If a body is in static equilibrium, then by definition that body is not accelerating. If we know that the body is not accelerating then we know that the sum of the forces acting on that body must be equal to zero. This is the basis for equilibrium analysis for a particle. In order to solve for any unknowns in our sum of forces equation, we actually need to turn the one vector equation into a set of scalar equations. For two dimensional problems, we will split our one vector equation down into two scalar equations. We do this by summing up all the \(x\) components of the force vectors and setting them equal to zero in our first equation, and summing up all the \(y\) components of the force vectors and setting them equal to zero in our second equation. \[ \sum \vec \, = \, 0 \] \[ \sum F_x \, = \, 0 \, ; \,\,\, \sum F_y \, = \, 0 \] We do something similar in three dimensional problems except we will break all our force vectors down into \(x\), \(y\), and \(z\) components, setting the sum of \(x\) components equal to zero for our first equation, the sum of all the \(y\) components equal to zero for our second equation, and the sum of all our \(z\) components equal to zero for our third equation. \[ \sum \vec \, = \, 0 \] \[ \sum F_x \, = \, 0 \, ; \,\,\, \sum F_y \, = \, 0 \, ; \,\,\, \sum F_z \, = \, 0 \] Once we have written out the equilibrium equations, we can solve the equations for any unknown forces.
The first step in finding the equilibrium equations is to draw a free body diagram of the body being analyzed. This diagram should show all the known and unknown force vectors acting on the body. In the free body diagram, provide values for any of the know magnitudes or directions for the force vectors and provide variable names for any unknowns (either magnitudes or directions). 
Next you will need to chose the \(x\), \(y\), and \(z\) axes. These axes do need to be perpendicular to one another, but they do not necessarily have to be horizontal or vertical. If you choose coordinate axes that line up with some of your force vectors you will simplify later analysis. Once you have chosen axes, you need to break down all of the force vectors into components along the \(x\), \(y\) and \(z\) directions (see the vectors page in Appendix 1 if you need more guidance on this). Your first equation will be the sum of the magnitudes of the components in the \(x\) direction being equal to zero, the second equation will be the sum of the magnitudes of the components in the \(y\) direction being equal to zero, and the third (if you have a 3D problem) will be the sum of the magnitudes in the \(z\) direction being equal to zero. Collectively these are known as the equilibrium equations. Once you have your equilibrium equations, you can solve them for unknowns using algebra. The number of unknowns that you will be able to solve for will be the number of equilibrium equations that you have. In instances where you have more unknowns than equations, the problem is known as a statically indeterminate problem and you will need additional information to solve for the given unknowns. 
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Video \(\PageIndex<9>\): Worked solution to example problem \(\PageIndex\), provided by Dr. Jacob Moore. YouTube source: https://youtu.be/HQqNGJR3ybQ.
This page titled 2.5: Equilibrium Analysis for Concurrent Force Systems is shared under a CC BY-SA 4.0 license and was authored, remixed, and/or curated by Jacob Moore & Contributors (Mechanics Map) via source content that was edited to the style and standards of the LibreTexts platform.
