SPATZ/spatz/sensors/antenna/tx_gain.py
2024-04-06 18:15:14 +02:00

192 lines
6.8 KiB
Python

from numpy.typing import ArrayLike
from typing import List, AnyStr
from numpy import matrix
from typing import List
import re
from io import StringIO
import numpy as np
import pandas as pd
import math
from spatz.sensors import Sensor
from spatz.simulation import Simulation
from spatz.transforms import Transform
from spatz.dataset import Dataset
from spatz.logger import Logger
import time
GAIN_NAME = "Abs(Gain)"
'''
Class representing a CST gain pattern
This (and the sensor below) follow the convetions laid out by https://www.antenna-theory.com/basics/radpattern.php.
I.e, theta represents the elevation angle and goes from 0 to 180 deg, Phi represents the azimuth angle.
The data is interpolated, you will have to specify the step size for this to work correctly.
'''
class GainPattern():
def __init__(self, filepath: str, step_size: int):
self._stepsize = step_size
# This is a cursed parser. If it breaks, though luck.
with open(filepath,"r") as file:
# Read Header
header = file.readline()
header = re.sub(r'\[(.*?)\]',",",header).replace(" ","").replace(",\n",'\n')
# Discard ---- line
file.readline()
# Parse to DF
lines = file.readlines()
clean_csv = [header]
start_time = time.time()
num_lines = len(lines)
for i,line in enumerate(lines):
if(i % step_size == 0 or i == num_lines-1):
cleaned = re.sub(r'\s+',',',line).removeprefix(',').removesuffix(',').strip()
clean_csv.append(cleaned + '\n')
clean_csv = ''.join(clean_csv)
filelike = StringIO(clean_csv)
self._df = pd.read_csv(filelike)
print(f"Processed {num_lines} lines in {(time.time()-start_time):.1f}s.")
print(f"Used {num_lines // step_size} lines due to step size")
self._df.to_csv("gainpattern.csv")
def get_phi_cut(self, phi:float) -> ArrayLike: #Return farfield cut with phi = const (Looking from the side)
assert 0 <= phi < 180
sub_df = self._df.loc[self._df["Phi"] == phi]
angles = sub_df["Theta"]
gain = sub_df[GAIN_NAME]
return angles,gain
def get_theta_cut(self, theta:float) -> ArrayLike: #Return farfield cut with theta = const (looking from the top)
assert 0<= theta < 180
sub_df_left = self._df.loc[self._df["Theta"] == theta]
angles_l = sub_df_left["Phi"]
gain_l = sub_df_left[GAIN_NAME]
sub_df_right = self._df.loc[self._df["Theta"] == (360-theta)]
angles_r = sub_df_right["Phi"]+180
gain_r = sub_df_right[GAIN_NAME]
angles = pd.concat([angles_l,angles_r])
gain = pd.concat([gain_l,gain_r])
return angles,gain
def __get_gain_internal(self,phi_step:float,theta_step:float):
assert phi_step%self._stepsize ==0
assert theta_step%self._stepsize==0
row = self._df.loc[(self._df["Theta"] == theta_step) & (self._df["Phi"] == phi_step)].iloc[0]
return row[GAIN_NAME]
def get_gain(self, phi, theta) -> float:
assert 0 <= phi < 360
assert 0 <= theta < 180
#Interpolate using binlinear interpolation https://en.wikipedia.org/wiki/Bilinear_interpolation
phi_lower = math.floor(phi/self._stepsize)*self._stepsize
phi_upper = phi_lower + self._stepsize
theta_lower = math.floor(theta/self._stepsize)*self._stepsize
theta_upper = theta_lower + self._stepsize
G11 = self.__get_gain_internal(phi_lower,theta_lower)
G12 = self.__get_gain_internal(phi_lower,theta_upper)
G21 = self.__get_gain_internal(phi_upper,theta_lower)
G22 = self.__get_gain_internal(phi_upper,theta_upper)
v1 = np.array([phi_upper-phi,phi-phi_lower])
v2 = np.array([[theta_upper-theta],[theta-theta_lower]])
A = np.array([[G11,G12],[G21,G22]])
interpolated = 1/(self._stepsize*self._stepsize) * v1 @ A @ v2
return interpolated[0]
'''
Sensor to simulate TX antenna gain in direction of ground station
Returns the gain in dBi per timestep.
'''
class AntennaTxGain(Sensor):
def __init__(self, dataset: Dataset, logger: Logger, transforms: List[Transform] = [], gain_pattern_path = "data/gain_pattern/farfield_2_45_GHz.txt"):
super().__init__(dataset, logger, transforms)
self._pattern = GainPattern(gain_pattern_path,1)
def _get_data(self) -> ArrayLike | float:
magic_matrix = np.array([
[0,1,0],
[1,0,0],
[0,0,-1]
])
# Get current position of rocket in FL Frame (Launcher Frame).
pos_fl = self._dataset.fetch_values(['x', 'y', 'z']) #X,Y,Z is in FL (Launcher frame) -> Z is up, X is east
gs_offset_fl = np.array([-1810,-1500,100]) #Radar hill is approx 1.81km west. 1.5km south, 100higher
rocket_to_gs_fl = pos_fl-gs_offset_fl
rocket_to_gs_fl_n = rocket_to_gs_fl/np.linalg.norm(rocket_to_gs_fl)
# Rocket in body frame is simply [1,0,0]^T by definition
rocket_b = np.array([1,0,0])
rocket_fl = magic_matrix @ np.linalg.inv(self._dataset.launch_rail_to_body()) @ rocket_b
rocket_fl_n = rocket_fl / np.linalg.norm(rocket_fl)
# Angle between rocket and pos returns elevation angle (Phi). Assume a rotation of 0° for now to get theta
theta = 180-np.rad2deg(np.arccos(np.clip(np.dot(rocket_to_gs_fl_n,rocket_fl_n),-1.0,1.0))) #Clip trick from: https://stackoverflow.com/questions/2827393/angles-between-two-n-dimensional-vectors-in-python
self._log("rocket_x",rocket_fl_n[0])
self._log("rocket_y",rocket_fl_n[1])
self._log("rocket_z",rocket_fl_n[2])
self._log("pos_x",rocket_to_gs_fl_n[0])
self._log("pos_y",rocket_to_gs_fl_n[1])
self._log("pos_z",rocket_to_gs_fl_n[2])
self._log("theta",theta)
#return phi
#Get Theta cut for this angle
#angles, gains = self._pattern.get_theta_cut(np.round(theta))
#min_gain = np.min(gains)
#min_ix = np.argmin(gains)
#min_angle = angles[min_ix]
#self._log("works_case_angle",min_angle)
min_gain = self._pattern.get_gain(45,theta)
# Fetch gain in this direction
return min_gain
def _sensor_specific_effects(self, x: ArrayLike) -> ArrayLike:
return x
def _get_name(self) -> AnyStr:
return 'antenna/tx_gain'
if __name__ == '__main__':
pattern = GainPattern("data/gain_pattern/farfield_all.txt")
print(pattern.get_gain(0,12))
print(pattern.get_gain(0,16))
print(pattern.get_gain(6,12))
print(pattern.get_gain(0,10))
print(pattern.get_theta_cut(90))