Flight Summary
Flight Statistics
Data normalized across several flight logs, spanning from NS45 to NS80, excepting NS54, NS55, and NS68 (NS54 is reserved for a flight still in development, and both NS55 and NS68 failed to record location data).
Due to a settings issue, before NS59, the cell tracker hardware stopped recording above 12.1 km (except for NS53). This limit is shown as a grey horizontal line in the figures depicting altitude.
require(ggplot2)
Loading required package: ggplot2
require(directlabels)
Loading required package: directlabels
require(scales)
Loading required package: scales
source("setup.R")
flight_times <- read_flight_times("flight_times.txt")
flight_data <- read_flight_data("flight_data/", calculate_difftime = TRUE)
Ascent Rate
Ascent Rate vs Time of Year
ggplot(flight_data,
aes(
x = as.Date(format(DateTime, format = "%m-%d"), format = "%m-%d"),
y = Ascent_Rate_m_s,
colour = Flight
)) +
geom_point() + geom_path() +
geom_hline(yintercept = 0, alpha = 0.2) +
scale_x_date(
date_breaks = "1 month",
labels = date_format("%b"),
limits = as.Date(c("01-01", "12-31"), format = "%m-%d"),
expand = c(0, 0)
) +
geom_dl(aes(label = gsub("NS", "", Flight)),
method = list(cex = 0.8, dl.trans(y = y + 0.2), "top.bumpup")) + guides(colour = FALSE) +
labs(title = "Ascent Rate vs Time of Year", x = "Time of Year", y = "Ascent Rate (m/s)")
Ascent Rate After Burst
ggplot(flight_data,
aes(x = burst_difftime / 60,
y = Ascent_Rate_m_s,
colour = Flight)) +
geom_path() +
xlim(-0.5, 3) +
geom_dl(aes(label = gsub("NS", "", Flight)), method = list("smart.grid", "small.box.labels")) + guides(colour = FALSE) +
labs(title = "Ascent Rate After Burst", x = "Time Since Burst (minutes)", y = "Ascent Rate (m/s)")
Ascent Rate vs Altitude
ggplot(flight_data,
aes(x = Altitude_m / 1000,
y = Ascent_Rate_m_s,
colour = Flight)) +
geom_path() +
geom_dl(aes(label = gsub("NS", "", Flight)),
method = list("far.from.others.borders", "small.box.labels")) + guides(colour = FALSE) +
labs(title = "Ascent Rate vs Altitude", x = "Altitude (km)", y = "Ascent Rate (m/s)")
Ground Speed
Ground Speed vs Time of Year
ggplot(flight_data,
aes(
x = as.Date(format(DateTime, format = "%m-%d"), format = "%m-%d"),
y = Ground_Speed_m_s,
colour = Flight
)) +
geom_point() + geom_path() +
scale_x_date(
date_breaks = "1 month",
labels = date_format("%b"),
limits = as.Date(c("01-01", "12-31"), format = "%m-%d"),
expand = c(0, 0)
) +
geom_dl(aes(label = gsub("NS", "", Flight)),
method = list(cex = 0.8, dl.trans(y = y + 0.2), "top.bumpup")) + guides(colour = FALSE) +
labs(title = "Ground Speed vs Time of Year", x = "Time of Year", y = "Ground Speed (m/s)")
Ground Speed vs Altitude
ggplot(
flight_data,
aes(
x = Altitude_m / 1000,
y = Ground_Speed_m_s,
colour = as.POSIXlt(DateTime)$yday
)
) +
geom_point() +
scale_colour_gradient2(
limits = c(0, 366),
low = "green",
mid = "red",
midpoint = 366 / 2,
high = "blue"
) +
labs(
title = "Ground Speed vs Altitude",
x = "Altitude (km)",
y = "Ground Speed (m/s)",
colour = "Day of Year"
) +
theme(
legend.position = c(1, 1),
legend.direction = "horizontal",
legend.justification = "right"
)
Green: late winter, Yellow: spring, Red: summer, Purple: autumn, Blue: early winter
Ascent and Descent Durations
For flights with definite burst and landing times, we can extract the times it took for the balloon to ascend and descend from max altitude.
flight_durations <- data.frame()
for (current_flight in flight_times$Flight)
{
if (!is.na(flight_times$Launch_Time[flight_times$Flight == current_flight]) &&
!is.na(flight_times$Burst_Time[flight_times$Flight == current_flight]) &&
!is.na(flight_times$Landing_Time[flight_times$Flight == current_flight]))
{
current_ascent_duration <-
as.numeric(with(
flight_times,
difftime(Launch_Time[Flight == current_flight], Burst_Time[Flight == current_flight], units = "mins")
)) * -1
current_descent_duration <-
as.numeric(with(
flight_times,
difftime(Landing_Time[Flight == current_flight], Burst_Time[Flight == current_flight], units = "mins")
))
flight_durations <- rbind(
flight_durations,
data.frame(
Flight = current_flight,
Date = flight_times$Date[flight_times$Flight == current_flight],
Ascent_Duration_min = current_ascent_duration,
Descent_Duration_min = current_descent_duration,
Ratio = current_ascent_duration / current_descent_duration
)
)
}
}
rm(current_flight,
current_ascent_duration,
current_descent_duration)
rmarkdown::paged_table(flight_durations)
On average, ascent takes 69 minutes, while descent takes 36 minutes, with a ratio of 2.
Ascent Duration vs Descent Duration
ggplot(
flight_durations,
aes(
x = Descent_Duration_min,
y = Ascent_Duration_min,
colour = as.POSIXlt(Date)$yday
)
) +
geom_point(size = 0.1) + geom_abline(slope = 1:3) +
scale_colour_gradient2(
limits = c(0, 366),
low = "green",
mid = "red",
midpoint = 366 / 2,
high = "blue"
) +
geom_dl(aes(label = gsub("NS", "", Flight)), method = list(cex = 0.8)) +
labs(
title = "Ascent Duration vs Descent Duration",
x = "Descent Duration (minutes)",
y = "Ascent Duration (minutes)",
colour = "Day of Year"
) +
coord_fixed(ratio = 1) +
scale_x_continuous(breaks = seq(
from = 0,
to = max(flight_data$Downrange_Distance_m),
by = 10
)) +
scale_y_continuous(breaks = seq(
from = 0,
to = max(flight_data$Altitude_m),
by = 10
)) +
theme(
legend.position = c(1, 0.96),
legend.direction = "horizontal",
legend.justification = "right"
)
Green: late winter, Yellow: spring, Red: summer, Purple: autumn, Blue: early winter
---
title: "Flight Analysis"
output:
  html_notebook: 
    code_folding: hide
    toc: yes
    number_sections: yes
    toc_float: 
        collapsed: false
---

[Flight Summary](flight_summary.nb.html)

[Flight Statistics](flight_statistics.nb.html)

Data normalized across several flight logs, spanning from `r min(levels(flight_data$Flight))` to `r max(levels(flight_data$Flight))`, excepting NS54, NS55, and NS68 (NS54 is reserved for a flight still in development, and both NS55 and NS68 failed to record location data).

Due to a settings issue, before NS59, the cell tracker hardware stopped recording above 12.1 km (except for NS53). This limit is shown as a grey horizontal line in the figures depicting altitude.

```{r setup}
require(ggplot2)
require(directlabels)
require(scales)

source("setup.R")

flight_times <- read_flight_times("flight_times.txt")
flight_data <- read_flight_data("flight_data/", calculate_difftime = TRUE)
```

# Ascent Rate

## Ascent Rate vs Time of Year

```{r ascent_rate_vs_time_of_year, fig.height=7.4164079, fig.width=12}
ggplot(flight_data,
       aes(
           x = as.Date(format(DateTime, format = "%m-%d"), format = "%m-%d"),
           y = Ascent_Rate_m_s,
           colour = Flight
       )) +
    geom_point() + geom_path() +
    geom_hline(yintercept = 0, alpha = 0.2) +
    scale_x_date(
        date_breaks = "1 month",
        labels = date_format("%b"),
        limits = as.Date(c("01-01", "12-31"), format = "%m-%d"),
        expand = c(0, 0)
    ) +
    geom_dl(aes(label = gsub("NS", "", Flight)),
            method = list(cex = 0.8, dl.trans(y = y + 0.2), "top.bumpup")) + guides(colour = FALSE) +
    labs(title = "Ascent Rate vs Time of Year", x = "Time of Year", y = "Ascent Rate (m/s)")
```

## Ascent Rate After Burst

```{r ascent_rate_after_burst, fig.height=7.4164079, fig.width=12}
ggplot(flight_data,
       aes(x = burst_difftime / 60,
           y = Ascent_Rate_m_s,
           colour = Flight)) +
    geom_path() +
    xlim(-0.5, 3) +
    geom_dl(aes(label = gsub("NS", "", Flight)), method = list("smart.grid", "small.box.labels")) + guides(colour = FALSE) +
    labs(title = "Ascent Rate After Burst", x = "Time Since Burst (minutes)", y = "Ascent Rate (m/s)")
```

## Ascent Rate vs Altitude

```{r ascent_rate_vs_altitude, fig.height=7.4164079, fig.width=12}
ggplot(flight_data,
       aes(x = Altitude_m / 1000,
           y = Ascent_Rate_m_s,
           colour = Flight)) +
    geom_path() +
    geom_dl(aes(label = gsub("NS", "", Flight)),
            method = list("far.from.others.borders", "small.box.labels")) + guides(colour = FALSE) +
    labs(title = "Ascent Rate vs Altitude", x = "Altitude (km)", y = "Ascent Rate (m/s)")
```

# Ground Speed

## Ground Speed vs Time of Year

```{r ground_speed_vs_time_of_year, fig.height=7.4164079, fig.width=12}
ggplot(flight_data,
       aes(
           x = as.Date(format(DateTime, format = "%m-%d"), format = "%m-%d"),
           y = Ground_Speed_m_s,
           colour = Flight
       )) +
    geom_point() + geom_path() +
    scale_x_date(
        date_breaks = "1 month",
        labels = date_format("%b"),
        limits = as.Date(c("01-01", "12-31"), format = "%m-%d"),
        expand = c(0, 0)
    ) +
    geom_dl(aes(label = gsub("NS", "", Flight)),
            method = list(cex = 0.8, dl.trans(y = y + 0.2), "top.bumpup")) + guides(colour = FALSE) +
    labs(title = "Ground Speed vs Time of Year", x = "Time of Year", y = "Ground Speed (m/s)")
```

## Ground Speed vs Altitude

```{r ground_speed_vs_altitude, fig.height=7.4164079, fig.width=12}
ggplot(
    flight_data,
    aes(
        x = Altitude_m / 1000,
        y = Ground_Speed_m_s,
        colour = as.POSIXlt(DateTime)$yday
    )
) +
    geom_point() +
    scale_colour_gradient2(
        limits = c(0, 366),
        low = "green",
        mid = "red",
        midpoint = 366 / 2,
        high = "blue"
    ) +
    labs(
        title = "Ground Speed vs Altitude",
        x = "Altitude (km)",
        y = "Ground Speed (m/s)",
        colour = "Day of Year"
    ) +
    theme(
        legend.position = c(1, 1),
        legend.direction = "horizontal",
        legend.justification = "right"
    )
```

Green: late winter, Yellow: spring, Red: summer, Purple: autumn, Blue: early winter

# Ascent and Descent Durations

For flights with definite burst and landing times, we can extract the times it took for the balloon to ascend and descend from max altitude. 

```{r duration_ratios}
flight_durations <- data.frame()

for (current_flight in flight_times$Flight)
{
    if (!is.na(flight_times$Launch_Time[flight_times$Flight == current_flight]) &&
        !is.na(flight_times$Burst_Time[flight_times$Flight == current_flight]) &&
        !is.na(flight_times$Landing_Time[flight_times$Flight == current_flight]))
    {
        current_ascent_duration <-
            as.numeric(with(
                flight_times,
                difftime(Launch_Time[Flight == current_flight], Burst_Time[Flight == current_flight], units = "mins")
            )) * -1
        current_descent_duration <-
            as.numeric(with(
                flight_times,
                difftime(Landing_Time[Flight == current_flight], Burst_Time[Flight == current_flight], units = "mins")
            ))
        
        flight_durations <- rbind(
            flight_durations,
            data.frame(
                Flight = current_flight,
                Date = flight_times$Date[flight_times$Flight == current_flight],
                Ascent_Duration_min = current_ascent_duration,
                Descent_Duration_min = current_descent_duration,
                Ratio = current_ascent_duration / current_descent_duration
            )
        )
    }
}

rm(current_flight,
   current_ascent_duration,
   current_descent_duration)

rmarkdown::paged_table(flight_durations)
```

On average, ascent takes `r signif(mean(flight_durations$Ascent_Duration_min), digits = 2)` minutes, while descent takes `r signif(mean(flight_durations$Descent_Duration_min), digits = 2)` minutes, with a ratio of `r signif(mean(flight_durations$Ratio), digits = 2)`.

## Ascent Duration vs Descent Duration

```{r current_ascent_duration_vs_current_descent_duration, fig.height=12, fig.width=7.4164079}
ggplot(
    flight_durations,
    aes(
        x = Descent_Duration_min,
        y = Ascent_Duration_min,
        colour = as.POSIXlt(Date)$yday
    )
) +
    geom_point(size = 0.1) + geom_abline(slope = 1:3) +
    scale_colour_gradient2(
        limits = c(0, 366),
        low = "green",
        mid = "red",
        midpoint = 366 / 2,
        high = "blue"
    ) +
    geom_dl(aes(label = gsub("NS", "", Flight)), method = list(cex = 0.8)) +
    labs(
        title = "Ascent Duration vs Descent Duration",
        x = "Descent Duration (minutes)",
        y = "Ascent Duration (minutes)",
        colour = "Day of Year"
    ) +
    coord_fixed(ratio = 1) +
    scale_x_continuous(breaks = seq(
        from = 0,
        to = max(flight_data$Downrange_Distance_m),
        by = 10
    )) +
    scale_y_continuous(breaks = seq(
        from = 0,
        to = max(flight_data$Altitude_m),
        by = 10
    )) +
    theme(
        legend.position = c(1, 0.96),
        legend.direction = "horizontal",
        legend.justification = "right"
    )
```
Green: late winter, Yellow: spring, Red: summer, Purple: autumn, Blue: early winter

```{r teardown, include=FALSE}
rm(read_flight_times, read_flight_data)

rm(small.box.labels)
#rm(flight_times)
#rm(flight_data)
```