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Description of laboratory research facility and methodology of measurementsDevices and outfits: Set of inductances, set of capacities, set of resistances, voltmeter, sound generator ÃÇ-36. In a given work we study capacitor, inductor and resistor voltages dependencies on external driving EMF frequency Ω. Magnitudes of R, C, L and amplitude of driving EMF Em remain constant during the work.
Obviously that effective current and EMF related as If we’ll change the frequency of generator then phase lag between current and EMF also will be changed as the reactance changes. As it seen from (63), (64) and Fig.13, at low frequencies uL < uC and uL > uC at high. Obviously that there will be some frequencies ΩC = ΩL at which uC = uL and get maximum. Using indexes of voltmeter, switched to capacitor or inductance coil we can find frequency ΩC or ΩL, which, in case of high enough quality, will be equal to resonance frequency. So, in this work we can plot: a) Effective voltage on capacitor UC versus driving EMF frequency Ω = 2πν, where ν determined with ÃÇ-36 limb; b) Effective current I = 2πνCUC in a circuit versus Ω; c) Effective voltage on inductor UL = IΩL, or substituting I and Ω, UL = 4π2ν2CUCL. Inductance L can be determined from the match of driving and natural frequencies of the circuit at resonance, i.e.:
4 Data processing (see laboratory work ¹ 4-1).
Date: 2015-12-24; view: 827
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