When the displacement u of a medium is written as a function of position coordinate x and time t, as u ( x , t )= a sin( ωt -κx +δ), this wave is called a sine wave traveling in the positive x direction. Here, a is the amplitude, sin is the sine function, κ= 2πk ,ω=2πν, k =1/λ,ν=1/ T , 2π radians is 360 degrees, κ and k are called wave numbers, k is the inverse of the wavelength λ, ω is the angular frequency, and ν is the frequency which is the inverse of the period T. At a certain position, the medium performs simple harmonic motion with period T. At a certain time t, the displacement of the medium changes sinusoidally with wavelength λ in the x direction, and has spatial periodicity. ( ωt -κx +δ) is the phase of the sine wave, and the phase at time zero, position x0 , is [Yoshiro Kainuma] [Reference] |©Shogakukan "> Sine wave Source: Shogakukan Encyclopedia Nipponica About Encyclopedia Nipponica Information | Legend |
媒質の変位uが、位置座標xと時刻tの関数として、u(x,t)=asin(ωt-κx+δ)と書かれるとき、この波をプラスx方向に進行する正弦波という。ここに、aは振幅、sinは正弦関数、κ=2πk,ω=2πν,k=1/λ,ν=1/T、2πラジアンは360度、κ、kは波数とよばれ、kは波長λの逆数、ωは角振動数、νは振動数で周期Tの逆数である。ある一定の位置においては、媒質は周期Tの単振動をする。ある一定の時刻tにおいては、媒質の変位はx方向に波長λで正弦関数的に変化し、空間的な周期性をもつ。(ωt-κx+δ)は正弦波の位相で、時刻ゼロ、位置x0における位相は、 [飼沼芳郎] [参照項目] |©Shogakukan"> 正弦波 出典 小学館 日本大百科全書(ニッポニカ)日本大百科全書(ニッポニカ)について 情報 | 凡例 |
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