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(window.webpackJsonp=window.webpackJsonp||[]).push([[6],{"2QOB":function(e,n,t){"use strict";t.r(n),function(e){function l(){var e=Sn(["E_{fotone} = h cdot f"],["E_{fotone} = h \\cdot f"]);return l=function(){return e},e}function a(){var e=Sn(["lambda_{max} cdot T"],["\\lambda_{max} \\cdot T"]);return a=function(){return e},e}function i(){var e=Sn(["lambda"],["\\lambda"]);return i=function(){return e},e}function r(){var e=Sn(["1 eV"]);return r=function(){return e},e}function o(){var e=Sn(["10^1 eV"]);return o=function(){return e},e}function u(){var e=Sn(["E_n = \frac{1}{n^2} cdot E_1 = - \frac{1}{n^2} cdot \frac{a_0^2}{2 cdot m cdot hbar^4} = - \frac{1}{n^2} cdot \frac{m_{elettrone} cdot k^2 cdot e^4}{2 cdot hbar^2}"],["E_n = \\frac{1}{n^2} \\cdot E_1 = - \\frac{1}{n^2} \\cdot \\frac{a_0^2}{2 \\cdot m \\cdot \\hbar^4} = - \\frac{1}{n^2} \\cdot \\frac{m_{elettrone} \\cdot k^2 \\cdot e^4}{2 \\cdot \\hbar^2}"]);return u=function(){return e},e}function c(){var e=Sn(["a_0 = left ( \frac{h}{2 pi} \right )^2 cdot \frac{1}{m_{elettrone} cdot k cdot e^2} = 5.29 cdot 10^{-11} m"],["a_0 = \\left ( \\frac{h}{2 \\pi} \\right )^2 \\cdot \\frac{1}{m_{elettrone} \\cdot k \\cdot e^2} = 5.29 \\cdot 10^{-11} m"]);return c=function(){return e},e}function s(){var e=Sn(["r_n = n^2 cdot a_0 = n^2 cdot \frac{hbar}{m_{elettrone} cdot k cdot e^2} "],["r_n = n^2 \\cdot a_0 = n^2 \\cdot \\frac{\\hbar}{m_{elettrone} \\cdot k \\cdot e^2} "]);return s=function(){return e},e}function p(){var e=Sn(["m cdot v_n cdot 2 pi cdot r = n cdot h"],["m \\cdot v_n \\cdot 2 \\pi \\cdot r = n \\cdot h"]);return p=function(){return e},e}function d(){var e=Sn(["hbar = left ( \frac{h}{2 pi} \right )"],["\\hbar = \\left ( \\frac{h}{2 \\pi} \\right )"]);return d=function(){return e},e}function f(){var e=Sn(["h"]);return f=function(){return e},e}function v(){var e=Sn(["n"]);return v=function(){return e},e}function m(){var e=Sn(["R = 1.097 cdot 10^7 \frac{1}{m}"],["R = 1.097 \\cdot 10^7 \\frac{1}{m}"]);return m=function(){return e},e}function g(){var e=Sn(["\frac{1}{lambda} = R left ( \frac{1}{4} - \frac{1}{n^2} \right )"],["\\frac{1}{\\lambda} = R \\left ( \\frac{1}{4} - \\frac{1}{n^2} \\right )"]);return g=function(){return e},e}function _(){var e=Sn(["phi"],["\\phi"]);return _=function(){return e},e}function h(){var e=Sn(["omega"],["\\omega"]);return h=function(){return e},e}function z(){var e=Sn(["\frac{2 pi}{lambda} = left | \vec{k} \right |"],["\\frac{2 \\pi}{\\lambda} = \\left | \\vec{k} \\right |"]);return z=function(){return e},e}function k(){var e=Sn(["A_{max}"]);return k=function(){return e},e}function b(){var e=Sn(["A(t) = A_{max} cdot sin left ( \frac{2 pi}{lambda} - omega t + phi \right )"],["A(t) = A_{max} \\cdot \\sin \\left ( \\frac{2 \\pi}{\\lambda} - \\omega t + \\phi \\right )"]);return b=function(){return e},e}function D(){var e=Sn(["c = \frac{1}{sqrt{epsilon_0 cdot mu_0}} = 3.00 cdot 10^8 \frac{m}{s}"],["c = \\frac{1}{\\sqrt{\\epsilon_0 \\cdot \\mu_0}} = 3.00 \\cdot 10^8 \\frac{m}{s}"]);return D=function(){return e},e}function q(){var e=Sn(["c"]);return q=function(){return e},e}function L(){var e=Sn(["E = c cdot B"],["E = c \\cdot B"]);return L=function(){return e},e}function F(){var e=Sn(["B"]);return F=function(){return e},e}function E(){var e=Sn(["E"]);return E=function(){return e},e}function A(){var e=Sn(["N"]);return A=function(){return e},e}function P(){var e=Sn(["Delta V_{indotta} = - \frac{N cdot Delta Phi_{B_{spira}}}{Delta t} = - \frac{N cdot B cdot A cdot cos(alpha)}{Delta t}"],["\\Delta V_{indotta} = - \\frac{N \\cdot \\Delta \\Phi_{B_{spira}}}{\\Delta t} = - \\frac{N \\cdot B \\cdot A \\cdot cos(\\alpha)}{\\Delta t}"]);return P=function(){return e},e}function C(){var e=Sn(["Delta V_{indotta} = - \frac{Delta Phi_B}{Delta t}"],["\\Delta V_{indotta} = - \\frac{\\Delta \\Phi_B}{\\Delta t}"]);return C=function(){return e},e}function I(){var e=Sn(["Phi_B = \vec{B} cdot \vec{A} = B cdot A cdot cos(alpha)"],["\\Phi_B = \\vec{B} \\cdot \\vec{A} = B \\cdot A \\cdot \\cos(\\alpha)"]);return I=function(){return e},e}function S(){var e=Sn(["A"]);ret
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