Physics & Material Science Lab Experiments

Physics & Material Science Lab Experiments

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Determination of Hall co-efficient

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₹2.0

AIM:  Determination of Hall co-efficient Apparatuses Required : (A)  Electromagnet  - (12mm Air Gap): 7.5 Killo gauss(B)  Electromagnet Power Supply : 5A 0 - 60V DC(C) Hall Effect Set-up cum Gauss Meter : Digital (D) Hall Probe (E) Gauss Probe (F) Probe Stand(G) Connecting Wires ..

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Dependance of Hall Coefficienton Temperature

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₹2.0

Dependance of Hall Coefficient on TemperatureApparatuses Required : (A)  Electromagnet  - (12mm Air Gap): 7.5 Killo gauss(B)  Electromagnet Power Supply : 5A 0 - 60V DC(C) Hall Effect Set-up cum Gauss Meter : Digital(D) Hall Probe - Temperature type(E) Gauss Probe(F) Probe Stand(G) Connecting W..

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E/M BY HELICAL METHOD

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E/M BY HELICAL METHOD Experimental Training Board has been designed specifically to determine e/m by Helical Method. The board is absolutely self contained and requires no other apparatus. Practical experience on this board carries great educative value for Science and Engineering Students. ..

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E/M BY MAGIC EYE METHOD

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E/M BY MAGIC EYE METHOD..

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E/M BY MAGNETRON VALVE METHOD

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₹2.0

E/M BY MAGNETRON VALVE METHOD..

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E/M BY SHORT SOLENOID METHOD

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E/M BY SHORT SOLENOID METHOD..

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E/M BY THOMSON METHOD

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E/M BY THOMSON METHOD..

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Electron Spin Resonance Spectrometer

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₹2.0

Electron Spin Resonance SpectrometerFeaturesFET based marginal R.F. OscillatorDigital diaplay of frequencyExcellent peaks displayDigital display of Helmoltz Coil CurrentCompatible with general pupose CRO in X-Y modeIntroductionIn recent years Magnetic Resonance has developed into a very useful and powerful tool in solid state research. In this meth..

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Four Probe Apparatus

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₹10,900.0

Resistivity and Band Gap Measurement of semiconductor is a versatile and useful system for physics and basic electronics laboratories. Band Gap can be measured by using Four Probe Method. This is one of the widely used methods for measuring the Resistivity and Band Gap of semiconductors. A collinear four-pr..

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Frank Hertz Experiment

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Frank Hertz ExperimentIntroduction  From the early spectroscopic work it is clear that atoms emitted radiation at discrete frequencies; from Bohr’s model, the frequency of the radiation n is related to the change of energy levels through DE=hn. It is then to be expected that transfer of energy to atomic electrons by any mechanism sho..

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Gouys 's Method Measurement of Susceptibility of Paramagnetic Solids

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₹64,802.0

Gouys 's MethodApparatus for Measurement of Susceptibility of Paramagnetic Solids by Gouy’s MethodIn the Gouy’s method of susceptibility measurement, the solid sample in the form of a long cylinder (area of cross section A) is hung from the pan of a balance and is placed such that one end of the sample is between the pole-pieces of the magnet (fiel..

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Hall Effect Experiment

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Hall Effect ExperimentAIM:  Determination of Hall co-efficientApparatuses Required : (A)  Electromagnet  - (12mm Air Gap): 7.5 Killo gauss(B)  Electromagnet Power Supply : 5A 0 - 60V DC(C) Hall Effect Set-up cum Gauss Meter : Digital(D) Hall Probe(E) Gauss Probe(F) Probe Stand(G) Connectin..

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Hall Effect in Metals

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Hall Effect in Metals..

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Ionization Potential Set-Up

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Ionization Potential Set-UpIntroduction  The electrons in the atoms have discrete stationary states. Franck and Hertz in 1914 describes the first observation of quantized excitation from one quantized state to another one year after N. Bohr published his theory of hydrogen atom. His method depends on detecting the on-set of inelastic coll..

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Magnetic Field Measurement Apparatus

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Magnetic Field Measurement Apparatus..

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