hw4 calculcations
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146
hw4.Rmd
146
hw4.Rmd
@@ -27,14 +27,17 @@ dedicated file on the local disc.
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The problem description, method, R script and implementation results
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should be presented in a single HTML document, which should be
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sent to the subject teacher's e-mail by May 21, 2026 at 23:59 CEST.
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\newpage
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# Input
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### Select the file
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```{r select-file}
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library(rstudioapi)
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rinex_file <- rstudioapi::selectFile()
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```
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### Read the file
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```{r read-file}
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extract_klobuchar_parameters <- function(rinex_file) {
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ion_alpha <- numeric(4)
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@@ -66,6 +69,12 @@ extract_klobuchar_parameters <- function(rinex_file) {
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}
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klobuchar_params <- extract_klobuchar_parameters(rinex_file)
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alpha <- function(index){
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klobuchar_params$ION_ALPHA[index+1]
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}
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beta <- function(index){
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klobuchar_params$ION_BETA[index+1]
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}
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print(klobuchar_params)
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```
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@@ -75,54 +84,145 @@ print(klobuchar_params)
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selected_date <- as.Date("2000-1-1")
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```
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\newpage
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# Klobuchar calculation
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1. Calculate earth-centered angle
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What are R_E and h?
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- $R_E$ is the earth's mean radius, $6371$ km.
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- $h$ is the height of the ionosphere, which is $350$ km for GPS ($375$ for Beidou).
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```{r klob-inputs}
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# constants
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R_E = 6371e3
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h = 350e3
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# inputs
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lat = 45.33709 # phi
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lon = 14.42496 # lambda
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E = 90 # elevation
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A = 180 # azimuth
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```
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### 1. Calculate earth-centered angle
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$$ \psi = \pi/2 - E - \arcsin(\frac{R_E}{R_E + h} \cos(E)) $$
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```{r klob-1}
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psi = pi/2 - E - asin(R_E / (R_E+h) * cos(E))
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```
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```{r klob-1-demo, echo=FALSE}
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psi
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```
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2. Compute the latitude of the IPP (ionospheric pierce point)
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### 2. Compute the latitude of the IPP (ionospheric pierce point)
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$$ \phi_I = \arcsin( sin \varphi_u \cos \psi + \cos\varphi_u \sin\psi \cos A )$$
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3. Compute the longitude of the IPP
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```{r klob-2}
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phi_I = asin(sin(lat) * cos(psi) + cos(lat) * sin(psi)* cos(A))
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```
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```{r klob-2-demo, echo=FALSE}
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phi_I
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```
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### 3. Compute the longitude of the IPP
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$$ \lambda_I= \lambda_u + \frac{\psi \sin A}{\cos \phi_I}$$
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4. Find the geomagnetic latitude of the IPP
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What is phi_P?
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```{r klob-3}
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lambda_I = lat + (psi * sin(A))/cos(phi_I)
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```
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```{r klob-3-demo, echo=FALSE}
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lambda_I
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```
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### 4. Find the geomagnetic latitude of the IPP
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$$ \phi_m = \arcsin(\sin\phi_I \sin\phi_P + \cos\phi_I \cos\phi_P \cos(\lambda_I - \lambda_P)) $$
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5. Find the local time at the IPP
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with $\phi_P = 78.3$°, $\lambda_P = 291.0$° the coordinates of the geomagnetic pole.
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```{r klob-4}
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phi_P = 78.3
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lambda_P = 291
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phi_m = asin(sin(phi_I) * sin(phi_P) + cos(phi_I) * cos(phi_P) * cos(lambda_I - lambda_P))
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```
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```{r klob-4-demo, echo=FALSE}
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phi_m
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```
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### 5. Find the local time at the IPP
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$$ t = 43200 \lambda_I / \pi + t_{GPS} $$
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With:
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$\lambda_I$ in radians, $t$ in seconds.
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where $0 \leq t \leq 86 400$. Therefore:
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If $t \geq 86 400$, subtract $86 400$. If $t < 0$, add $86 400$.
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```{r klob-5}
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tGPS = 1 # TODO
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t = 43200 * lambda_I / pi + tGPS
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```
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```{r klob-5-demo}
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t
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```
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6. Compute the amplitude of ionospheric delay
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### 6. Compute the amplitude of ionospheric delay
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$$ A_I = \sum_{n=0}^{3} \alpha_n(\phi_m/\pi)^n $$
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If $A_I < 0$, then $A_I =0$.
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```{r klob-6}
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n = c(0,1,2,3)
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A_I = sum(alpha(n) * (phi_m/pi) ^ n)
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if (A_I < 0) {
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A_I = 0
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}
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```
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```{r klob-6-demo, echo=FALSE}
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A_I
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```
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7. Compute the period of ionospheric delay
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### 7. Compute the period of ionospheric delay
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$$ P_I = \sum_{n=0}^{3} \beta_n(\phi_m/\pi)^n $$
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If $P_I < 72 000$ then $P_I = 72000$.
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8. Compute the phase of ionospheric delay
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```{r klob-7}
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P_I = sum(beta(n) * (phi_m/pi) ^ n)
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if (P_I < 72000) {
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P_I = 72000
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}
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```
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```{r klob-7-demo, echo=FALSE}
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P_I
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```
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### 8. Compute the phase of ionospheric delay
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$$ X_I = \frac{2\pi ( t-50400)}{P_I}$$
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9. Compute the slant factor (ionospheric mapping function)
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```{r klob-8}
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X_I = (2 * pi * (t-50400))/P_I
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```
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```{r klob-8-demo, echo=FALSE}
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X_I
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```
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### 9. Compute the slant factor (ionospheric mapping function)
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$$ F=\left[1 - (\frac{R_E}{R_E + h} \cos E)^2\right]^{-1/2} $$
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10. Compute the ionospheric time delay
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```{r klob-9}
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F = (1- (R_E/(R_E+h) * cos(E) )^2)^(-1/2)
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```
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```{r klob-9-demo, echo=FALSE}
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F
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```
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### 10. Compute the ionospheric time delay
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$$
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I_1 = \begin{cases}
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[5 \cdot 10^{-9} + A_I \cos X_I] \times F, & \quad |X_I| < \pi/2 \\
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5 \cdot 10^{-9} \times F, & \quad |X_I| \geq \pi/2
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\end{cases}
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$$
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The delay I1 is given in seconds and is referred to the GPS L1 or
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```{r klob-10}
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if (abs(X_I)< pi/2) {
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I_1 = (5e-9 + A_I * cos(X_I)) * F
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}else{
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I_1 = 5e-9 * F
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}
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```
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```{r klob-10-demo, echo=FALSE}
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I_1
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```
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The delay $I_1$ is given in seconds and is referred to the GPS L1 or
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Beidou B1 frequencies.
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```{r simulate}
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# input constants
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lat = 45.33709 # phi
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lon = 14.42496 # lambda
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E = 90
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A = 180
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```
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