HOAN,N,. dt HOAN,N2 dl 2nfl, cos(2nft) =- 8.8 However, our measuring devices indicate only effective values of altemating quantities. This effective value is defined as square root of square average of the original signal over one period T = 1/f After straightforward calculation, we find the following relation between measurable quantities: U. - AN2fl. 8.9 In this experiment, we will investigate the effective current strength (1,), frequency (f ), number of winding (N2) and cross sectional area (A ) dependence of induced voltage.
HOAN,N,. dt HOAN,N2 dl 2nfl, cos(2nft) =- 8.8 However, our measuring devices indicate only effective values of altemating quantities. This effective value is defined as square root of square average of the original signal over one period T = 1/f After straightforward calculation, we find the following relation between measurable quantities: U. - AN2fl. 8.9 In this experiment, we will investigate the effective current strength (1,), frequency (f ), number of winding (N2) and cross sectional area (A ) dependence of induced voltage.
Classical Dynamics of Particles and Systems
5th Edition
ISBN:9780534408961
Author:Stephen T. Thornton, Jerry B. Marion
Publisher:Stephen T. Thornton, Jerry B. Marion
Chapter3: Oscillations
Section: Chapter Questions
Problem 3.37P
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