Shortcut Methods

Numerical Problems


1) Work Function and Maximum Wavelength λmax=hcϕ Where,

  • λmax is the maximum wavelength of light in meters (m).
  • h is Planck’s constant (6.626×1034Js).
  • c is the speed of light (3×108m/s).
  • ϕ is the work function in joules (J).

Given:

  • Work function, ϕ=4.2eV=(4.2eV)(1.6×1019J/eV)=6.72×1019J

Calculations λmax=(6.626×1034Js)(3×108m/s)6.72×1019J=292nm


2) Work Function and Stopping Potential eVs=hfϕ Where,

  • eVs is the stopping potential energy in joules (J).
  • h is Planck’s constant (6.626×1034Js).
  • f is the frequency of the incident light in hertz (Hz).
  • ϕ is the work function in joules (J).

Given:

  • Wavelength of light, λ=400nm=400×109m
  • Stopping potential, Vs=0.5V=0.5J/C

Calculations First, calculate the frequency of light using the formula: f=cλ=3×108m/s400×109m=7.5×1014Hz

Now, calculate the work function: eVs=hfϕ ϕ=hfeVs=(6.626×1034Js)(7.5×1014Hz)(0.5J) ϕ=4.97×1019J0.5J=0.000498J=(0.31eV)

Therefore, the work function of the metal is 0.31 eV (negative value indicates that the given wavelength is below the threshold wavelength).


3) Effect of Frequency on Stopping Potential eVs1=hf1ϕ eVs2=hf2ϕ

Dividing the second equation by the first equation:

eVs2eVs1=hf2ϕhf1ϕ

Since ϕ is the same for both frequencies:

Vs2Vs1=f2f1 Given:

  • Stopping potential for frequency f1,Vs1=2V
  • The frequency of light is doubled, f2=2f1

Calculations: Vs22V=2f1f1=2 Vs2=2(2V)=4V

Therefore, the stopping potential will become 4V when the frequency of light is doubled.


4) Stopping Potential and Light Intensity VsI

Where,

  • Vs is the stopping potential in volts (V).
  • I is the intensity of light.

Given:

  • Intensity of light from source 1, I1
  • Intensity of light from source 2, I2=2I1
  • Stopping potential for source 1, Vs1

Calculations As the intensity of light increases, the stopping potential also increases. Since the intensity of light from source 2 is twice the intensity of light from source 1:

Vs2Vs1=I2I1=2I1I1=2

Therefore, the ratio of the stopping potentials is 2, indicating that the stopping potential for source 2 is twice the stopping potential for source 1.


5) Maximum Kinetic Energy of Emitted Photoelectrons Kmax=hfϕ

Where,

  • Kmax is the maximum kinetic energy of emitted electrons in joules (J).
  • h is Planck’s constant (6.626×1034Js).
  • f is the frequency of incident light in hertz (Hz).
  • ϕ is the work function in joules (J).

Given:

  • Wavelength of light, λ=300nm=300×109m
  • Work function, ϕ=2.5eV=(2.5eV)(1.6×1019J/eV)=4.0×1019J

Calculations First, calculate the frequency of light using the formula: f=cλ=3×108m/s300×109m=1015Hz Now, calculate the maximum kinetic energy: Kmax=hfϕ=(6.626×1034Js)(1015Hz)4.0×1019J=2.63×1019J

Therefore, the maximum kinetic energy of emitted photoelectrons is 2.63×1019J


6) Number of Photons n=Ihf Where,

  • n is the number of photons per second.
  • I is the intensity of light in watts (W).
  • h is Planck’s constant (6.626×1034Js).
  • f is the frequency of incident light in hertz (Hz).

Given:

  • Intensity of light, I=1μA=106A
  • Wavelength of light, λ=550nm=550×109m
  • Work function, ϕ=1.8eV=(1.8eV)(1.6×1019J/eV)=2.88×1019J

Calculations First, calculate the frequency of light using the formula: f=cλ=3×108m/s550×109m=5.45×1014Hz

Now, calculate the number of photons per second: n=Ihf=106W(6.626×1034Js)(5.45×1014Hz) n=2.94×1013 photons/s


7) De Broglie Wavelength of Emitted Electrons λ=hp=h2mekmax Where,

  • λ is the de Broglie wavelength of the emitted electrons in meters (m).
  • h is Planck’s constant (6.626×1034Js).
  • me is the mass of an electron (9.109×1031kg).
  • Kmax is the maximum kinetic energy of emitted electrons in joules (J).

Given:

  • Wavelength of incident light, λ=250nm=250×109m
  • Work function, ϕ=4.5eV=(4.5eV)(1.6×1019J/eV)=7.2×1019J

Calculations First, calculate the maximum kinetic energy of emitted electrons using the formula: $$K_{max}=hf−\phi= \frac{hc}{\lambda}-\phi



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