def spatial_corr(self, cross_len = 2.0, nos = 80):
"""Spatial Correlatoin, cross length (corss_len) is assigned as two lambdas by default. nos means number of sections."""
self.spatial_correlation = []
spatial_max = 0
step = float(cross_len) / nos
for each in range(nos + 1):
temp = 0
for k, each_AoA in enumerate(self.AoA_all):
each_step = each*step*sine(each_AoA/180.0*PI)*2*PI
phase = cosine(each_step) + 1j*sine(each_step)
temp = temp + self.power_from_BS_to_UE_V[k]*phase
self.spatial_correlation.append(abs(temp))
self.spatial_correlation = [each / self.spatial_correlation[0] for each in self.spatial_correlation]
step_tenth_lambda = 0.1
step_half_lambda = 0.5
step_full_lambda = 1.0
self.power_from_BS_to_UE_tenth_lambda = []
self.power_from_BS_to_UE_half_lambda = []
self.power_from_BS_to_UE_full_lambda = []
for k, each_AoA in enumerate(self.AoA_all):
step = step_tenth_lambda*sine(each_AoA/180.0*PI)*2*PI
phase = cosine(step) + 1j*sine(step)
self.power_from_BS_to_UE_tenth_lambda.append(self.power_from_BS_to_UE_V[k]*phase)
step = step_half_lambda*sine(each_AoA/180.0*PI)*2*PI
phase = cosine(step) + 1j*sine(step)
self.power_from_BS_to_UE_half_lambda.append(self.power_from_BS_to_UE_V[k]*phase)
step = step_full_lambda*sine(each_AoA/180.0*PI)*2*PI
phase = cosine(step) + 1j*sine(step)
self.power_from_BS_to_UE_full_lambda.append(self.power_from_BS_to_UE_V[k]*phase)
def print_math():
""" Prints some calculated values. """
x = math.cosine(Pi)
print(x)
y = math.sine(Pi)
print("The sine of PI is", y)
def ani(self, cross_len = 2.0, nos = 80):
"""cross length (corss_len) is assigned as two lambdas by default. nos means number of sections."""
self.ani_x = {}
self.ani_y = {}
spatial_max = 0
delta = float(cross_len) / nos
for n in range(nos + 1):
step = n*delta
data = []
for k, each_AoA in enumerate(self.AoA_all):
step2 = step*sine(each_AoA/180.0*PI)*2*PI
phase = cosine(step2) + 1j*sine(step2)
data.append(self.power_from_BS_to_UE_V[k]*phase)
self.ani_x[n] = np.array([each.real for each in data])
self.ani_y[n] = np.array([each.imag for each in data])
def spatial_corr(self, cross_len=2.0, nos=80):
"""Spatial Correlatoin, cross length (corss_len) is assigned as two lambdas by default. nos means number of sections."""
self.spatial_correlation = []
spatial_max = 0
step = float(cross_len) / nos
for each in range(nos + 1):
temp = 0
for k, each_AoA in enumerate(self.AoA_all):
each_step = each * step * sine(each_AoA / 180.0 * PI) * 2 * PI
phase = cosine(each_step) + 1j * sine(each_step)
temp = temp + self.power_from_BS_to_UE_V[k] * phase
self.spatial_correlation.append(abs(temp))
self.spatial_correlation = [
each / self.spatial_correlation[0]
for each in self.spatial_correlation
]
step_tenth_lambda = 0.1
step_half_lambda = 0.5
step_full_lambda = 1.0
self.power_from_BS_to_UE_tenth_lambda = []
self.power_from_BS_to_UE_half_lambda = []
self.power_from_BS_to_UE_full_lambda = []
for k, each_AoA in enumerate(self.AoA_all):
step = step_tenth_lambda * sine(each_AoA / 180.0 * PI) * 2 * PI
phase = cosine(step) + 1j * sine(step)
self.power_from_BS_to_UE_tenth_lambda.append(
self.power_from_BS_to_UE_V[k] * phase)
step = step_half_lambda * sine(each_AoA / 180.0 * PI) * 2 * PI
phase = cosine(step) + 1j * sine(step)
self.power_from_BS_to_UE_half_lambda.append(
self.power_from_BS_to_UE_V[k] * phase)
step = step_full_lambda * sine(each_AoA / 180.0 * PI) * 2 * PI
phase = cosine(step) + 1j * sine(step)
self.power_from_BS_to_UE_full_lambda.append(
self.power_from_BS_to_UE_V[k] * phase)
def terminator(ox, oy, radius, angle, col):
alpha = 220
if ox + radius > 0 and ox - radius < xSize:
if radius < 2:
angle = 180 - abs(180 - angle)/1
circle(screen,[col[0]*angle/180,col[1]*angle/180,col[2]*angle/180],(ox,oy),radius)
else:
angle = angle*pi/180
angle = 2*pi-angle
for y in range(2*int(radius)):
rowRadius = sqrt(radius**2 - (radius - y)**2)
darkLength = int(rowRadius - rowRadius*sine(angle - pi/2))
if angle > pi:
darkStart = ox - rowRadius
else:
darkStart = ox + rowRadius - darkLength + 1
if angle < 0.1 :
darkLength -= 1
f = angle/0.1
bit = pygame.Surface((1, 1), pygame.SRCALPHA)
bit.fill((0, 0, 0, alpha*f))
screen.blit(bit, (ox + rowRadius,oy - radius + y))
if angle > 2*pi - 0.1:
darkLength -= 1
darkStart += 1
f = (2*pi - angle)/0.1
bit = pygame.Surface((1, 1), pygame.SRCALPHA)
bit.fill((0, 0, 0, alpha*f))
screen.blit(bit, (ox - rowRadius,oy - radius + y))
horizontal_line = pygame.Surface((abs(darkLength), 1), pygame.SRCALPHA)
horizontal_line.fill((0, 0, 0, alpha))
screen.blit(horizontal_line, (darkStart,oy - radius + y))
def foo6():
print(math.sine(3))
print(math.sin(math.pi / 2))
def sin(x):
if 2 * x == pi:
return 0.99999999
else:
return None
pi = 3.14
print(sin(pi / 2)) # our variable and function
print(math.sin(math.pi / 2)) # math module's variable and function
from math import sin, pi # import only what is required
print(sin(pi / 2))
# from module import *
# to import all entities above statement is used
# import module as alias
# aliasing module or giving our own name
import math as m # math keyword cannot be used now
print(m.sin(m.pi / 2))
from math import pi as PI, sin as sine
print(sine(PI / 2))
import math
print(math.sin(math.pi / 2))
print('-' * 10, '2')
from math import sin, pi
print(sin(pi / 2))
print('-' * 10, 'aliasing:')
import math as M
print(M.sin(M.pi / 2))
# after successful execution of an aliased import, the original module name becomes inaccessible and must not be used.
print('-' * 10, 'aliasing 2:')
from math import sin as sine, pi as P
print(sine(P / 2))
#-----------------------------------------------
# Some useful modules
#-----------------------------------------------
print('-' * 50)
print(' 4.2')
print('-' * 50)
import os
print(dir(os)) # list os module functions in a sorted list
print('-' * 10, 'math:')
print(M.e)
# ---
from math import ceil, floor, trunc, factorial, hypot
x = 1.4
y = 2.6
# ceil(x) - return smallest integer greater or equal to x
# -*- coding: utf-8 -*-
"""
Created on Fri Mar 13 09:12:37 2020
@author: David
"""
import math as mt
print(mt.sin(mt.pi / 2))
print(mt.pi)
for i in range(6):
print(i, mt.sin(i))
from math import pi as numberpi
from math import sin as sine
print(sine(numberpi / 2))
from math import e as numbere, sin as sine, cos as cose
print("**************")
print(numbere)
print(cose(numberpi / 2))
print(sine(numberpi / 2))
else: rad = int(pythag(ySize,xSize)*degrees(atan(r/(d*d*d*3/1331)))/150)
#Stars
for star in stars:
origx = star[0]
origy = star[1]
star[0] += 90
star[1] -= ySize/2
col = [star[2],star[2],star[2]]
odist = sqrt(pow(star[1]*fov/xSize,2) + pow(star[0] - 90 - angle,2))
if odist < 2*rad*fov/xSize:
#col = [255,0,0]
arg = atan2(star[1]*fov/xSize, star[0] - 90 - angle)
dist = pow(odist,2)/(4*rad*fov/xSize) + rad*fov/xSize
star[0] = angle + 90 + dist*cosine(arg)
star[1] = dist*sine(arg)*xSize/fov
#if star[0] - 90 > angle: star[0] = angle + 90 + pow(star[0] - 90 - angle,2)/(4*rad*fov/xSize) + rad*fov/xSize
#elif star[0] - 90 < angle: star[0] = angle + 90 - pow(star[0] - 90 - angle,2)/(4*rad*fov/xSize) - rad*fov/xSize
#print(angle, rad*fov/xSize, arg, odist, dist, origx, origy, star[0], star[1])
for n in range(-1,2):
screen.set_at((int(xSize/2 + (star[0] + offset + 360*n)/fov*xSize), int(star[1] + ySize/2) + 1), col)
screen.set_at((int(xSize/2 + (star[0] + offset + 360*n)/fov*xSize), int(star[1] + ySize/2) - 1), col)
screen.set_at((int(xSize/2 + (star[0] + offset + 360*n)/fov*xSize), int(star[1] + ySize/2)), col)
screen.set_at((int(xSize/2 + (star[0] + offset + 360*n)/fov*xSize + 1), int(star[1] + ySize/2)), col)
screen.set_at((int(xSize/2 + (star[0] + offset + 360*n)/fov*xSize - 1), int(star[1] + ySize/2)), col)
star[0] = origx
star[1] = origy
for c in collect:
a = c[1]
def f(x):
return sine(x)
#Function import with rename from math import sin as sine print(sine(90)) print(sin(90)) #throws an exception sin is not defined
import datetime as dt strptime = dt.datetime.strptime import math Fs = 10000000 # Sampling frequency T = 1/Fs # Sampling period L = 1200 # Length of signal t = (0:L-1)*T # Time vector freq = 1420000000 signal = 0.7*sine(2*pi*freq*t) corrupted_signal = signal + 2*rand(size(t)) fig, ((ax1, ax2, ax3, ax4)) = plt.subplots(nrows = 4, ncols=1, sharex=True) ax1 = plt.gca()
def cal(X, Y):
C = cosine(X)
S = sine(Y)
print('The Cosine is:', C, ', and the Sine is:', S)
return C, S
def cosine(x):
return -math.sine(p*(math.pi *.5)) + 1
def sin(deg): return sine(radians(deg)) def cos(deg): return cosine(radians(deg))
def sin(deg):
return sine(radians(deg))
import numpy as np import matplotlib.pyplot as plt import math F = 15 # thrust avg r = 0.033 # radius theta = 0 # angle between force and moment arm torque = r * F * math.sine(theta)
