MODULE 8 IQ 3 Flashcards

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1
Q

limitations of rutherford’s atomic model

A
  • could not explain electron/atomic stability
  • no restriction on orbit of electrons –> produce continuous spectra –> contradicts existing discrete emission lines of hydrogen atoms
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2
Q

bohr’s 1st postulate

A

electrons orbit in stationary states and do not radiate energy –> stays in quantised energy levels

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3
Q

bohr’s 2nd postulate

A

transition between stationary states would be accompanied by absorption or emission of energy in the form of EMR

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4
Q

bohr’s 3rd postulate

A

angular momentum is quantised
- electrons undergo uniform circular motion due to electrostatic attraction between itself and nucleus

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5
Q

limitations of bohr’s atomic model

A
  • did not clearly explain discrete emission of photons beyond hydrogen
  • didn’t explain why hydrogen spectral lines were not of equal intensity
  • zeeman effect –> when gas is excited in magnetic field, emission spectrum shows a splitting of spectral line
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6
Q

balmer equation

A

calculate wavelengths of these lines
1/wavelength = R(1/m^2 - 1/n^2)

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7
Q

rydberg’s equation

A

predict wavelength of proton absorbed or emitted when an electron transitions between orbits of different states

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8
Q

louis de broglie equation

A

wavelength = h/mv

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9
Q

louis de broglie model

A

linked waves and particles together
- any moving particle has an associated wavelength
- should be possible to detect wave nature of electrons if they were diffracted from surface of crystal

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10
Q

using de broglie to explain stationary states

A

applying particle-wave duality –> electron orbits were standing waves (radius of each energy level was an integer multiple of electron’s wavelength)
n x h/2(pi) = 2(pi)r
- now orbit in standing waves, they do not lose energy

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11
Q

davisson and gemer

A

tried to observe the scattering of electrons onto the surface of a piece of nickel
- accidentally annealed the metal, producing a smooth region of large crystals
- formed interference pattern –> calculate wavelength of electron by using diffraction methods: wavelength = 2dsin(theta)

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12
Q

erwin schrodinger model of the atom

A
  • defined a wave function through solving a differential equation derived from the forces acting upon an electron
  • square of this wave gave probability that an electron would be at that distance from the nucleus
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