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Maximum Photoelectrons Emitted from Isolated Silver Sphere

A silver sphere of radius 1 cm1\text{ cm} and work function 4.7 eV4.7\text{ eV} is suspended from an insulating thread in free-space. It is under continuous illumination of 200 nm200\text{ nm} wavelength light. As photoelectrons are emitted, the sphere gets charged and acquires a potential. The maximum number of photoelectrons emitted from the sphere is A×10Z\text{A} \times 10^Z (where 1<A<101 < \text{A} < 10). The value of 'ZZ' is

Official Numerical Answer7

Step-by-Step Solution

To find the maximum number of photoelectrons emitted from the isolated silver sphere, we analyze the photoelectric effect and the electrostatic potential acquired by the sphere.

  1. Energy of the Incident Photons:
    The energy of a photon of wavelength λ=200 nm\lambda = 200\text{ nm} is given by:
    E=hcλE = \frac{hc}{\lambda}
    Using standard values:
    hc≈1240 eV⋅nm(or 1242 eV⋅nm)hc \approx 1240\text{ eV}\cdot\text{nm} \quad (\text{or } 1242\text{ eV}\cdot\text{nm})
    E=1240 eV⋅nm200 nm=6.2 eVE = \frac{1240\text{ eV}\cdot\text{nm}}{200\text{ nm}} = 6.2\text{ eV}

  2. Maximum Kinetic Energy of Emitted Photoelectrons:
    The work function of the silver sphere is Φ=4.7 eV\Phi = 4.7\text{ eV}.
    According to Einstein's photoelectric equation, the maximum initial kinetic energy of the emitted photoelectrons is:
    Kmax⁡=E−Φ=6.2 eV−4.7 eV=1.5 eVK_{\max} = E - \Phi = 6.2\text{ eV} - 4.7\text{ eV} = 1.5\text{ eV}

  3. Stopping Condition (Limiting Potential):
    As photoelectrons are emitted, the isolated sphere loses negative charge and acquires a positive charge QQ. Consequently, an electric potential VV develops on the sphere:
    V=14πε0QRV = \frac{1}{4\pi\varepsilon_0}\frac{Q}{R}
    where:

  • R=1 cm=10−2 mR = 1\text{ cm} = 10^{-2}\text{ m} is the radius of the sphere,
  • 14πε0=9×109 N⋅m2/C2\frac{1}{4\pi\varepsilon_0} = 9 \times 10^9\text{ N}\cdot\text{m}^2/\text{C}^2.

Photoemission ceases when the positive potential of the sphere reaches a value such that even the fastest emitted electrons (with kinetic energy Kmax⁡K_{\max}) are pulled back to the sphere. This occurs when the potential VV equals the stopping potential VsV_s:
eVmax⁡=Kmax⁡=1.5 eV  ⟹  Vmax⁡=1.5 Ve V_{\max} = K_{\max} = 1.5\text{ eV} \implies V_{\max} = 1.5\text{ V}

  1. Maximum Charge and Number of Emitted Photoelectrons:
    The maximum positive charge accumulated on the sphere is:
    Qmax⁡=4πε0RVmax⁡Q_{\max} = 4\pi\varepsilon_0 R V_{\max}
    Substituting the given values:
    Qmax⁡=10−2 m×1.5 V9×109 N⋅m2/C2=1.59×10−11 C=16×10−11 C≈1.67×10−12 CQ_{\max} = \frac{10^{-2}\text{ m} \times 1.5\text{ V}}{9 \times 10^9\text{ N}\cdot\text{m}^2/\text{C}^2} = \frac{1.5}{9} \times 10^{-11}\text{ C} = \frac{1}{6} \times 10^{-11}\text{ C} \approx 1.67 \times 10^{-12}\text{ C}

The total number of photoelectrons emitted, nn, corresponds to this charge:
n=Qmax⁡en = \frac{Q_{\max}}{e}
where e=1.6×10−19 Ce = 1.6 \times 10^{-19}\text{ C}.

n=16×10−111.6×10−19=1089.6≈1.04×107n = \frac{\frac{1}{6} \times 10^{-11}}{1.6 \times 10^{-19}} = \frac{10^8}{9.6} \approx 1.04 \times 10^7

  1. Determining the Value of ZZ:
    The question specifies that the maximum number of photoelectrons is written in the form:
    n=A×10Zwith 1<A<10n = \text{A} \times 10^Z \quad \text{with } 1 < \text{A} < 10

Since n≈1.04×107n \approx 1.04 \times 10^7:
A≈1.04andZ=7\text{A} \approx 1.04 \quad \text{and} \quad Z = 7

Thus, the value of ZZ is 77.