In IB we learn that electrons are emitted when light is incident on a metal surface, which is a form of electromagnetic radiation.
CloseFor every material there is a certain frequency of light under which no light is emitted.
CloseThe work function is the energy required to take an electron from the metal. It is the energy that will release an electron such that it will have 0 kinetic energy when at the surface of the metal.
CloseWe can use the conservation of energy to solve this question. Equating the kinetic energy with the loss in potential energy \( \frac{1}{2}mv^2 = eV \). Rearranging for \( v \) gives: \[ v = \sqrt{\frac{2Ve}{m}} \]
CloseLouis de Broglie proposed that all matter exhibits wave-like behavior, not just electrons or high-energy particles. This wave-particle duality applies to all particles, meaning every particle, from electrons to protons, has an associated matter wave.
CloseIf their de Broglie wavelengths are equal, then \(\frac{h}{p_p} = \frac{h}{p_a}\). This simplifies to \(\frac{1}{m_p v_p} = \frac{1}{m_a v_a}\). Knowing that the mass of an alpha particle is four times that of a proton, its speed must be one-fourth the proton's speed to maintain the same momentum. Thus, the ratio \(\frac{v_{\text{proton}}}{v_{\text{alpha}}} = 4\).
CloseThe correct answer is: A.
The energy of the photons is given by: \[ E = hf \] where \( h = 6.63 \times 10^{-34} \: \mathrm{Js} \), and \( f = 6.0 \times 10^{14} \: \mathrm{Hz} \). Substituting: \[ E = (6.63 \times 10^{-34})(6.0 \times 10^{14}) = 3.978 \times 10^{-19} \: \mathrm{J} \] Converting to electron volts: \[ E = \frac{3.978 \times 10^{-19}}{1.6 \times 10^{-19}} \approx 2.49 \: \mathrm{eV} \] The maximum kinetic energy is given by: \[ K.E. = E - \phi = 2.49 - 2 \approx 0.5 \: \mathrm{eV} \]
CloseThe correct answer is: C.
Electrons are emitted only if the frequency of the incident light is greater than or equal to the threshold frequency. Since \( 3.0 \times 10^{14} \: \mathrm{Hz} < 4.0 \times 10^{14} \: \mathrm{Hz} \), no electrons are emitted.
CloseThe correct answer is: A.
The de Broglie wavelength is given by: \[ \lambda = \frac{h}{p} \] where \( h = 6.63 \times 10^{-34} \: \mathrm{Js} \), and \( p = mv = (9.1 \times 10^{-31})(2.0 \times 10^6) = 1.82 \times 10^{-24} \: \mathrm{kg \cdot m/s} \). Substituting: \[ \lambda = \frac{6.63 \times 10^{-34}}{1.82 \times 10^{-24}} \approx 3.6 \times 10^{-10} \: \mathrm{m} \]
CloseThe correct answer is: D.
The wavelength shift is given by the Compton formula: \[ \Delta \lambda = \frac{h}{m_e c}(1 - \cos\theta) \] where \( h = 6.63 \times 10^{-34} \: \mathrm{Js} \), \( m_e = 9.11 \times 10^{-31} \: \mathrm{kg} \), \( c = 3.0 \times 10^8 \: \mathrm{m/s} \), and \( \theta = 90^\circ \). Substituting: \[ \Delta \lambda = \frac{(6.63 \times 10^{-34})}{(9.11 \times 10^{-31})(3.0 \times 10^8)}(1 - \cos90^\circ) \] \[ \Delta \lambda \approx 0.0024 \: \mathrm{nm} \]
CloseThe correct answer is: C.
Electron diffraction, such as through a crystal lattice, demonstrates the wave nature of electrons as it produces an interference pattern, which is a property of waves.
CloseOption | Maximum K.E. (\( \mathrm{eV} \)) |
---|---|
A | 0.5 |
B | 1.0 |
C | 2.0 |
D | 2.5 |
Option | Observation |
---|---|
A | Electrons are emitted with zero kinetic energy. |
B | Electrons are emitted with nonzero kinetic energy. |
C | No electrons are emitted. |
D | The metal is heated but no electrons are emitted. |
Option | Wavelength (\( \mathrm{m} \)) |
---|---|
A | \( 3.6 \times 10^{-10} \) |
B | \( 1.1 \times 10^{-10} \) |
C | \( 6.6 \times 10^{-10} \) |
D | \( 2.7 \times 10^{-10} \) |
Option | Wavelength Shift (\( \mathrm{nm} \)) |
---|---|
A | \( 0.0010 \) |
B | \( 0.0049 \) |
C | \( 0.0024 \) |
D | \( 0.0036 \) |
Option | Observation |
---|---|
A | Photoelectric effect |
B | Compton scattering |
C | Electron diffraction |
D | Rutherford scattering |