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module concept Qs
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A. outgoing, large
B. outgoing, small
C. incoming, large
D. incoming, small
E. None of the above
C. incoming, large
A. No, as it would be harder to accelerate them and make them stay on path.
B. Only at night.
C. It depends.
D. Yes, otherwise the ejected electrons interact with molecules in the air.
D. Yes, otherwise the ejected electrons interact with molecules in the air.
A. Yes, electrons are always ejected.
B. Yes, if the incoming light has insufficient energy then electrons are ejected.
C. No, if the incoming light has insufficient energy then no electrons are ejected.
D. No, no electrons will be ejected under any conditions
E. None of the above
C. No, if the incoming light has insufficient energy then no electrons are ejected.
A. No, because in this experiment light is not acting like a wave. If light were acting like a wave then the intensity would be proportional to the size (amplitude) of the wave and the bigger the wave the greater its energy.
B. No, because decreasing the intensity of the light increases the number of electrons being ejected.
C. Yes, because of increasing the intensity of the light increases the number of electrons being ejected.
D. Yes, because in this experiment light is acting like a wave.
E. None of the above
A. No, because in this experiment light is not acting like a wave. If light were acting like a wave then the intensity would be proportional to the size (amplitude) of the wave and the bigger the wave the greater its energy.
A. E (photon) > 0
B. E (photon) < E (remove e-)
C. E (photon) = E (remove e-)
D. E (photon) > E (remove e-)
E. C and D
E. C and D
A. E (photon) – E (remove e-) = E (excess)
B. E (photon) – E (remove e-) = EK (e-)
C. hv - work function = 1/2mv2
D. λv = c
E. None of the above
D. λv = c
A. Measure how much energy is required to remove an electron from a metal surface.
B. Measure how much energy is required to add an electron to a metal surface.
C. Measure how much free energy is released to remove an electron from a metal surface.
D. Measure how much free energy is released to add an electron to a metal surface.
E. None of the above
A. Measure how much energy is required to remove an electron from a metal surface.
A. If electrons were ejected decreasing the light intensity resulted in no ejected electrons.
B. If electrons were ejected increasing the light intensity resulted in no ejected electrons.
C. If no electrons were ejected decreasing the light intensity resulted in ejected electrons.
D. If no electrons were ejected increasing the light intensity still resulted in no ejected electrons.
E. None of the above
D. If no electrons were ejected increasing the light intensity still resulted in no ejected electrons.
A. Use shorter wavelength or higher frequency light.
B. Use shorter wavelength or lower frequency light.
C. Use longer wavelength or higher frequency light.
D. Use longer wavelength or lower frequency light.
E. None of the above
A. Use shorter wavelength or higher frequency light.
A. particle, wave
B. particle, interaction
C. wave, particle
D. wave, photon
E. None of the above
C. wave, particle
A. Ultraviolet
B. Infrared
C. Visible light
D. Gamma rays
A. Ultraviolet
A. Light with many wavelengths is shone on the hydrogen sample. A detector measures wavelengths of light which are absorbed or emitted by the hydrogen atoms.
B. Light with many wavelengths is shone on the hydrogen sample. A detector measures the wavelengths of reflected light.
C. Light with many wavelengths is shone on the hydrogen sample. A detector measures the frequencies of light absorbed or emitted which vary due to the different speeds of the hydrogen atoms.
D. Light with many wavelengths is shone on the hydrogen sample. A detector measures the wavelengths of scattered light.
A. Light with many wavelengths is shone on the hydrogen sample. A detector measures wavelengths of light which are absorbed or emitted by the hydrogen atoms.
A. Atomic absorption spectroscopy; Emission line spectrum
B. Atomic emission spectroscopy; Absorption line spectrum
C. Atomic absorption spectroscopy; Absorption line spectrum
D. Atomic emission spectroscopy; Emission line spectrum
C. Atomic absorption spectroscopy; Absorption line spectrum
A. Atomic absorption spectroscopy; Emission line spectrum
B. Atomic emission spectroscopy; Absorption line spectrum
C. Atomic absorption spectroscopy; Absorption line spectrum
D. Atomic emission spectroscopy; Emission line spectrum
D. Atomic emission spectroscopy; Emission line spectrum
A. All wavelengths of light are absorbed or emitted. Spectrum consists of lines.
B. No wavelengths of light are absorbed or emitted. Spectrum consists of waves.
C. Only specific wavelengths of light are absorbed or emitted. Spectrum consists of lines.
D. Only specific wavelengths of light are absorbed or emitted. Spectrum consists of waves.
C. Only specific wavelengths of light are absorbed or emitted. Spectrum consists of lines.
A. We mean that a photon with a specific energy lowers the energy of the electron in the hydrogen atom to its ground state. That is, the photon's energy matches the energy difference between two electronic energy levels.
B. We mean that a photon with a specific energy absorbs the energy of the electron in the hydrogen atom to a higher energy level. That is, the photon's energy matches the energy product of the two electronic energy levels.
C. We mean that a photon with a specific energy excites the electron in the hydrogen atom to a lower energy level. That is, the photon's energy matches the energy sum of two electronic energy levels.
D. We mean that a photon with a specific energy excites the electron in the hydrogen atom to a higher energy level. That is, the photon's energy matches the energy difference between two electronic energy levels.
D. We mean that a photon with a specific energy excites the electron in the hydrogen atom to a higher energy level. That is, the photon's energy matches the energy difference between two electronic energy levels.
A. Bohr, v = ∆E/h, frequency of the absorbed light, energy difference between the electronic energy levels, Plank constant
B. Boltzmann, v = ∆E/h, velocity of the absorbed light, energy difference between the atomic energy levels, Plank constant
C. Planck, h = ∆E/v, frequency of the absorbed light, energy difference between the electronic energy levels, Boltzmann constant
D. Rutherford, v = ∆E/h, wavelength of the absorbed light, energy difference between the minimum and maximum energy levels, Plank constant.
A. Bohr, v = ∆E/h, frequency of the absorbed light, energy difference between the electronic energy levels, Plank constant