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 The Spectrum Of X Xay Obtained Farm Coolidge Tube
Is Generally Continues Duane Continuous X Ray
Spectra.
 A Continuous Spectrum Is Obtained When The Low
Energy Electors The Target Under Certain Conditions
But In General The Background Of Continuous
Spectrum Always Has The Characteristic Line The
Characteristic Energy Of The Striking Electrons In
Creases Continuous Spectrum Remain The Same Bor
Various Energies Of The Dirking Electrons
 At Each Energy Value Of The Striking Electrons
The Carve Has A Sharp Limit On The Short
Wavelength Side
 The Shortest Wave Lengthen Limit (Limn) Does
Not Depend On The Material Of The Target But
Depends On The Tube Voltage
 Higher The Accelerating Voltage Affined Across
The Tube , Shorter Is The Wavelength Limit
 Higher The Accelerating Voltage , Higher Is The Internist Of X Ray
Of All Wavelength
 At Each Accelerating Voltage , The Intensity Of X Ray First Increase
As The Wavelength Decreases From The Longer Side Become
Maximum Corresponding To A Definite Wave Length The , Intensity
Rapidly Falls To Zero .
 Higher The Table Voltage Lower Is The Wavelength At Which The
Maxima Of Intensify Occurs
 Although The Short Wavelength Limit At A Given Tube Voltage Is
Index Pendent Of The Material Of The Target , But The Current ,
Depends On The Atomic Number Of The Target Material
 The Bract That The Sharp Lower Wavelength Limit Limn Of The
Continuous Spectrum Is Independent Of The Target Material And
Depends Only On The Accelerating Voltage Planking Quantum
Theory’s , According To Which If The Accelerating Potent As
Between The Bailment And Amide The Of The X Ray Table Is V
Volt, The Minimum Kinetic Energy By The Electron In Passing From
The Cathode To The Tangent Will Be Co Joule .
 When This Electron Strikes An Atom Of A Target ,
It Can Give Up At The Mast Its Entire Kinetic Energy To The Atom
Of The Target As A Result Of Which Thane Is Emitted In Form Of A
Photon.
 If u is the frequency Of Photon Emitted The Energy Of
Photon Will Be Hub Obviously Hub Will Be Either Fayal
To Eva Or Less Then Is
 Thus The X Ray Emitted From The Target Will Be Of
Frequencies In A Continuous Range Below A Maximum
Limit The Maximum Frequency max Is Given As
 Thus The Shortest Wavelength Limit Limn Is Inversely Proportional To
The Tube Voltage V The Expression (2) Is Also Knur As The Duane –
Hunt’s Low
 At May Be Mentioned Here That In The Emission Of X Ray When The
Entire Kinetic Energy Of Electrum Is Concerted Into The Radiant
Energy We Get The X Ray Of Shortest Wavelength Whereas In The
Photos – Electric Effect, Radiant Energy Is Mating Conover Anton The
Kinetic Energy Of Electrons
 This Is Why The Phenomenon Of Continuous Spectra Of X Rays Is
Also Culled The Inverse Photo Electric Effect.
The End

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CONTINUOUS X RAY SPECTRUM ITS DEPENDENCE ON VOLTAGE DUANE AND HUNT LAWRohini yadav 2

  • 1.
  • 2.
  • 3.
  • 4.
  • 5.  The Spectrum Of X Xay Obtained Farm Coolidge Tube Is Generally Continues Duane Continuous X Ray Spectra.  A Continuous Spectrum Is Obtained When The Low Energy Electors The Target Under Certain Conditions But In General The Background Of Continuous Spectrum Always Has The Characteristic Line The Characteristic Energy Of The Striking Electrons In Creases Continuous Spectrum Remain The Same Bor Various Energies Of The Dirking Electrons
  • 6.  At Each Energy Value Of The Striking Electrons The Carve Has A Sharp Limit On The Short Wavelength Side  The Shortest Wave Lengthen Limit (Limn) Does Not Depend On The Material Of The Target But Depends On The Tube Voltage  Higher The Accelerating Voltage Affined Across The Tube , Shorter Is The Wavelength Limit
  • 7.  Higher The Accelerating Voltage , Higher Is The Internist Of X Ray Of All Wavelength  At Each Accelerating Voltage , The Intensity Of X Ray First Increase As The Wavelength Decreases From The Longer Side Become Maximum Corresponding To A Definite Wave Length The , Intensity Rapidly Falls To Zero .  Higher The Table Voltage Lower Is The Wavelength At Which The Maxima Of Intensify Occurs  Although The Short Wavelength Limit At A Given Tube Voltage Is Index Pendent Of The Material Of The Target , But The Current , Depends On The Atomic Number Of The Target Material
  • 8.  The Bract That The Sharp Lower Wavelength Limit Limn Of The Continuous Spectrum Is Independent Of The Target Material And Depends Only On The Accelerating Voltage Planking Quantum Theory’s , According To Which If The Accelerating Potent As Between The Bailment And Amide The Of The X Ray Table Is V Volt, The Minimum Kinetic Energy By The Electron In Passing From The Cathode To The Tangent Will Be Co Joule .  When This Electron Strikes An Atom Of A Target , It Can Give Up At The Mast Its Entire Kinetic Energy To The Atom Of The Target As A Result Of Which Thane Is Emitted In Form Of A Photon.
  • 9.  If u is the frequency Of Photon Emitted The Energy Of Photon Will Be Hub Obviously Hub Will Be Either Fayal To Eva Or Less Then Is  Thus The X Ray Emitted From The Target Will Be Of Frequencies In A Continuous Range Below A Maximum Limit The Maximum Frequency max Is Given As
  • 10.  Thus The Shortest Wavelength Limit Limn Is Inversely Proportional To The Tube Voltage V The Expression (2) Is Also Knur As The Duane – Hunt’s Low  At May Be Mentioned Here That In The Emission Of X Ray When The Entire Kinetic Energy Of Electrum Is Concerted Into The Radiant Energy We Get The X Ray Of Shortest Wavelength Whereas In The Photos – Electric Effect, Radiant Energy Is Mating Conover Anton The Kinetic Energy Of Electrons  This Is Why The Phenomenon Of Continuous Spectra Of X Rays Is Also Culled The Inverse Photo Electric Effect.