_Solar_Storm_Frequency.doc"><strong>BSMRA_Correlation of Apparent Temperature Decrease With Historical Solar Storm Frequency.doc</strong></a><strong> <br></strong><a href="http://www.geocraft.com/WVFossils/greenhouse_data.html"><img src="a_14_Percent_Change_TSI.jpg"></a> <a href="http://smtp.antelecom.net/blogs/bsmaGMF/a_15_BSMRA-HTV_Greenhouse_Gases.pdf"><img src="a_14_Percent_Change_TSI_Mars.jpg"></a> <br><strong>C.A. Paiva_<a href="http://smtp.antelecom.net/blogs/bsmaGMF/a_14_Global_Temperature_Net_Increase_as_a_Function_of_Solar_Rotation_Decrease_and_Storm_Activity.doc">BSMRA</a>_</strong><a href="a_14_Global_Temperature_Net_Increase_as_a_Function_of_Solar_Rotation_Decrease_and_Storm_Activity.doc"><strong>Global Temperature Net Increase as a Function of Solar Rotation Decrease and Storm Activity.doc</strong></a><strong> <br>C.A. Paiva_<a href="http://smtp.antelecom.net/blogs/bsmaGMF/a_14_Global_Heating_Allen_A.pdf">BSMRA_</a></strong><strong><a href="http://smtp.antelecom.net/blogs/bsmaGMF/a_14_Global_Heating_Allen_A.pdf">Global Heating Allen A.pdf</a></strong> <br><strong>C.A. Paiva_<a href="http://smtp.antelecom.net/blogs/bsmaGMF/a_14_Ken_Allen_Geophysicist_Canadian_Geological_Survey.pdf">BSMRA</a>_</strong><a href="a_14_Ken_Allen_Geophysicist_Canadian_Geological_Survey.pdf"><strong>Ken Allen Geophysicist Canadian Geological Survey.pdf</strong></a> <br><strong>C.A. Paiva_<a href="http://smtp.antelecom.net/blogs/bsmaGMF/a_14_Global_Heating_Ken_Allen_B.pdf">BSMRA</a>_</strong><a href="a_14_Global_Heating_Ken_Allen_B.pdf"><strong>Global Heating Ken Allen B.pdf</strong></a><strong> </strong><br><strong>C.A. Paiva_<a href="http://smtp.antelecom.net/blogs/bsmaGMF/a_14_Triton_Heating_Up.pdf">BSMRA</a>_</strong><a href="a_14_Triton_Heating_Up.pdf"><strong>Triton Heating Up.pdf</strong></a><strong> <br>C.A. Paiva_<a href="http://smtp.antelecom.net/blogs/bsmaGMF/a_14_Global_Warming_on_Pluto_Puzzles_Scientists.pdf">BSMRA_</a></strong><strong><a href="http://smtp.antelecom.net/blogs/bsmaGMF/a_14_Global_Warming_on_Pluto_Puzzles_Scientists.pdf">Global Warming on Pluto Puzzles Scientists.pdf</a></strong> <br><a href="http://www.tmgnow.com/repository/solar/lassen1.html"><img src="a_14_GMF_and_Earth_Rotation_Rate_Correlation.jpg"></a> <br><strong>C.A. Paiva_</strong><a href="http://smtp.antelecom.net/blogs/bsmaGMF/a_14_Earth_Rotation__Temperature_and_Geomagnetic_Field_Correlation.doc"><strong>BSMRA</strong></a><strong>_</strong><a href="a_14_Earth_Rotation__Temperature_and_Geomagnetic_Field_Correlation.doc"><strong>Earth Rotation, Temperature and Geomagnetic Field Correlation.doc</strong></a> <br><strong>C.A. Paiva_</strong><a href="http://smtp.antelecom.net/blogs/bsmaGMF/a_14_Solar_UV_Radiance_Increases_and_Earth_Temperatures.doc"><strong>BSMRA_Solar UV Radiance Increases and Earth Temperatures.doc</strong></a> </p>
<p><a href="http://www.tmgnow.com/repository/solar/lassen1.html"><img src="a_14_North_Pole_Melting.jpg"></a></p><p> <a href="http://www.geocraft.com/WVFossils/greenhouse_data.html"><img src="a_14_North_Pole_Melting2.jpg"></a> <br><strong>C.A. Paiva_</strong><a href="http://smtp.antelecom.net/blogs/bsmaGMF/a_14_Cowling_s_Theorem.doc"><strong>BSMRA_Cowling's Theorem.doc</strong></a><strong> <br><a href="http://smtp.antelecom.net/blogs/bsmaGMF/a_14_Friis_Christensen_Primary_Paper.pdf">C.A. Paiva_</a></strong><strong><a href="http://smtp.antelecom.net/blogs/bsmaGMF/a_14_Friis_Christensen_Primary_Paper.pdf">BSMRA_Friis Christian Solar Activity and Climate.doc</a></strong><strong> <br><a href="http://smtp.antelecom.net/blogs/bsmaGMF/a_14_Friis_Christensen_Primary_Paper.pdf">C.A. Paiva_</a></strong><strong><a href="http://smtp.antelecom.net/blogs/bsmaGMF/a_14_Friis_Christensen_Primary_Paper.pdf">BSMRA_Friis Christensen Primary Paper.pdf</a></strong><strong> <br></strong><a href="http://smtp.antelecom.net/blogs/bsmaGMF/a_14_Hansen_Solar_Storm_Correlations_2.pdf"><strong>BSMRA</strong></a><strong>_</strong><a href="a_14_Hansen_Solar_Storm_Correlations_2.pdf"><strong>Hansen Solar Storm Correlations 2.pdf</strong></a> </p>
<p><a href="http://smtp.antelecom.net/blogs/bsmaGMF/a_14_Clifford_A._Paiva_Global_Warming_Due_to_Water_Vapor_H20v_NOT_Carbon_Dioxide_CO2.pdf"><img src="a_14_H2Ovapor_out_1.jpg"></a></p><p> <a href="http://smtp.antelecom.net/blogs/bsmaGMF/a_2_TSI_INCREASE_26_September_1991000.pdf"><img src="a_14_H2Ovapor_out_2.jpg"></a></p><p><a href="http://images.google.com/imgres?imgurl=http://wattsupwiththat.files.wordpress.com/2008/03/essifigure1.png&amp;imgrefurl=http://wattsupwiththat.com/2008/03/30/evidence-of-a-significant-solar-imprint-in-annual-globally-averaged-temperature-trends-part-2/&amp;usg=__1do43YCal46y-ZhFyszY9cL-PHI=&amp;h=530&amp;w=640&amp;sz=60&amp;hl=en&amp;start=2&amp;tbnid=hE2OFosI9gB2UM:&amp;tbnh=113&amp;tbnw=137&amp;prev=/images%3Fq%3Dearth%2Bdeceleraton%2Bjavariah%26gbv%3D2%26hl%3Den%26client%3Dfirefox-a%26rls%3Dorg.mozilla:en-US:official"><img src="a_14_H2Ovapor_out_3.jpg"></a></p><p><a href="http://smtp.antelecom.net/blogs/bsmaGMF/a_14_Clifford_A._Paiva_Global_Warming_Due_to_Water_Vapor_H20v_NOT_Carbon_Dioxide_CO2.pdf"><img src="a_14_H2O_vapor_out_1.jpg"></a></p><p><a href="http://smtp.antelecom.net/blogs/bsmaGMF/a_14_Clifford_A._Paiva_Global_Warming_Due_to_Water_Vapor_H20v_NOT_Carbon_Dioxide_CO2.pdf"><img src="a_14_H2O_vapor_out_2.jpg"></a> </p>
<p><strong><a href="http://smtp.antelecom.net/blogs/bsmaGMF/a_14_The_Climatic_Effects_of_Water_Vapour_complete.doc">BSMRA</a>_</strong><a href="a_14_The_Climatic_Effects_of_Water_Vapour_complete.doc"><strong>The Climatic Effects of Water Vapour_complete.doc</strong></a><strong> <br><a href="http://smtp.antelecom.net/blogs/bsmaGMF/a_14_The_Greenhouse__Effects_of_Water_Vapor_Versus_Carbon_Dioxide.doc">BSMRA</a>_</strong><a href="a_14_The_Greenhouse__Effects_of_Water_Vapor_Versus_Carbon_Dioxide.doc"><strong>The Greenhouse Effects of Water Vapor Versus Carbon Dioxide.doc</strong></a><strong> </strong></p>
<p><strong><a href="http://smtp.antelecom.net/blogs/bsmaGMF/a_14_BSMRA_Paiva_and_Increased_solar_brightness_and_warming_of_the_Earth_since_1979.doc">BSMRA</a>_</strong><a href="a_14_BSMRA_Paiva_and_Increased_solar_brightness_and_warming_of_the_Earth_since_1979.doc"><strong>BSMRA Paiva and Increased solar brightness and warming_of_the_Earth_since_1979.doc</strong></a> </p>
<p><strong><a href="http://smtp.antelecom.net/blogs/bsmasolar/a_8_Solar_Rotation_Decrease_From_1956_up_to_present.doc">BSMRA Earth Angular Velocity Decrease Data</a></strong></p>
<p><a href="http://smtp.antelecom.net/blogs/bsmaGMF/a_14_Friis_Christensen_Primary_Paper.pdf"><strong>Clifford Anthony Paiva_BSMRA_</strong><strong>Friis Christensen Primary Paper.pdf</strong></a><strong> </strong></p>
<p><a href="http://smtp.antelecom.net/blogs/bsmaGMF/a_15_Clifford_Anthony_Paiva_BSMRA_Geomagnetic_Field_Mathematics.doc"><strong>Clifford Anthony Paiva_BSMRA_Geomagnetic Field Mathematics.doc</strong></a><strong> </strong></p><p><a href="http://smtp.antelecom.net/blogs/bsmaGMF/a_14_Clifford_A._Paiva_Global_Warming_Due_to_Water_Vapor_H20v_NOT_Carbon_Dioxide_CO2.pdf"><strong>Clifford A. Paiva Global Warming Due to Water Vapor H20v NOT Carbon Dioxide CO2.pdf</strong></a><strong> </strong></p><p><strong><br></strong></p><br><a href="a_14_Clifford_A._Paiva_Resume__Vita__2010.pdf">Clifford A. Paiva Resume (Vita) 2010.pdf</a>
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      <em> @ 12:00 PM</em>
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			  <p><b>Cliff:</b> This section delineates the reduction in angular velocities for the Sun, Earth and Solar System planets, with resultant increases in temperature for the system. Increases in total solar irradiance, particularly in the .1-.2 micron bandpass (UV) from the Virgo satellite is presented and stated as most dangerous to biologic systems.  Anthropogenic global warming effects cannot be a significant contributor since such effects are measured for Mars and Jupiter (moons). <small>(08/01/09)</small></p>
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     <h2 class="date-header">Saturday, 04 October 2008</h2>
      
   <div class="post"><a name=12></a>
    <h3 class="post-title">Clifford Anthony Paiva_BSMRA_Earth Rotation Decrease Results In Decreases In GeoCore Induced Currents and Decreases in Joule Heating for the Trough Regions</h3>
    <div class="post-body">
      <p><P><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_12_Methane_Ocean_Floor.pdf"><IMG src="a_12_Global_Temp_As_Function_of_ERS_Deceleration_Moving_Average_OUT_2.jpg"></A> <BR><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_15_BSMRA-HTV_Greenhouse_Gases.pdf"><IMG src="a_12_Global_Temp_As_Function_of_ERS_Deceleration_Polytrends_OUT.jpg"></A>&nbsp;</P>
<P><A href="http://smtp.antelecom.net/blogs/BSMRAMainsite/"><STRONG>Back to BSMRA Main Site</STRONG></A></P>
<P><STRONG><A href="http://www.google.com/search?q=Clifford+A.+Paiva+BSMRA&amp;hl=en&amp;filter=0">[All BSMRA Sites]</A></STRONG></P>
<P><STRONG>C.A. Paiva_BSMRA_</STRONG><A href="a_12_International_Earth_Rotation_Reference_System_Service__IERS_.doc"><STRONG>International Earth Rotation Reference System Service (IERS).doc</STRONG></A><STRONG> <BR>C.A. Paiva_</STRONG><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_12_Solar_Wind_and_Length_of_Day.PDF"><STRONG>BSMRA</STRONG></A>_<A href="a_12_Solar_Wind_and_Length_of_Day.PDF"><STRONG>Solar Wind and Length of Day.PDF</STRONG></A><STRONG> <BR></STRONG><BR><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_15_BSMRA-HTV_Greenhouse_Gases.pdf"><IMG src="a_12_Earth_Rotation_Decrease_1.jpg"></A> <BR><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_15_BSMRA-HTV_Greenhouse_Gases.pdf"><IMG src="a_12_Earth_Rotation_Decrease_2.jpg"></A> <BR><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_2_TSI_INCREASE_26_September_1991000.pdf"><IMG src="a_12_Rotation_Decrease_1.jpg"></A> <BR><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_12_Sun_and_Earth_Coupled_Decreases_in_Angular_Rotation.PDF"><STRONG>BSMRA</STRONG>_<STRONG>Sun and Earth Coupled Decreases in Angular Rotation.PDF</STRONG></A> <BR><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_15_BSMRA-HTV_Greenhouse_Gases.pdf"><IMG src="a_12_Rotation_GMF_out_1.jpg"></A> <BR><A href="http://smtp.antelecom.net/blogs/bsmasolar/a_2_HTV_Greenhouse_Gases.pdf"><IMG src="a_12_Rotation_GMF_out_2.jpg"></A> <BR><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_2_TSI_INCREASE_26_September_1991000.pdf"><IMG src="a_12_GMF_out_3.jpg"></A> <BR><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_12_Geomagnetic_Field_and_Earth_Conducting_Core_Rotation_Through_Solar_Magnetic_Field.PDF"><STRONG>BSMRA_Geomagnetic Field and Earth Conducting Core Rotation Through Solar Magnetic Field.PDF</STRONG></A><STRONG> <BR><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_12_Why_Geocore_Dynamos_Do_Not_Work__Resistance_And_Coriolis_Effects.pdf">BSMRA</A></STRONG>_<A href="a_12_Why_Geocore_Dynamos_Do_Not_Work__Resistance_And_Coriolis_Effects.pdf"><STRONG>Why Geocore Dynamos Do Not Work; Resistance And Coriolis Effects.pdf</STRONG></A> <BR><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_12_Methane_Ocean_Floor.pdf"><IMG src="a_12_Geomagnetic_Field_Symmetry.jpg"></A>&nbsp;<STRONG><BR><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_12_Geomagnetic_Diffusion.PDF">BSMAR</A>_</STRONG><A href="a_12_Geomagnetic_Diffusion.PDF"><STRONG>Geomagnetic Diffusion.PDF</STRONG></A><STRONG> <BR><A href="http://smtp.antelecom.net/blogs/bsmasolar/a_2_HTV_Greenhouse_Gases.pdf">BSMRA</A>_</STRONG><STRONG><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_12_Methane_Ocean_Floor.pdf">Methane Ocean Floor.pdf</A></STRONG><STRONG> <BR></STRONG><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_12_Methane_Ocean_Floor.pdf"><IMG src="a_12_GMF_Decrease_out_3.jpg"></A>&nbsp;</P>
<P><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_15_Clifford_Anthony_Paiva_BSMRA_Geomagnetic_Field_Mathematics.doc"><STRONG>Clifford Anthony Paiva_BSMRA_Geomagnetic Field Mathematics.doc</STRONG></A> </P>
<P><A href="http://smtp.antelecom.net/blogs/bsmasolar/"><IMG src="a_12_GMF_Earth_Rotation.jpg"></A> </P>
<P><STRONG>Geomagnetic Field Decay Half-Life</STRONG></P>
<P><IMG src="a_12_GMF_Half-Life.jpg"> </P></p>
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   		    <p class="post-footer">
      <em> @ 15:22 PM</em>
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			  <p><b>Cliff:</b> As stated earlier just use the PDF and WORD formats for higher resolution...thanks. <small>(10/19/08)</small></p>
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     <h2 class="date-header">Monday, 01 September 2008</h2>
      
   <div class="post"><a name=10></a>
    <h3 class="post-title">Clifford Anthony Paiva_BSMRA_Arctic, Northwest Passage and Northern Route Temperature Increases</h3>
    <div class="post-body">
      <p><P><A href="http://smtp.antelecom.net/blogs/BSMRAMainsite/"><STRONG>Back to BSMRA Main Site</STRONG></A></P>
<P><STRONG><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_10_HIRES_Antarctic_Larsen_Shelf_Melt__Suface_and_Submerged_Fractures.PDF">BSMRA</A>_</STRONG><A href="http://www.membrane.com/global_warming/notes/melting_at_both_ends.html"><STRONG>HIRES Antarctic Larsen Shelf Melt; Suface and Submerged Fractures.PDF</STRONG></A> <BR><A href="http://www.membrane.com/global_warming/notes/melting_at_both_ends.html"><IMG src="a_10_2007_Polar_Ice_Cap_out_1.jpg"></A> </P>
<P><A href="http://www.membrane.com/global_warming/notes/melting_at_both_ends.html"><STRONG>http://www.membrane.com/global_warming/notes/melting_at_both_ends.html</STRONG></A></P>
<P><STRONG><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_2_TSI_INCREASE_26_September_1991000.pdf">BSMRA_Total Solar Irradiance Increases</A></STRONG></P>
<P><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_15_Clifford_Anthony_Paiva_BSMRA_Geomagnetic_Field_Mathematics.doc"><STRONG>Clifford Anthony Paiva_BSMRA_Geomagnetic Field Mathematics.doc</STRONG></A> </P></p>
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   		    <p class="post-footer">
      <em> @ 20:14 PM</em>
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			  <p><b>Cliff:</b> The 2009 minimum is currently approaching 50% reduction since the 1979 North Pole ice cap minimum. No serious doubt should be entertained concerning the arctic ocean temperature increase. <small>(02/14/09)</small></p>
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   <div class="post"><a name=9></a>
    <h3 class="post-title">Clifford Anthony Paiva_BSMRA_Arctic and Antarctic Temperature Increases As A Function of  Solar and Geophysical External and Internal Processes Respectively</h3>
    <div class="post-body">
      <p><DIV><STRONG><A href="http://smtp.antelecom.net/blogs/BSMRAMainsite/">Back to BSMRA Main Site</A></STRONG></DIV>
<DIV><STRONG>Increased Solar Radiance; Total Solar Irradiance; Sunspots = Solar Storms; Antarctica Global Warming</STRONG>:</DIV>
<P><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_9_Hansen_Solar_Storm_Correlations_2.pdf"><IMG src="a_0_1220325018_Larsen_Ice_Shelf_Fracture_4.jpg"></A> <A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_9_Hansen_Solar_Storm_Correlations_2.pdf"><IMG src="a_1_1220325019_Larsen_Ice_Shelf_Fracture.jpg"></A> <A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_9_Hansen_Solar_Storm_Correlations_2.pdf"><IMG src="a_2_1220325020_Larsen_Ice_Shelf_Fracture_2.jpg"></A> <A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_9_Hansen_Solar_Storm_Correlations_2.pdf"><IMG src="a_3_1220325021_Larsen_Ice_Shelf_Fracture_3.jpg"></A> <BR><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_9_Increased_solar_brightness_and_warming_of_the_Earth_since_1979.doc"><STRONG>BSMRA</STRONG>_<STRONG>Increased solar brightness and warming of the Earth since 1979.doc</STRONG></A><STRONG> <BR><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_9_Hansen_Solar_Storm_Correlations_2.pdf">BSMRA</A></STRONG>_<A href="a_9_Hansen_Solar_Storm_Correlations_2.pdf"><STRONG>Hansen Solar Storm Correlations 2.pdf</STRONG></A><STRONG> </STRONG></P>
<P><A href="a_9_Cliff_PRIMARY_Prime_Military__RESUME__2009.doc"><STRONG>Clifford A. Paiva&nbsp;RESUME 2009.doc</STRONG></A> </P>
<P><STRONG><A href="http://smtp.antelecom.net/blogs/bsmasolar/a_2_HTV_Greenhouse_Gases.pdf">BSMRA_Global Heating and Hydrothermal Vent Complexes</A></STRONG></P>
<P><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_15_Clifford_Anthony_Paiva_BSMRA_Geomagnetic_Field_Mathematics.doc"><STRONG>Clifford Anthony Paiva_BSMRA_Geomagnetic Field Mathematics.doc</STRONG></A><STRONG> </STRONG></P></p>
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      <em>Clifford A. Paiva @ 20:10 PM</em>
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			  <p><b>Cliff:</b> Global heating is a function of water vapor concentration&nbsp;(and absorption) of thermal energy (8-12 microns radiation), and&nbsp;of joule heat generation, which in turn is a &nbsp;result of: a. Earth conductive core rotation through the Sun's magnetic field resulting in induced geocore currents and the Earth's geomagnetic field; b. decrease in rotation of the Earth and corresponding decrease in the Earth's&nbsp;geomagnetic field, &nbsp;which results in generating a reverse (Lenz) current and even more joule heat; c. geocore and mantle friction from the Earth's rotation decrease. Also as the joule heat from the geocore&nbsp;moves through the mantle (aesthenosphere)&nbsp;and crust (lithosphere)&nbsp;the millions of hydrothermal vent complexes releases this heat.&nbsp;&nbsp;The release is&nbsp;ejecta n the form of methane and other greenhouse gases. Shutting down every factory on the planet will not affect this geophysical and space physical (solar radiance increase) problem.  <small>(09/01/08)</small></p>
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     <h2 class="date-header">Friday, 08 August 2008</h2>
      
   <div class="post"><a name=8></a>
    <h3 class="post-title">Clifford Anthony Paiva_BSMRA_Michael Faraday and James Clerk-Maxwell: On Physical Lines of Force (1861) and A Dynamical Theory of the Electromagnetic Field (*1864); Sir Oliver Heaviside's Vector Calculus Representation of Clerk-Maxwell's Original (1861) Electromagnetic Field Equations</h3>
    <div class="post-body">
      <p><DIV align="justify"><A href="http://smtp.antelecom.net/blogs/BSMRAMainsite/"><STRONG>Back to BSMRA Main Site</STRONG></A></DIV>
<DIV align="justify"> </DIV>
<DIV align="justify"><STRONG><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_8_BSMRA_Maxwell_s_1861_paper.pdf">The Maxwell Electromagntic Field Equations</A></STRONG> as presented in most electromagnetic texts addressing <A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_8_BSMRA_Maxwell_1864_1.pdf"><STRONG>electromagnetic wave propagation</STRONG> </A>are really incorrect as to origins of the formulae involved.  The<STRONG><EM><U> vector representation</U></EM></STRONG> (and reduction) of the original 20 equations introduced by Clerk-Maxwell in 1861, is due to <STRONG><A href="http://en.wikipedia.org/wiki/Oliver_Heaviside">Sir Oliver Heaviside</A></STRONG>.  Sir Heaviside invented vector calculus primarily to restructure Maxwell's scalar and quaternion formats into his more usable vector form.    Heaviside co-discovered the <STRONG><A href="http://en.wikipedia.org/wiki/Poynting_vector">Poynting Vector Divergence of Electromagntetic Propagation Intensity ExH</A></STRONG> which relates  propagation direction and, in a conduction medium, <STRONG><A href="http://www.statemaster.com/encyclopedia/Joule-heating">joule heat dissipation losses</A></STRONG>.  Sir Heaviside also discovered the existence of the Earth's ionosphere<STRONG> </STRONG>and long distance telegraphy.  Included is a photo of <STRONG><A href="http://images.google.com/images?q=Michael+Faraday&amp;rls=com.microsoft:en-us:IE-SearchBox&amp;oe=UTF-8&amp;sourceid=ie7&amp;rlz=1I7GGLJ_en&amp;um=1&amp;ie=UTF-8&amp;ei=nbwAS-mPEoKSsgOQ7uGHCw&amp;sa=X&amp;oi=image_result_group&amp;ct=title&amp;resnum=4&amp;ved=0CCkQsAQwAw">Michael Faraday.</A></STRONG>  Most of the electromagnetic mathematical formulations by Clerk-Maxwell addressed the 50 years of <A href="http://www.greenlion.com/farad-er.html"><STRONG>Faraday's accomplishments</STRONG> </A>at the <STRONG><A href="http://www.rigb.org/registrationControl?action=home">Royal Institute in London</A></STRONG>.  The experimental work he accomplished at the <STRONG><A href="http://www.rigb.org/registrationControl?action=home">Royal Institute of Great Britain</A></STRONG> provided the pre-requisite experimental foundation, the mathematical physics of which was provided initially by <STRONG><A href="http://en.wikipedia.org/wiki/James_Clerk_Maxwell">James Clerk-Maxwell</A></STRONG>, and  later in streamlined vector form by Sir Oliver Heaviside.  Signficantly it took three men to construct the powerful foundation upon which the discipline of electromagnetics and electrodynamics has been laid. <A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_8_BSMRA_Maxwell_s_1861_paper.pdf"><STRONG>Clerk-Maxwell's 1861 <EM>On Physical Lines of Force</EM></STRONG> </A>(NOTE: Clerk-Maxwell's development of the <A href="http://en.wikipedia.org/wiki/Lorentz_force">Deflection Force (equation 77 in Clerk-Maxwell's 1861 paper</A>, is mistakenly attributed to Hendrik Lorentz); and Clerk-Maxwell's1<STRONG><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_8_BSMRA_Maxwell_1864_1.pdf">864 <EM>A Dynamical Theory of the Electromagnetic Field</EM></A></STRONG>.  These papers  significantly contributed to Clerk-Maxwell's mathematical Treatise on Electromagnetism (1873) and is available by scrolling down and clicking the hyperlink.</DIV>
<P><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_8_BSMRA_Maxwell_s_1861_paper.pdf"><IMG src="a_0_1218212952_Faraday_Heaviside_JCM_out_1.jpg"></A></P><P><A href="http://en.wikipedia.org/wiki/Maxwell's_equations"><IMG src="a_1_1218212953_Faraday_Heaviside_JCM_out_2.jpg"></A> </P><P><A href="http://en.wikipedia.org/wiki/Maxwell's_equations"><IMG src="a_3_1218212954_JCM.bmp"></A> <BR><BR><A href="a_8_BSMRA_Maxwell_1864_1.pdf"><STRONG>BSMRA_Maxwell_1864 A Dynamical Theory of the Electromagnetic Field_1.pdf</STRONG></A> </P>
<P><A href="a_8_BSMRA_Maxwell_1864_2.pdf"><STRONG>BSMRA_Maxwell_1864 A Dynamical Theory of the Electromagnetic Field 2.pdf</STRONG></A> </P>
<P><A href="a_8_BSMRA_Maxwell_1864_3.pdf"><STRONG>BSMRA_Maxwell_1864 A Dynamical Theory of the Electromagnetic Field_3.pdf</STRONG></A> </P>
<P><A href="a_8_BSMRA_Maxwell_1864_4.pdf"><STRONG>BSMRA_Maxwell_1864_A Dynamical Theory of the Electromagnetic Field 4.pdf</STRONG></A> </P>
<P><A href="a_8_BSMRA_Maxwell_1864_5.pdf"><STRONG>BSMRA_Maxwell_1864_A Dynamical Theory of the Electromagnetic Field 5.pdf</STRONG></A> </P>
<P><A href="a_8_BSMRA_Maxwell_1864_6.pdf"><STRONG>BSMRA_Maxwell_1864_A Dynamical Theory of the Electromagnetic Field 6.pdf</STRONG></A> </P>
<P><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_8_BSMRA_Maxwell_s_1861_paper.pdf"><STRONG>BSMRA_Maxwell 1861 On Physical Lines of Force.pdf</STRONG></A> </P>
<P><STRONG><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_2_TSI_INCREASE_26_September_1991000.pdf">BSMRA_Total Solar Radiance Increases</A></STRONG></P>
<P><STRONG><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_8_PUBLISHED_SCIENTIFIC_PAPERS.pdf">BSMRA</A>_</STRONG><A href="a_8_PUBLISHED_SCIENTIFIC_PAPERS.pdf"><STRONG>PUBLISHED_SCIENTIFIC_PAPERS.pdf</STRONG></A> <BR><A href="http://en.wikipedia.org/wiki/Michael_Faraday"><IMG src="a_8_Faraday.jpg"></A> </P>
<P><A href="http://www.gutenberg.org/etext/14986"><STRONG>Michael Faraday: Experimental Researches in Electricity, Volume One</STRONG></A><STRONG> (E-Book Online)</STRONG></P>
<P><STRONG><A href="http://www.gutenberg.org/catalog/world/readfile?fk_files=11280">James Clerk-Maxwell</A> (E-Books and Papers Online)</STRONG></P>
<P><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_15_Clifford_Anthony_Paiva_BSMRA_Geomagnetic_Field_Mathematics.doc"><STRONG>Clifford Anthony Paiva_BSMRA_Geomagnetic Field Mathematics.doc</STRONG></A> </P></p>
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      <em>Clifford A. Paiva @ 09:29 AM</em>
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			  <p><b>Cliff:</b> The majority of electromagnetic texts state the vector form of Clerk-Maxwell&#39;s field equations.  In fact, if these four equations were presented to Maxwell in the 1870s he would not recognize them since vector calculus was not yet introduced to the mathematical physics world.  Oliver Heaviside invented vector analysis and calculus and transcribed Clerk-Maxwell&#39;s original 20 field equations, reducing these to four primary vector equations.  Heaviside also co-discovered the Poynting Vector, the Maxwell Lorentz force in vector form, the Earth&#39;s ionosphere and trans-atlantic communications transmission. <small>(08/08/08)</small></p>
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     <h2 class="date-header">Wednesday, 25 June 2008</h2>
      
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<P><STRONG><A href="http://smtp.antelecom.net/blogs/bsmasolar/a_2_HTV_Greenhouse_Gases.pdf">BSMRA_Global Heating and Warming Caused by Hydrothermal Vent Complexes</A></STRONG></P>
<P><A href="http://smtp.antelecom.net/blogs/bsmaGMF/a_15_Clifford_Anthony_Paiva_BSMRA_Geomagnetic_Field_Mathematics.doc"><STRONG>Clifford Anthony Paiva_BSMRA_Geomagnetic Field Mathematics.doc</STRONG></A> </P></p>
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      <em>Clifford A. Paiva @ 09:50 AM</em>
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			  <p><b>Cliff:</b> Contributors to global heating: a.) Earth rotation decrease and transfer of rotational kinetic energy to friction generated thermal energy  (geocore through mantle, crust, oceans and atmosphere); b.) decay of the geomagnetic field inducing geocore electrical currents and joule heat from the currents; c.) increase methane and carbon dioxide greenhouses gases emanating from the increasing temperatures of the calcium carbonate (CaCO3) calcarous limestone sediments which cover the  lithosphere beneath the oceans, including the globally distributed hydrothermal vent complex systems; d.) increased temperatures of the Sun and the associated solar storm frequency.  The cumulative effect from these processes is an increase in Earth (and other planets) mean temperature indices. <small>(10/19/08)</small></p>
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     <h2 class="date-header">Friday, 23 May 2008</h2>
      
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    <h3 class="post-title">Clifford Anthony Paiva_BSMRA_Geomagnetic Field Decay in Correlation to the Increase in Solar Storm Activity and Radiance</h3>
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      <p><DIV align="justify"><FONT color="#000080"><STRONG><A href="http://www.google.com/search?q=Clifford+A.+Paiva+BSMRA&amp;hl=en&amp;filter=0">[All BSMRA Sites]</A></STRONG></FONT></DIV>
<DIV align="justify"><FONT color="#000080">This section addresses the increase in solar storm activity and radiance as driving factors for the decay of the Earth's geomagnetic field (GMF).  Apparently the decay of the GMF primary protective barrier (against high energy particles, i.e.. UV, X-ray, gamma ray, cosmic rays) for the Earth, is decaying as a function of <U><STRONG>decreased</STRONG></U> geocore current density.  The Earth possesses an internal induced current of billions of amps which is generated by the conducting geocore's rotation through the Sun's interplanetary magnetic field.  Since the geocore is decreasing in rotational angular velocity through the Sun's magnetic field, the induced current within the Earth dies.  As the internal geocore's current intensity decays so does its associated induced geomagnetic field also disintegrate.  The equation for this Faraday Disk effect is (final electric current) = (initial current)[exp{[(induction)(angular velocity)/2piL]-(R/L)}(time).  The sign becomes increasingly negative as the angular velocity decreases.  Changing (reversing) geomagnetic field polarity <STRONG><U>does not</U></STRONG> increase the current density, and certainly <STRONG><U>does not increase the induced geomagnetic field's intensity.</U></STRONG>  To increase the geomagnetic field's intensity the Earth's geocore must <EM>increase</EM> in angular velocity.  This is not possible in accordance with the Second Law of Thermodynamics as freely rotational systems tend to decrease in rotation as a function of time through dissipative media.  As a matter of fact all planet's of this solar system, including the Sun itself, is <EM>decreasing</EM> in angular velocity, and the associated magnetic fields of Mercury, Earth, Jupiter, Saturn, Uranus, and Neptune are also decreasing as these planets slow in rotation.  The Sun's equatorial rotation rate is itself also decreasing in rotation through the Milky Way's intra-galactic magnetic field. (Other sections of the BSMR website address galaxies and galactic mass-loss; see the <STRONG>All Sites</STRONG> file).</FONT></DIV>
<P><IMG src="a_0_1211578384_GMF_9.jpg"></P><P><IMG src="a_1_1211578385_GMF_1.jpg"></P><P><IMG src="a_2_1211578386_GMF_2.jpg"></P><P><IMG src="a_3_1211578386_GMF_3.jpg"></P><P><IMG src="a_4_1211578387_GMF_4.jpg"></P><P><IMG src="a_5_1211578387_GMF_5.jpg"></P><P><IMG src="a_6_1211578388_GMF_6.jpg"></P><P><IMG src="a_7_1211578389_GMF_7.jpg"></P><P><IMG src="a_8_1211578389_GMF_8.jpg"> </P>
<P><A href="http://smtp.antelecom.net/blogs/BSMRAMainsite/"><STRONG>Back to BSMRA Main Site</STRONG></A></P>
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      <em>Cliff Paiva @ 14:33 PM</em>
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		<p class="profile-textblock">[PLEASE USE CONTROL (+) FOR ZOOMS AND CONTROL (0) FOR NORMAL VIEWS]. All EXCEL plots were generated at BSMRA.  The zero relationship to polarity reversal
and intensity is provided.  

GLOBAL HEATING (WARMING): 
Global warming is a function of increased evaporation rates of water vapor from 
the
the 330 million cubic miles from this ocean planet.  The increased rates are a
function
of tidal friction among a decelerating geocore, aesthenosphere (mantle), 
lithosphere (crust) and oceans. Also the collapsing geomagnetic field-generated 
Geo-Core electrical joule heating, and increased
solar storm activity (see Hansen, etc. below) play an ever increasing significant
role.  Increased hydrothermal venting of extremely warm waters and methane also
play a major role.   Methane and carbon dioxide are 
currently
emissions with less direct effect than water vapor; being generated from the increased 
temperatures of the
continental shelves.  From the continental shelves calcium carbonates are converted 
to carbon dioxide (CO2).  
Methane (CH4), which 
possesses 20 times more heat capacitance than CO2, is also being released 
from the northern shelf areas.  

GEOMAGNETIC FIELD: The geomagnetic field is a primary source of joule 
heating 
within the Earth's Geo-Core.  The loss of the effective geomagnetic field in 
less than 1000 
years will
be ultimately lethal to this planet's biosphere.  The increased evaporation rates at the
North and South 
Poles will dramatically increase condensation and precipitation over 
the continents and probably be misinterpreted as a drop in overall climate temperatures.

FROM THE LORD'S POSITION;

Folks should not singularly ask the Lord Jesus Christ to prevent geophysical tragedies 
caused by global heating on the one hand, while continue  our  "legalization" of
homosexual perversion (a perverted Barak Obama and his administration not withstanding)
and the killing of unborn children on the other hand.  God is not amused by 
this sort of audacious hypocracy.)

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