1.3 Rutherford, Planck, and Bohr *** Flashcards

1
Q

Earnest Rutherford

A

an atom has a dense, positively charged nucleus which accounts for only a small portion of the atom’s volume

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2
Q

Max Planck

A
  • developed the first quantum theory:
    • energy emitted as electromagnetic radiation from matter comes in discrete bundles called quanta
    • Planck’s relation (equation): determines the energy of a quanta
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3
Q

quanta (quantum is singular)

A

discrete bundles of energy emitted as electromagnetic radiation from matter

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4
Q

electromagnetic radiation

A

produced by the vibration of charged particles with electrical and magnetic properties (travels at the speed of light)

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5
Q

Planck’s relation (energy of a quantum)

A
  • E = hf
    • E = energy of a quanta
    • h = Planck’s constant = 6.626 x 10-34 J ∙ s
    • f = frequency of the radiation (f is sometimes designated by the Greek letter, nu: ν )

***of note:

v = fλ

or

c= fλ

c = speed of light (3 x 108m/s)

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6
Q

Niels Bohr

A
  • developed the Bohr model
    • angular momentum of an electron
    • energy of an electron
    • orbit
    • ground state and excited state
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7
Q

Bohr model

A
  • Bohr model: a hydrogen atom consists of a central (+) proton which a (-) electron travels around in discrete, circular orbits
    • centripetal forces acting on the electron due to electrostatic force between (+) charged proton and (–) charged electron
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8
Q

angular momentum (of an electron)

A
  • angular momentum: L = nh/2π

L = angular momentum of an electron orbiting the nucleus of a hydrogen atom

n = principal quantum number (any positive integer)

h = Planck’s constant = 6.626 x 10-34 J ∙ s

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9
Q

angular momentum (cont…)

A
  • classical mechanics states an object revolving in a circle (such as an electron), can assume an infinite number of values for its radius and velocity
    • using Planck’s quantum theory, Bohr placed restrictions on the possible values of angular momentum
      • ***principal quantum number (n) does this
        • it is the only variable in the equation (the rest are constants)
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10
Q

energy of an electron (eq)

A

E = - RH / n2

  • E = Rydberg unit of energy
    • RH = 2.18 x 10-18 J/electron
  • n = principal quantum number
    • ***E n ( means directly proportional)
      • the energy of an electron increases - becomes less negative (closer to zero) - the farther out it is from the nucleus (greater n becomes)
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11
Q

atomic orbital (orbit)

A
  • UTD definition: the region of space where there is a high probability of finding an electron
  • the pathway an electron follows around a nucleus
    • if one could transfer an amount of energy exactly equal to the difference between one orbit and another, this could result in an electron “jumping” from one orbit to a higher one
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12
Q

ground state (n=1)

A
  • n = 1
  • ground state of an atom is the lowest energy
    • all electrons are in the lowest possible orbit if an atom is in ground state
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13
Q

excited state (n > 1)

A
  • an excited state of an atom is when at least one electron has moved to a subshell higher than normal energy

***all systems tend toward minimal energy → on the MCAT atoms will generally exist in the ground state unless subjected to extreme heat or irradiation

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14
Q

Bohr model

A

***we know know Bohr’s model is not UTD

***it only accounts for an atom with only 1 electron, not multiple

***it is not possible to pinpoint the velocity and location in space of an electron at any point in time

***electrons are not restricted to specific pathways; but they tend to localize in space

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15
Q

applications of the Bohr model

A

atomic emission and atomic absorption

***Bohr Model only applies to one-electron systems (such as H+ or Li2+)

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16
Q

atomic emission spectra

A
  • at room temp, the majority of atoms are in the ground state
    • heat or irradiation can excited electrons to higher energy states
      • Absorb light
      • Higher potential
      • Excited state
      • Distance (farther from nucleus)
  • the lifetime of an excited state is brief → electrons return rapidly to ground state → electrons emit discrete amounts of energy in the form of photons
17
Q

Figure 1.5 Atomic Emission of a Photon as a result of a ground state transition

A
18
Q

atomic emission spectra

A
  • emission spectrum: the spectrum of frequencies of electromagnetic radiation (energy) emitted due to an electron transitioning from a higher energy state to a lower energy state
    • the electromagnetic energy emitted is in the form of a photon
      • there are many possible electron transitions for each atom of an element
        • each transition has specific energy differences
          • the energy of the emitted photon is = the energy difference between the two states
            • this difference is quantized, not continuous (stairs vs ramp)
              • the result is a spectrum of the specific wavelengths/frequencies (fluorescence)
                • what we see is the color of the emitted light
                  • we can use this spectrum to identify elements
19
Q

line spectrum (atomic emission spectrum)

A

Each line on the spectrum corresponds to a specific electron transition

20
Q

energy of photon (eq): electromagnetic energy of emitted photon from electron energy transition

A

E = energy of a emitted photon

h = Planck’s constant (6.626 x 10-34 J ∙ s)

c = speed of light (3 x 108 m/s)

λ = wavelength of the radiation

*** E = hf = hc/λ

****energy is inversely proportional to wavelength

-when an electron returns from an excited state to a ground state, it releases a discrete amount of energy in the form of a photon

21
Q

Bohr model of hydrogen atom:

  • Lyman series
  • Balmer series
  • Paschen series
A

group of hydrogen emission lines corresponding to transition levels:

  • Lyman series: n ≥2 to n =1
  • Balmer series: n ≥3 to n =2
  • Paschen series: n ≥4 to n =3
22
Q

the energy associated with a change in the principal quantum number (n) from a higher initial value to to a lower final value

A
  • combined from Planck’s and Bohr’s equations

***unlike other equations → this is initial* minus *final

positive (+) E → emission

negative (-) E → absorption

23
Q
A
  • the energy of an emitted photon corresponds to the difference in energy between the higher-energy initial state and the lower-energy final state
24
Q

atomic absorption spectrum

A
  • when an electron transitions from a lower energy level to a higher energy level, it must absorb a specific level of energy in order to do so
    • each element absorbs energy at different, specific wavelengths (λ)
      • elements in the gas phase are identified using the absorption spectra
25
Q

atomic emission spectra and atomic absorption spectra

A
  • each element has a characteristic set of energy levels specific to that element
    • when an electron moves from a lower energy level to a higher energy level → it must absorb the right amount of energy to do so
    • when an electron moves from a higher energy level to a lower energy level → it must emit the right amount of energy to do so
  • this energy is in the form of light (photon)

***the amount of energy an electron must absorb or emit is the same when transitioning between the same two levels

26
Q

1.3 Concept Check (#1)

A
27
Q

1.3 Concept Check (#2)

A
28
Q

1.3 Concept Check (#3)

A