PLUS TWO
PHYSICS
ATOMS
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                                                       A very small fraction of incident alpha
                                                        particle retraced its path
                   ATOMS
Scattering of alpha particle
Geiger Marsden experiment
Experimental set up
 Radioactive source of alpha particle is kept
  inside an lead cavity with a narrow opening
 5.5MeV a-particles emitted by the source
  are made into a narrow well collimated
  beam using led slits. Beam is allowed to fall
  on a thin gold foil of thickness 2.1 × 10 m
 The alpha particle scattered in different di-
  rection can be absorbed by using the rotat-
  able Zinc sulphide screen and microscope
                                                   Conclusions
  arrangement.
                                                       Since most of the alpha particle passed
 These alpha particle produce light flashes            through the foil undeflected, it is concluded
  on the screen so the number of alpha par-             that major part of an atom is empty.
  ticle scattered at different angles can be
  counted                                              A few of the alpha particle suffer a large an-
                                                        gle deviation and are very small fraction re-
                                                        traced its path.
Observations                                           since the alpha particle itself 7350 times
                                                        heavier than the electron, neither an elec-
 The most of alpha particle passed through
                                                        tron nor similar positive charged particle
  the foil straight or with very small deviation
                                                        could cause such a large angle deviation.
 About 0.14 percentage of incident a-particle
  scattered by more than 1∘                            Rutherford argued that, the alpha particle
 About one in 8000 get deflected through 90∘           must had encountered a very heavy posi-
   or more.                                             tive particle on its path.
                ADMISSION STARTED      6009 100 300                                                      3
  The electrostatic force of repulsion between          As it approaches the nucleus its velocity
   the alpha particle and this heavy positive             (kinetic energy )progressively decreases
   core causes such a large angle deviation               due to electrostatic force of repulsion from
                                                          the nucleus.
  This central positive core is named as nu-
   cleus                                                 At some distance d from the nucleus the
                                                          alpha particle come to rest for moment
  Very rarely an alpha particle travels head             and then retraces its path.
   on towards the nucleus. these alpha parti-            At the distance 𝑑, when the a particle is
   cle re-traces its path. The size of the nucleus        at rest, it's kinetic energy is completely
   is very small                                          converted into the electrostatic potential
                                                          energy.
Impact parameter                                        The distance 𝑑 is called distance of closest
                                                        approach.
 Impact parameter is the perpendicular dis-
 tance of the initial velocity vector of the alpha          Ze
 particles from the centre of the nucleus.
                                                          01. An a-particle having a kinetic energy
                                                              5MeV is found to be scattered by a gold
                                                              nucleus through 180∘. Calculate the
  Those with small impact parameter sufferer
   large scattering.
                                                              distance of closest approach. 𝑍 = 79 for
  a- particle with large impact parameter get                gold
   scattered through smaller angles
  In the case of head on collision,impact pa-
   rameter is zero and a-particles rebound
   back.
                                                     Rutherford’s Nuclear
Distance of closest approach                         model of atom
  Consider an alpha particle of mass m and             On the basis of the alpha particle scattering ex-
   initial velocity v moves towards the nucleus         periment in 1911 Rutherford proposed his nuclear
   of charge is Ze.                                     model of an atom. nuclear model which is also
                                                        known as planetary atom model.
                  ADMISSION STARTED      6009 100 300                                                       4
 An atom maybe regarded as a sphere of              Radius of nth orbit
  size 10−10 m. The entire positive charge and
  most of the mass is concentrated at the
  central core called nucleus.                          Which means the radii of the stationary or-
 The electrons have no place inside the nu-            bit are in the ratio 1: 4: 9: 16..
  cleus they revolve around the nucleus at
  some distance away. The centripetal force
  for the revolution is provided by the electro-
  static force of attraction between the nucle-
  us and electrons.
                                                         02. In bore model of hydrogen atom which
 The amount of positive charge of the nucle-                of the following is quantised?
  us is exactly equal to the amount of nega-
  tive charges on all the electrons of the atom.         (a) Linear momentum of the electron
  That means the atom is electrically neutral.           (b) Angular momentum of the electron
                                                         (c) Linear velocity of the electron
Drawbacks of Rutherford's atom                           (d) Angular velocity of the electron
model
 In Rutherford's atom model it is assumed
  that the electrons revolve around the nu-
  cleus in circular orbit and it experiences a
  centripetal acceleration.
 According to the electromagnetic theory,
  an accelerated electric charge should emit
  electromagnetic radiation therefore the re-            03. In the Bohr’s hydrogen atom model, the
  volving electron should emit radiation.                     radius of the stationary orbit is directly
                                                              proportional to the principal quantum
 If the radiation is continuously emitted it's an            number n as
  energy will decrease and electrons would
  finally fall into the nucleus. That means an           (a) 𝑛−2                 (b) 𝑛2
  atom cannot be stable.                                 (c) n                   (d) n–
Bohr atom model
In an atom the electrons cannot revolve around
the nucleus in all paths. They can only Revolve
through certain stationary orbit in which the
angular momentum of the revolving electron is
an integer multiple of ℎ/2𝜋                              04. In Bohr’s atom model the orbit radii are
                                                             in the rat
   Where h is the Plank's constant
                                                         (a) 1: 2: 3             (b) 1: 3: 5
   n = 1,2,3,.. is the principal quantum numbers         (c) 1: 4: 9             (d)2: 4: 6
   𝑚 = mass of the electron
   𝑣 = orbital velocity of electron
   𝑟 = radius of the orbit
                 ADMISSION STARTED       6009 100 300                                                      5
The line spectra of
hydrogen atom                                                  A. Name different series obtained in hy-
                                                                  drogen spectrum?
 According to bohr postulate, when an electron                 B. Draw energy level diagram of hydrogen
 make a transition from the outer orbit ni of the                 atom
 energy Ei to inner orbit nf of energy Ef a photon
 of energy 𝐸𝑖 − 𝐸𝑓 is emitted
  For Lyman series, 𝑛𝑓 = 1, 𝑛𝑖  = 2,3,4 …
  For Balmer series, 𝑛𝑓 = 2, 𝑛𝑖 = 3,4,5 …
  For Paschen series, 𝑛𝑓 = 3, 𝑛𝑖 = 4,5,6 ….
  For Brackett series, 𝑛𝑓  = 4, 𝑛𝑖 = 5,6,7
                                                        de Broglie explanation of Bohr
                                                        postulate of Quantisation
                                                             From Bohr's postulate the angular momentum
                                                             of orbiting electron is
                                                             de Broglie suggested that the electron in their
                                                             permitted orbits should be seen as a particle
                                                             wave. Just like waves travelling on a string.
   A. An electron is revolving around the nu-
      cleus of hydrogen atom in an orbit of ra-
      dius 9 times the radius of the first orbit.
      Angular momentum of the electron in                    Therefore the circumference of the orbit must
      this orbit is...                                       be an integral multiple of the particle wave-
                                                             length.
   B. Sketch the energy level diagram of hy-
      drogen atom and sketch the transition
      corresponding to Balmer series
                   ADMISSION STARTED          6009 100 300                                                     6
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