तरंग-संख्या हिंदी उपयोग और उदाहरण

स्पेक्ट्रम के जिन बैंडशीर्षों की तरंग संख्याएँ एक ही सारणी में रखी जा सकती हैं, वे सभी बैंड मिलकर एक बैंडप्रणाली (band system) बनाते हैं।

कोष्टक में पहले 'तरंग संख्या और फिर श्लोक संख्या लिखी गयी है, जैसे (IV.678) का अर्थ है तरंग ४ एवं श्लोक 678।

संगठित अणुओं का फिंगरप्रिंट क्षेत्र 500-2000 सेमी−1 (तरंग संख्या में) के बीच होता है।

कोणीय तरंग संख्या (Angular wave number)।

""k – तरंग संख्या (wave number), k\frac{2\pi} \lambda \, ।

तरंग-संख्या इसके अंग्रेजी अर्थ का उदाहरण

The wave number k is the absolute of the wave vector k q / \hbar and is related to the wavelength k 2\pi / \lambda.

Bragg diffraction occurs on the atomic crystal lattice, conserves the wave energy and thus is called elastic scattering, where the wave numbers final and incident particles, k_f and k_i, respectively, are equal and just the direction changes by a reciprocal lattice vector G Q k_f - k_i with the relation to the lattice spacing G 2\pi / d .

Likewise, the angular wave number k, measured in rad per m, is related to spatial frequency and wavelength by.

where the wave number or propagation constant kn of each harmonic is expressed as.

Here u_{n\boldsymbol{k}}(\boldsymbol{r}) is a function with the same periodicity as the crystal, n is the band index and k is the wave number.

The allowed wave numbers for a given potential are found by applying the usual Born–von Karman cyclic boundary conditions.

A surface state is described by the energy E_s and its wave vector \textbf{k}_{||} parallel to the surface, while a bulk state is characterized by both \mathbf{k}_{||} and \mathbf{k}_\perp wave numbers.

Motivated by a 1958 paper by Owen Philips that described a universal spectral form for the variance of ocean surface waves as a function of wave number, Chris Garrett and Munk attempted to make sense of the observations by postulating a universal spectrum for internal waves.

According to Munk, they chose a spectrum that could be factored into a function of frequency times a function of vertical wave number.

) The shortest wavelength needed to describe a wavemotion in the lattice is equal to 2a which then corresponds to the largest needed wave number k_{max}\pi/a and which also corresponds to the maximum possible |n|: n_{max}L/2a.