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 |
Kamis, 21 Mei 2015
PERCOBAAN FISIKA MODERN
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