diff --git a/PhysicsGravitationLabReport/ExperimentalSetup.pdf b/PhysicsGravitationLabReport/images/ExperimentalSetup.pdf similarity index 100% rename from PhysicsGravitationLabReport/ExperimentalSetup.pdf rename to PhysicsGravitationLabReport/images/ExperimentalSetup.pdf diff --git a/PhysicsGravitationLabReport/images/Force vs Mass m1 m2.pdf b/PhysicsGravitationLabReport/images/Force vs Mass m1 m2.pdf new file mode 100644 index 0000000..3cc0763 Binary files /dev/null and b/PhysicsGravitationLabReport/images/Force vs Mass m1 m2.pdf differ diff --git a/PhysicsGravitationLabReport/Force vs m1.pdf b/PhysicsGravitationLabReport/images/Force vs m1.pdf similarity index 100% rename from PhysicsGravitationLabReport/Force vs m1.pdf rename to PhysicsGravitationLabReport/images/Force vs m1.pdf diff --git a/PhysicsGravitationLabReport/images/Force vs m2.pdf b/PhysicsGravitationLabReport/images/Force vs m2.pdf new file mode 100644 index 0000000..a99dda3 Binary files /dev/null and b/PhysicsGravitationLabReport/images/Force vs m2.pdf differ diff --git a/PhysicsGravitationLabReport/main.pdf b/PhysicsGravitationLabReport/main.pdf index 62af160..e9f1551 100644 Binary files a/PhysicsGravitationLabReport/main.pdf and b/PhysicsGravitationLabReport/main.pdf differ diff --git a/PhysicsGravitationLabReport/main.tex b/PhysicsGravitationLabReport/main.tex index d6d42ff..c5278d6 100644 --- a/PhysicsGravitationLabReport/main.tex +++ b/PhysicsGravitationLabReport/main.tex @@ -16,6 +16,7 @@ \usepackage{placeins} \usepackage{float} +\graphicspath{{images/}} % ---------- Word-style margins ---------- @@ -399,18 +400,66 @@ $m_1$ and $F_g$ can be graphed as follows. Observing Figure \ref{fig:m1graph}, there is a linear trend between the gravitational force and the mass of object 1. This can be represented by the proportionality: \[ -F_g \propto m_1 +F_g \propto m_1. \] -Hence, the relationship can be described witht eh below equation, where $k_1$ is simply a constant: +Hence, the relationship can be described with the below equation, where $k_1$ is simply a constant: \begin{equation} F_g = k_1 \times m_1 -\label{eq:grav_force} +\label{eq:m1} \end{equation} Applying the same logic to Table \ref{tab:grav_m2} yields the following relationship between $F_g$ and $m_2$ +\begin{figure}[h!] % h! = “here” placement + \centering + \includegraphics[width=0.7\textwidth]{Force vs m2} % <-- your image file name + \caption{$F_g$ vs $m_2$ graphed} + \label{fig:m2graph} +\end{figure} + +Note that again, there is a linear trend, implying + +\[ +F_g \propto m_2. +\] + +Hence, the relationship can be described with the below equation, where $k_2$ is simply another constant: + +\begin{equation} +F_g = k_2 \times m_2. +\label{eq:m2} +\end{equation} + +Looking at equation \ref{eq:m1} and \ref{eq:m2}, they can be safely combined into one equation, where there is yet another constant of proportionality $k_3$: + +\begin{equation} +F_g = k_3 (m_1 \times m_2). +\label{eq:m1and2} +\end{equation} + +Note, that when $m_1$ and $m_2$ are the same, equation \ref{eq:m1and2} simplifies to + +\[ +F_g = k_3 \times m^2. +\] + +Looking at Table \ref{tab:grav_equal}, this derived relationship can be verified by graphing as follows: + + + +\begin{figure}[h!] % h! = “here” placement + \centering + \includegraphics[width=0.7\textwidth]{Force vs Mass m1 m2} % <-- your image file name + \caption{$F_g$ vs mass of $m_1$ = $m_2$} + \label{fig:m1m2graph} +\end{figure} + + +As suggested by equation \ref{eq:m1and2}, there is a proportional quadratic relationship between the masses of the objects and the resulting gravitational force (see Figure \ref{fig:m1m2graph}). +Therefore, equation \ref{eq:m1and2} is validated by the simulation. + \section*{Error Analysis}