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Model No: HO-ED-S-04A

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Holmarc’s Zeeman Effect Apparatus, Model: HO-ED-S-04A is designed for the determination of e/m ratio, which requires knowledge in optics, mechanics, electromagnetism, modern physics and computer operations. Traditional Zeeman effect apparatus needs more skills in operation and measurement. With its new and integrated design, this device is easier to setup and operate so that students can lay focus in understanding the principles and theories involved.

A low-pressure mercury lamp is placed inside a variable current electro-magnet. Radiation passes through a narrow-band interference filter (or Dye based filter), centered around the desired wavelength and enters the Fabry-Perot etalon. This device consists of two reflective parallel plates which serve to transmit strong incoming radiation at different orders of wavelength. The apparatus has a built-in minimum separation D = 3.995 mm. Small tilting knobs allow careful adjustment of the plate.

The significant difference in our setup is in the imaging system used for viewing and recording the interference patterns. We use a USB 2.0 camera, it can be directly connected to the PC to monitor the fringe pattern and can save desired pictures. This makes the alignment of the optics much easier and eliminates the need for photographic processing. The Fabry-Perot etalon is the heart of the apparatus which allows us to detect small shifts in wavelengths of light emitted from the source. Basically, it is a pair of parallel highly reflective mirrors separated by a distance.

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To find Spacing of the etalon
Calibration of the magnetic field
Verification of the magnetic moment constant Bohr magneton ( μ0 )
Analysis of Plank’s constant ( h ) and speed of light ( c ) using Zeeman Effect.
Mechanical Hardware
Optical Rail
Length: 500mm
Model No: HO-ED-RL-HC2-500
Quantity : 1no.
Gauss Prob Mount
Model No: HO-ED-GPM-01
Quantity : 1no.
IR Filter Mount
Model No: HO-ED-IFM-01
Quantity : 1no.
Green Filter Mount
Model No: HO-ED-GFM-01
Quantity : 1no.
Polarizer Rotator with Mount
Model No: HO-ED-PR-01
Quantity : 1no.
CCD Camera Mount
Model No: HO-ED-CCDM-01
Quantity : 1no.
Rail Carriage
Model No: HO-ED-RLC-HC2-25
Quantity : 5nos.
Optical Components
Fabri-Perot Etalon
Model No: HO-ED-INT-FPE-02
Quantity : 1no.
IR Filter
Model No: HO-IRF-01
Quantity : 1no.
Green Filter
Model No: HO-GF-01
Quantity : 1no.
Detectors
CCD Camera with
USB 2.0 Connectivity
Model No: HO-ED-CCD-01
Quantity : 1no.
Light Sources
Mercury Tube
with Power supply
Model No: HO-LH-MT-01
Quantity : 1no.
Electrical & Electronic Devices
Electromagnet
with Power supply
Model No: HO-ED-EMP-02
Quantity : 1no.
Gauss Meter
Model No: HO-ED-GM-01
Quantity : 1no.
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In this experimental setup, the spectrum produced by atom in the magnetic field is resolved by Fabry-Perot etalon. Fringe width changes in an external magnetic field are noted and e/m ratio can be calculated.

• Determination of electron charge/mass ratio from Zeeman effect and the calculation of energy shift due to the applied magnetic field.

Important Features

Mercury lamp is used as light source. No special and costly light sources like Cadmium lamp required. Zeeman effect from a common and familiar light source helps students to understand the phenomena better.

A CCD camera is used to capture the real time image of spectrum from etalon and can be viewed from a computer monitor. The images saved in the computer at various magnetic fields are used for analysis and calculations.

The equipment is easy to be maintained. All modules and components are locally available.

Modules in the Zeeman Effcet Apparatus
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High power electro-magnet with power supply.
Gauss meter along with sensor.
Mercury lamp.
Mounted filters and ploarizers.
Fabry- Perot etalon.
CCD camera and software.
Rail and carriage based mechanical mounts for all optics.
Notebook computer (optional inclusion)
The apparatus can be used to study normal Zeeman shift of the spectral lines of mercury at λ = 546nm, in fields up to 1.6k Gauss at 10mm gap. The experiment starts with calibration of electromagnet. Thereafter, optical system is aligned to observe the circular fringes on the computer monitor due to the interference of green light from mercury lamp at the FP etalon. As the magnetic field is increased, the splitting can be observed in real time on the monitor. Images at different magnetic fields are saved in the computer for calculations. Bohr magnetron constant and the e/m ratio are determined from the experiment.

The technique employed for studying Zeeman effect in this apparatus is a spectroscopic method with CCD imaging. Fabry-Perot etalon is used for obtaining interference spectra of split wavelengths. As the magnetic field is varied, Zeeman effect in wavelength shift can be observed.

A typical image produced by the experiment. This image was taken at 0T on the 546nm line. This image was taken at 1.6T on the 546nm line. Energy level diagram of 7S → 6P transitions
 
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