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During a photoelectric investigation, a packet of light energy, A, of 4,8 x 10⁻¹⁹ J is shone onto a metal surface, as shown in the diagram below. The metal surface has a threshold frequency of 8,1 x 1014 Hz.

Physics

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Answer

10.4

7.12×105 m/s7.12 \times 10^5 \text{ m/s}

Step-by-step solution

4 steps

Part 10.1

The term for the underlined phrase "a packet of light energy" is a *photon

Part 10.2

Threshold frequency is the minimum frequency of incident light required to eject electrons from the surface of a metal.

Part 10.3· 2 steps

  1. Calculate the work function (ϕ\phi) of the metal using the threshold frequency (f0f_0).

    The work function is given by the formula ϕ=hf0\phi = h f_0, where hh is Planck's constant (6.626×10−346.626 \times 10^{-34} J⋅\cdots).

    ϕ=(6.626×10−34 J⋅s)×(8.1×1014 Hz)\phi = (6.626 \times 10^{-34} \text{ J}\cdot\text{s}) \times (8.1 \times 10^{14} \text{ Hz}) ϕ=5.36906×10−19 J\phi = 5.36906 \times 10^{-19} \text{ J}
  2. Compare the energy of light packet A (EAE_A) with the work function (ϕ\phi).

    Given EA=4.8×10−19E_A = 4.8 \times 10^{-19} J.
    Since EA<ϕE_A < \phi (4.8×10−19 J<5.36906×10−19 J4.8 \times 10^{-19} \text{ J} < 5.36906 \times 10^{-19} \text{ J}), the energy of light A is not sufficient to eject an electron.
    Answer: NO

Part 10.4

7.12×105 m/s7.12 \times 10^5 \text{ m/s}

  1. Calculate the maximum kinetic energy (KmaxK_{max}) of the ejected photoelectrons using the photoelectric effect equation.

    The energy of light packet B is EB=7.68×10−19E_B = 7.68 \times 10^{-19} J. The work function ϕ=5.36906×10−19\phi = 5.36906 \times 10^{-19} J (from 10.3).

    EB=ϕ+KmaxE_B = \phi + K_{max} Kmax=EB−ϕK_{max} = E_B - \phi Kmax=(7.68×10−19 J)−(5.36906×10−19 J)K_{max} = (7.68 \times 10^{-19} \text{ J}) - (5.36906 \times 10^{-19} \text{ J}) Kmax=2.31094×10−19 JK_{max} = 2.31094 \times 10^{-19} \text{ J}
  2. Calculate the maximum speed (vmaxv_{max}) using the maximum kinetic energy.

    The formula for kinetic energy is Kmax=12mevmax2K_{max} = \frac{1}{2} m_e v_{max}^2, where mem_e is the mass of an electron (9.11×10−319.11 \times 10^{-31} kg).

    vmax=2Kmaxmev_{max} = \sqrt{\frac{2 K_{max}}{m_e}} vmax=2×(2.31094×10−19 J)9.11×10−31 kgv_{max} = \sqrt{\frac{2 \times (2.31094 \times 10^{-19} \text{ J})}{9.11 \times 10^{-31} \text{ kg}}} vmax=4.62188×10−199.11×10−31v_{max} = \sqrt{\frac{4.62188 \times 10^{-19}}{9.11 \times 10^{-31}}} vmax=5.0734138×1011v_{max} = \sqrt{5.0734138 \times 10^{11}} vmax=7.12278×105 m/sv_{max} = 7.12278 \times 10^5 \text{ m/s}

    Rounding to three significant figures:

    vmax=7.12×105 m/sv_{max} = \boxed{7.12 \times 10^5 \text{ m/s}}

Part 10.5

The maximum speed of the ejected photoelectrons will REMAIN THE SAME.

Part 10.6

The maximum kinetic energy (and thus maximum speed) of the ejected photoelectrons depends on the energy of individual photons (which is determined by their frequency) and the work function of the metal. The intensity of light relates to the number of photons incident per unit time, not the energy of each individual photon. Therefore, decreasing the intensity will decrease the number of ejected electrons (photoelectric current) but will not change their maximum kinetic energy or speed, as long as the frequency of the light remains constant.

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