Kamis, 21 Mei 2015

PERCOBAAN FISIKA MODERN



HARGA PERAlATAN LAB FISIKA MODERN dengan konten LEYBOLD









NO Nama Peralatan Merk     Type
1 Electron Spin Resonance    
1.1 Electron spin resonance at DPPH - determinig the magnetic field as a function of the resonance frequency LEYBOLD     P6.2.6.2
2 Michelson Interferometer    
2.1 Setting up a Michelson interferometer on the laser optics base plate LEYBOLD      P5.3.4.1
2.2 Determining the wavelength of the light of an He-Ne laser using a Michelson interferometer LEYBOLD     P5.3.4.2
2.3 Determining the wavelength of the light of an He-Ne laser using a Michelson interferometer - Set-up on the optical bench LEYBOLD     P5.3.4.3
2.4a Determination of the coherence time and the line width of spectral lines with the Michelson interferometer LEYBOLD      P5.3.4.4_a
2.4b Determination of the coherence time and the line width of spectral lines with the Michelson interferometer LEYBOLD  P5.3.4.4_b
2.5a Investigation of the pressure induced line broadening using a Michelson interferometer LEYBOLD  P5.3.4.5_a
2.5b Investigation of the pressure induced line broadening using a Michelson interferometer LEYBOLD  P5.3.4.5_b
2.6a Determination of the line splitting of two spectral lines using a Michelson interferometer LEYBOLD  P5.3.4.6_a
2.6b Determination of the line splitting of two spectral lines using a Michelson interferometer LEYBOLD  P5.3.4.6_b
3      
4 X-ray scattering    
4.1 Bragg reflection: determining the lattice constants of monocrystals LEYBOLD  P7.1.2.1
4.2 Laue diagrams: investigating the lattice structure of monocrystals LEYBOLD  P7.1.2.2
4.3 Debye-Scherrer photography: determining the lattice plane spacings of polycrystalline powder samples LEYBOLD  P7.1.2.3
5      
6 Determining Planck’s constant    
6.1a Determining Planck’s constant - Selection of wavelengths using interference filters on the optical bench LEYBOLD  P6.1.4.3_a
6.1b Determining Planck’s constant - Selection of wavelengths using interference filters on the optical bench LEYBOLD  P6.1.4.3_b
7 Balmer series of hydrogen    
7.1 Determining the wavelengths Halpha, Hbeta and Hgamma from the Balmer series of hydrogen LEYBOLD  P6.2.1.1
7.2 Observing the Balmer series of hydrogen using a prism spectrometer LEYBOLD  P6.2.1.2
7.3a Observing the splitting of the Balmer series on deuterated hydrogen (isotope splitting) LEYBOLD  P6.2.1.3_a
7.3b Observing the splitting of the Balmer series on deuterated hydrogen (isotope splitting) LEYBOLD  P6.2.1.3_b
8 Normal Zeeman effect    
8.1a Observing the normal Zeeman effect in transverse and longitudinal configuration - spectroscopy using a Fabry-Perot etalon LEYBOLD  P6.2.7.3_a
8.1b Observing the normal Zeeman effect in transverse and longitudinal configuration - spectroscopy using a Fabry-Perot etalon LEYBOLD  P6.2.7.3_b
8.2a Measuring the Zeeman splitting of the red cadmium line as a function of the magnetic field - spectroscopy using a Fabry-Perot etalon LEYBOLD  P6.2.7.4_a
8.2b Measuring the Zeeman splitting of the red cadmium line as a function of the magnetic field - spectroscopy using a Fabry-Perot etalon LEYBOLD  P6.2.7.4_b
9      
10 Dual nature of wave and particle    
10.1 Diffraction of electrons at a polycrystalline lattice (Debye-Scherrer diffraction) LEYBOLD  P6.1.5.1
10.2 Optical analogy to electron diffraction at a polycrystalline lattice LEYBOLD  P6.1.5.2
11 Rutherford Scattering    
11.1 Rutherford scattering: measuring the scattering rate as a function of the scattering angle and the atomic number LEYBOLD  P6.5.2.1
12 Compton effect    
12.1 Quantitative observation of the Compton effect LEYBOLD  P6.5.6.1
13 Hall effect    
13.1 Determining the density and mobility of charge carriers in p-Germanium LEYBOLD  P7.2.1.4
       

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