The Mercury Spectrum, Exercises of Chemistry

In this experiment a spectrometer equipped with a diffraction grating is used to identify spe- cific wavelengths from the emission spectrum of mercury, to ...

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The Mercury Spectrum
Introduction
A spectrometer is an instrument used for studying electromagnetic emissions. In this
experiment a spectrometer equipped with a diffraction grating is used to identify spe-
cific wavelengths from the emission spectrum of mercury, to measure these wave-
lengths precisely, and to compare them to accepted values.
Procedure
Adjust the diffraction grating so that the normal to its plane makes a small angle α
to the incident beam of light. This is shown schematically in Fig. 1. Since αu0,
the angles between the first and zeroth order intensity maxima on either side, θand θ0
respectively, are related to the wavelength λof the incident light according to [1]
λ=dsin(φ),(1)
accurate to first order in α. Here, dis the separation between the slits of the grating,
and
φ=θ0+θ
2(2)
Four visible spectral lines of mercury are depicted in Fig. 2. The accepted values
of their wavelengths and color associations are summarized in Table 1. To determine
the wavelengths of these spectral lines proceed as follows.
1. Turn on the power supply to which is attached the mecury discharge tube.
Color Wavelength [nm]
Violet 435.8
green 546.1
yellow–1 577.0
yellow–2 579.1
Table 1: A summary of wavelengths and color associations of the visible spectral lines
of mercury, as depicted in Fig. 2.
1
pf3
pf4

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The Mercury Spectrum

Introduction

A spectrometer is an instrument used for studying electromagnetic emissions. In this experiment a spectrometer equipped with a diffraction grating is used to identify spe- cific wavelengths from the emission spectrum of mercury, to measure these wave- lengths precisely, and to compare them to accepted values.

Procedure

Adjust the diffraction grating so that the normal to its plane makes a small angle α to the incident beam of light. This is shown schematically in Fig. 1. Since α u 0 , the angles between the first and zeroth order intensity maxima on either side, θ and θ′ respectively, are related to the wavelength λ of the incident light according to [1]

λ = d sin(φ) , (1)

accurate to first order in α. Here, d is the separation between the slits of the grating, and

φ =

θ′^ + θ 2

Four visible spectral lines of mercury are depicted in Fig. 2. The accepted values of their wavelengths and color associations are summarized in Table 1. To determine the wavelengths of these spectral lines proceed as follows.

  1. Turn on the power supply to which is attached the mecury discharge tube.

Color Wavelength [nm] Violet 435. green 546. yellow–1 577. yellow–2 579.

Table 1: A summary of wavelengths and color associations of the visible spectral lines of mercury, as depicted in Fig. 2.

α

θm

θ′ m

θl,m

θr,m

θ 0

Figure 1: A depiction of the m–th maximum for monochromatic light being dispersed by a diffraction grating. The angle α is the angle the normal to the diffraction grat- ing makes with respect to the incident beam of light. The quantity θ 0 is the angular coordinate of the zeroth order maximum. The quantities θl,m and θr,m are the an- gular coordinates of the m–th order maxima to the left and right of the zeroth order maximum.

  1. Align the telescope so that the cross hairs in the eyepiece are centered on the light emerging from the collimator tube. Adjust the platform on which the diffraction grating is placed so that the 0 ◦^ marking on the vernier aligns with an angular marking on the scale between the 35 ◦^ and 325 ◦.^1
  2. Attach the diffraction grating to the platform on the spectrometer.
  3. Attach the diffraction grating to the platform on the spectrometer. The normal to the plane of the grating should be aligned with the direction of the beam, i.e. α should be close to zero. If the diffraction grating is positioned properly, the angles θm and θ′ m are approximately equal, i.e. they should not differ by more than a degree.
  4. Identify the first order maxima of the four visible spectral lines to the left of the collimating tube.
  5. Measure the angles of the violet, green, and yellow–2 lines. Report them as θl in Table 2. Note: Because of the vernier scale angles can be measured to an accuracy of. 1 ◦.
  6. Perform the corresponding measurements for the first order maxima to the right of the collimating tube and report their values as θr. (^1) For some spectrometers, this may not be possible.

θl, 1 [deg] θr, 1 [deg] φ 1 [deg] λexp [nm] λaccepted [nm]

F

Violet

Green

Yellow–

Table 2: Data and Calculations