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Atoms
Thomson Model
Rutherford Scattering Experiment
• Bombarded Gold foil with alpha –particles ( He2+ ions )
Observations
• Very large number of particles went undeviated (or deviated through
small angles ) .
• Very few particles rebounded or suffered large angle deviations
• At small angles of deviations there are large
number of particles because most of the
particles suffered small angle deviations
Conclusions
• Atom is mostly empty
• Positive charge is concentrated in a small radius called nucleus
• Nucleus is very small as compared to Atom.
• Alpha Particle and Nuclei interaction
• Since both are positively charge they will repel each other . And
finally alpha particle will stop . Alpha particle has +2e charge
• Initial energy = (1/2)malphav2 Final Energy = K (2e) (Ze) / d
Bohr’s Model
• Electrons revolve around nucleus in fixed orbits having fixed energies
• For nth orbit , angular momentum about centre is :
Angular Momentum is Quantised
Whenever electron jumps from higher energy state to lower energy
state , energy is released in the form of photons .
Efinal –Einitial = hvphoton
Radius ,Velocity and Energy in orbit
Radius = ( It is obvious that radius will increase with n ,
but it increases with n2)
Velocity ∝
𝒁
𝒏
• Time period of electron in orbit
Distance = 2 pi rn ∝ n2/Z
Velocity ∝ Z/ n
Time period = Distance /Speed ∝ (n2/Z) x (n/Z) ∝ n3/Z2
Frequency = 1/T
Energy levels are discrete
• Total Energy = (∝ Z2/n2)
• Total energy is negative implies electron is bound
• Kinetic Energy = (KE is always +ve , ½ mv2)
• Potential Energy = Total Energy – Kinetic Energy
For Hydrogen
• Ground = -13.6 eV
• First excited = -3.4 eV
• Third = -1.51 eV
• Fourth = -0.85 eV
• .
• .
• Infinity = 0
Example : Following energies are given to H
atom .Will it accept ?
a) 10.2 eV Yes , because E2-E1 = 10.2
b) 5eV No
c) Photon of wavelength 102.5 nm
E = 1240/ 102.5 = 12.09 eV E3 – E1 =12.09
So it will accept
d) 1.89 eV Yes because E3-E2 =1.89 eV
So , If you give white light to H atom , it will accept only few
frequencies out of all .
• So if we give White light , it will absorb only some wavelengths .
• Also after getting excited it will emit some particular frequency
photons
• This is called atomic spectrum and is used as fingerprint for elements.
All elements have different spectrums
Only few wavelengths
absorbed 
Rydberg Formula
• When an electron is in excited state , it is unstable , So it jumps down
to lower states to gain some stability . When an electron jumps from
higher energy orbit to lower energy orbit , energy is emitted in the
form of photons with Wavelength
Name of series
• First line has smallest energy difference
 Largest λ
N=1 Lyman
N=2 Balmer
N=3 Paschen
Example :
• a ) 3  1
Einitial =-1.51eV Efinal= -13.6
Change = Efinal-Einitial =-13.6- (-1.51) =-12.09
-ve sign indicates energy is released .
Erelased = 12.09 eV = 1240 / λ  λ= 102.5 nm
b) Infinity  3
Einfinity =0 E3= -1.51
Change = -1.51 eV (-ve means Released )
1.51 = 1240/λ  λ =821.19 nm
c) Ionisation  1 – infinity
E 1 = -13.6eV Einfinity= 0
Change = final – initial = 0 – (-13.6) = + 13.6
+ve means energy is required to ionise
13.6 = 1240/ λ  λ= 91.17 nm
d) First excitation 12
Change = -3.4 –(-13.6) = +10.2eV
10.2 eV = 1240/ λ = 121.56 nm
A H sample is at 5 th excited state , How many
spectral lines are possible
5th excited  n=6
Possible = 65 6  4 6 3 62 6 1
54 53 52 51
43 42 41
32 31
21
Total number of lines = 15
Alternative : 6C2 = 15
An excited H sample is found to emit 6 different
spectral lines , find the state of sample
• Number of lines = 6
Let the sample is at nth state
nC2 = 6  n =4
Relation with de Broglie
• Wavelength of electron in n th orbit . Standing waves are formed ( L=n λ)
• r ∝ n2/Z  λ ∝n/Z

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Atoms

  • 3. Rutherford Scattering Experiment • Bombarded Gold foil with alpha –particles ( He2+ ions )
  • 4. Observations • Very large number of particles went undeviated (or deviated through small angles ) . • Very few particles rebounded or suffered large angle deviations • At small angles of deviations there are large number of particles because most of the particles suffered small angle deviations
  • 5. Conclusions • Atom is mostly empty • Positive charge is concentrated in a small radius called nucleus • Nucleus is very small as compared to Atom. • Alpha Particle and Nuclei interaction • Since both are positively charge they will repel each other . And finally alpha particle will stop . Alpha particle has +2e charge • Initial energy = (1/2)malphav2 Final Energy = K (2e) (Ze) / d
  • 6. Bohr’s Model • Electrons revolve around nucleus in fixed orbits having fixed energies • For nth orbit , angular momentum about centre is : Angular Momentum is Quantised Whenever electron jumps from higher energy state to lower energy state , energy is released in the form of photons . Efinal –Einitial = hvphoton
  • 7. Radius ,Velocity and Energy in orbit Radius = ( It is obvious that radius will increase with n , but it increases with n2) Velocity ∝ 𝒁 𝒏
  • 8. • Time period of electron in orbit Distance = 2 pi rn ∝ n2/Z Velocity ∝ Z/ n Time period = Distance /Speed ∝ (n2/Z) x (n/Z) ∝ n3/Z2 Frequency = 1/T
  • 9. Energy levels are discrete • Total Energy = (∝ Z2/n2) • Total energy is negative implies electron is bound • Kinetic Energy = (KE is always +ve , ½ mv2) • Potential Energy = Total Energy – Kinetic Energy
  • 10. For Hydrogen • Ground = -13.6 eV • First excited = -3.4 eV • Third = -1.51 eV • Fourth = -0.85 eV • . • . • Infinity = 0
  • 11. Example : Following energies are given to H atom .Will it accept ? a) 10.2 eV Yes , because E2-E1 = 10.2 b) 5eV No c) Photon of wavelength 102.5 nm E = 1240/ 102.5 = 12.09 eV E3 – E1 =12.09 So it will accept d) 1.89 eV Yes because E3-E2 =1.89 eV So , If you give white light to H atom , it will accept only few frequencies out of all .
  • 12. • So if we give White light , it will absorb only some wavelengths . • Also after getting excited it will emit some particular frequency photons • This is called atomic spectrum and is used as fingerprint for elements. All elements have different spectrums Only few wavelengths absorbed 
  • 13. Rydberg Formula • When an electron is in excited state , it is unstable , So it jumps down to lower states to gain some stability . When an electron jumps from higher energy orbit to lower energy orbit , energy is emitted in the form of photons with Wavelength
  • 14. Name of series • First line has smallest energy difference  Largest λ N=1 Lyman N=2 Balmer N=3 Paschen
  • 15. Example : • a ) 3  1 Einitial =-1.51eV Efinal= -13.6 Change = Efinal-Einitial =-13.6- (-1.51) =-12.09 -ve sign indicates energy is released . Erelased = 12.09 eV = 1240 / λ  λ= 102.5 nm b) Infinity  3 Einfinity =0 E3= -1.51 Change = -1.51 eV (-ve means Released ) 1.51 = 1240/λ  λ =821.19 nm
  • 16. c) Ionisation  1 – infinity E 1 = -13.6eV Einfinity= 0 Change = final – initial = 0 – (-13.6) = + 13.6 +ve means energy is required to ionise 13.6 = 1240/ λ  λ= 91.17 nm d) First excitation 12 Change = -3.4 –(-13.6) = +10.2eV 10.2 eV = 1240/ λ = 121.56 nm
  • 17. A H sample is at 5 th excited state , How many spectral lines are possible 5th excited  n=6 Possible = 65 6  4 6 3 62 6 1 54 53 52 51 43 42 41 32 31 21 Total number of lines = 15 Alternative : 6C2 = 15
  • 18. An excited H sample is found to emit 6 different spectral lines , find the state of sample • Number of lines = 6 Let the sample is at nth state nC2 = 6  n =4
  • 19. Relation with de Broglie • Wavelength of electron in n th orbit . Standing waves are formed ( L=n λ) • r ∝ n2/Z  λ ∝n/Z