Ch. 28- Atomic Physics

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Last updated 2:20 AM on 4/24/26
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12 Terms

1
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rest mass energy

-Mass is just another form of energy!

-E is total relativistic energy (needed for speeds greater than about 1% the speed of light to avoid large errors)

-K is relativistic kinetic energy (it has its own equation we are not going to talk about)

-from Einstein’s relativity

*if convert all electron mass into energy, get energy to hold nucelus together → nuclear power plants/fusion

<p><strong>-Mass is just another form of energy!</strong></p><p>-E is total relativistic energy (needed for speeds greater than about 1% the speed of light to avoid large errors)</p><p>-K is relativistic kinetic energy (it has its own equation we are not going to talk about)</p><p>-from Einstein’s relativity</p><p>*if convert all electron mass into energy, get energy to hold nucelus together → nuclear power plants/fusion</p>
2
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De Brogile wavelength

-In 1924, de Broglie postulated that because photons have wave and particle characteristics, perhaps all forms of matter have both properties. Nobel Prize: 1929

-Recall the momentum of a photon: 𝑝 = ℎ/𝜆 = h/mV

-The de Broglie wavelength of a particle is related to it’s momentum and therefore kinetic energy

-“Wave-particle duality”

<p>-In 1924, de Broglie postulated that because photons have wave and particle characteristics, perhaps all forms of matter have both properties. Nobel Prize: 1929</p><p>-Recall the momentum of a photon: 𝑝 = ℎ/𝜆 = h/mV</p><p>-The de Broglie wavelength of a particle is related to it’s momentum and therefore kinetic energy</p><p>-“Wave-particle duality”</p>
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what does and doesn’t de Brogile’s wavelength apply to?

-does apply to microscopic objects

-does NOT apply to macroscopic objects

4
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pico

10^-12

5
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Any particle can be diffracted with an appropriate

speed and appropriate slit size!

-Davisson and Germer (1925) first showed this with electrons while studying crystalline nickel.

  • bright rings=CI; dark rings=DI

  • rings same location, so electrons act like waves

  • uses: microscopes w/ electrons, use space between atoms (like distance between slits); atomic level detail

<p>speed and appropriate slit size!</p><p>-Davisson and Germer (1925) first showed this with electrons while studying crystalline nickel.</p><ul><li><p>bright rings=CI; dark rings=DI</p></li><li><p>rings same location, so electrons act like waves</p></li><li><p>uses: microscopes w/ electrons, use space between atoms (like distance between slits); atomic level detail</p></li></ul><p></p>
6
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electron microscopes

-Can probe sizes of order of a pico-meter (pm = 10-12 m) without using harmful x-rays (*bc use electrons)

-Create surface maps of tissue or inorganic materials down to atomic level detail!

-Not much voltage required to get the elections to the needed speed. (*much safer)

<p>-Can probe sizes of order of a pico-meter (pm = 10-12 m) without using harmful x-rays (*bc use electrons)</p><p>-Create surface maps of tissue or inorganic materials down to <strong>atomic level detail!</strong></p><p><strong>-Not much voltage</strong> required to get the elections to the needed speed. (*much safer)</p>
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box model

-1993, IBM: 48 iron atom “fence” is 7.13 nm in radius

-can move individual atoms

-peak=single Fe atom

-1 electron trapped in middle creates wave; trapped particles with similar de Brogile wavelengths=acts like a wave, various things become quantized (ex=nucleus)

<p>-1993, IBM: 48 iron atom “fence” is 7.13 nm in radius</p><p>-can move individual atoms</p><p>-peak=single Fe atom</p><p>-1 electron trapped in middle creates wave; trapped particles with similar de Brogile wavelengths=acts like a wave, various things become quantized (ex=nucleus)</p>
8
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relationship number of electrons and emission lines

-increase electrons=increase emission lines (from electrons transitioning between orbits)

<p>-increase electrons=increase emission lines (from electrons transitioning between orbits)</p>
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Bohr’s model of a 1 electron atom

-hydrogen or any atom singly ionized

-a negatively charged electron moves in a stable circular orbit about a positively charged nucleus

-when an electron transitions from one stable orbit to another, the atom’s energy changes and a photon is emitted or absorbed

-electron’s de Brogile wavelength must satisfy (equation)

-quantized

<p>-hydrogen or any atom singly ionized</p><p>-a negatively charged electron moves in a stable circular orbit about a positively charged nucleus</p><p>-when an electron transitions from one stable orbit to another, the atom’s energy changes and a photon is emitted or absorbed</p><p>-electron’s de Brogile wavelength must satisfy (equation)</p><p>-quantized</p>
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Bohr model electron orbits

-a0=Bohr Radius=0.0529nm=r1 (*smallest orbit; doesn’t increase linearly)

-The Bohr Model correctly explains the properties of the electron in the hydrogen atom on average (*varies based on where electron is and radii; reality=not perfect circle and actually electron cloud with probability to be in certain places)

<p>-a0=Bohr Radius=0.0529nm=r1 (*smallest orbit; doesn’t increase linearly)</p><p>-The Bohr Model correctly explains the properties of the electron in the hydrogen atom on average (*varies based on where electron is and radii; reality=not perfect circle and actually electron cloud with probability to be in certain places)</p>
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emission and absorption

-Spontaneous emission of radiation (light) can occur if an electron is in a higher level with an unoccupied level below: 𝐸𝑖𝑒 = 𝐸𝑓𝑒 + 𝐸𝛾.

-The visible light emitted by hydrogen gas corresponds to four transitions to the n=2 state.

  • Transitions to n=1 have small wavelengths (ultraviolet)

  • Transitions to n=3 have larger wavelengths (infrared)

-If a photon comes in with the exact right wavelength (energy) it an be absorbed by an atom: 𝐸𝑖𝑒 + 𝐸𝛾 = 𝐸𝑓𝑒.

-The emission/absorption spectrum can be used to identify what element is in a gas.

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ground state energy of hydrogen

-13.6eV

-increase n=energy closer to zero; at zero=ionized and add 13.6eV

-lowest energy AND most likely state/where electron spends most time

- -3.4eV=first excited state; -1.5eV=2nd excited state, etc.