Frank-Hertz Experiment & Photoelectric Effect Simulation
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Observe the quantized energy levels of mercury atoms by measuring the current through the tube at different accelerating voltages.
| Voltage (V) | Current (µA) | Peak Number | Energy (eV) |
|---|
Investigate how the kinetic energy of emitted photoelectrons varies with the frequency of incident light.
| Wavelength (nm) | Frequency (×10¹⁴ Hz) | Stopping Potential (V) | Current (nA) | Kinetic Energy (eV) |
|---|
Objective: To demonstrate the existence of discrete energy levels in atoms by measuring the kinetic energy lost by electrons during inelastic collisions with mercury atoms.
Theory: The Frank-Hertz experiment shows that electrons occupy only discrete, quantized energy states. When electrons are accelerated through a mercury vapor-filled tube, they undergo elastic collisions until they acquire sufficient energy to excite a mercury atom (4.9 eV). This results in a drop in current, which occurs periodically as the voltage increases.
Procedure:
Calculations: The first excitation energy is calculated by finding the average voltage difference between successive current peaks and converting to electronvolts (eV).
Objective: To verify the particle nature of light and determine Planck's constant by measuring the stopping potential for different frequencies of light.
Theory: The photoelectric effect occurs when photons of sufficient energy strike a metal surface, ejecting electrons. The maximum kinetic energy of the ejected electrons is given by K.E. = hν - φ, where h is Planck's constant, ν is the frequency of light, and φ is the work function of the material.
Procedure:
Calculations: Planck's constant is calculated from the slope of the stopping potential vs. frequency graph. The work function is determined from the intercept on the potential axis.