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Experiment 9

    Line Spectra
(Rydberg’s Constant)


       Younes Sina
Objective

 Use the emission spectrum of hydrogen atom in
  order to verify the relation between energy
  levels and the photon wavelength

 Calculate Rydberg’s constant R = 1.097x107m-1.
Theory
excited state




 When an element is heated strongly

 when a gas at low pressure is subjected to a high electric potential
When an element is heated strongly, or when a gas at low
pressure is subjected to a high electric potential, the element
begins to glow, indicating that it is emitting energy in the
visible region of the spectrum. This arises from electrons that
have absorbed a certain amount of energy and have been
promoted to a higher energy state. When the electrons revert
to a lower energy state, they lose energy by emitting
photons whose energy corresponds to the energy loss, E.

E = hc/λ
Planck's law
E = hc/λ
h : Planck's constant (6.63x10-34 J.s-1)
c : velocity of light in a vacuum (3.00x108 m.s-1)
λ: wavelength of the emitted photon

In the case of hydrogen, the transitions that can occur are shown in the
diagram below:
Only the transitions down to n = 2 have energy values such
that the associated wavelengths occur in the visible region
of the spectrum. These give rise to the so-called Balmer
series of lines, known as an ATOMIC EMISSION SPECTRUM.
The other series occur either in the infrared region
(Lyman), or in the ultraviolet region (Paschen, Brackett,
Pfund). These series are named after their discoverers.
Goal

Reading absorption spectrum of hydrogen atom using cold hydrogen tube


Reading wavelengths at which the dark lines appear


Reading spectral emission lines in the spectroscope using hot hydrogen tube


Observing spectral emission lines in the spectroscope using hot helium tube
Calculations
 Use the Balmer Series equation to calculate R for each of the
  measured wavelengths. Next, find the average value of R. It
  gives the measured value for R.

 Calculate a %error on R using the usual %error formula.




   λ62 = ? nm, λ52 = ? nm, λ42 = ? nm, λ32 = ? nm,
                                                     Raccepted = 1.097x107m-1

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Line Spectra (Rydberg’s Constant)

  • 1. Experiment 9 Line Spectra (Rydberg’s Constant) Younes Sina
  • 2. Objective  Use the emission spectrum of hydrogen atom in order to verify the relation between energy levels and the photon wavelength  Calculate Rydberg’s constant R = 1.097x107m-1.
  • 3. Theory excited state  When an element is heated strongly  when a gas at low pressure is subjected to a high electric potential
  • 4. When an element is heated strongly, or when a gas at low pressure is subjected to a high electric potential, the element begins to glow, indicating that it is emitting energy in the visible region of the spectrum. This arises from electrons that have absorbed a certain amount of energy and have been promoted to a higher energy state. When the electrons revert to a lower energy state, they lose energy by emitting photons whose energy corresponds to the energy loss, E. E = hc/λ
  • 5. Planck's law E = hc/λ h : Planck's constant (6.63x10-34 J.s-1) c : velocity of light in a vacuum (3.00x108 m.s-1) λ: wavelength of the emitted photon In the case of hydrogen, the transitions that can occur are shown in the diagram below:
  • 6. Only the transitions down to n = 2 have energy values such that the associated wavelengths occur in the visible region of the spectrum. These give rise to the so-called Balmer series of lines, known as an ATOMIC EMISSION SPECTRUM. The other series occur either in the infrared region (Lyman), or in the ultraviolet region (Paschen, Brackett, Pfund). These series are named after their discoverers.
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  • 15. Goal Reading absorption spectrum of hydrogen atom using cold hydrogen tube Reading wavelengths at which the dark lines appear Reading spectral emission lines in the spectroscope using hot hydrogen tube Observing spectral emission lines in the spectroscope using hot helium tube
  • 16. Calculations  Use the Balmer Series equation to calculate R for each of the measured wavelengths. Next, find the average value of R. It gives the measured value for R.  Calculate a %error on R using the usual %error formula. λ62 = ? nm, λ52 = ? nm, λ42 = ? nm, λ32 = ? nm, Raccepted = 1.097x107m-1