Section 4.3 Translational Equilibrium
An object is in translational equilibrium if the vector sum of the forces acting on that object add to zero.
- An object in translational equilibrium continues moving in a straight line with a constant speed as described by Newton’s First law. That is\begin{equation*} \sum\vec{F} = 0 \end{equation*}(Graphical and vector algebra problems.) or equivalently\begin{equation*} \sum\vec{F}_{x} = 0 \end{equation*}(x-component of net force),\begin{equation*} \sum\vec{F}_{y} = 0 \end{equation*}(y-component of net force),\begin{equation*} w = m g \end{equation*}(weight equation), and\begin{equation*} f = \mu N \end{equation*}(friction equation). In translational motion \(v\neq 0, a = 0,\) and \(F= 0\text{.}\)
- Problem Solving Technique: To solve a translational equilibrium problem one needs to:
- Read problem, list given quantities, and label a drawing of the physical situation.
- Draw force diagrams for each body in translational equilibrium.
- Resolve the forces into components.
- Sum the x- and y-components of forces and set them to zero.
- Include a weight equation for each mass.
- Include a friction equation for each surface.
- Solve equations simultaneously for the quantities of interest.