Authors: Russell C. Hibbeler
ISBN-13: 978-0133915426
See our solution for Question 6P from Chapter 6 from Hibbeler's Engineering Mechanics.
We are given the horizontal force at point D is ${F_1} = 3\;{\rm{kN}}$, the vertical force at point B is ${F_2} = 4\;{\rm{kN}}$, and the angle $\theta $ is $\theta = 30^\circ $.
We are asked the force in each member of the truss and state if the members are in the tension or compression.
The following is the free body diagram of the system:

We have the length of member BD is $BD = 1.5\;{\rm{m}}$.
We have the length of member AB is $AB = 2\;{\rm{m}}$.
We have the length of member BC is $BC = 2\;{\rm{m}}$.
The magnitude of angle $\theta $ is,
\[\tan \phi = \frac{{BD}}{{AB}}\]Substitute the values in the above expression.
\[\begin{array}{c} \tan \phi = \frac{{1.5\;{\rm{m}}}}{{2\;{\rm{m}}}}\\ \phi = 36.87^\circ \end{array}\]The reaction at point C by moment of all the forces about point A is,
\[\begin{array}{c} \Sigma {M_A} = 0\\ - {F_2}\left( {AB} \right) - {F_1}\left( {BD} \right) + {R_C}\cos \theta \left( {AB + BC} \right) = 0 \end{array}\] Step 6Substitute the values in the above expression.
\[\begin{array}{c} \left[ \begin{array}{c} - \left( {4\;{\rm{kN}}} \right)\left( {2\;{\rm{m}}} \right) - \left( {3\;{\rm{kN}}} \right)\left( {1.5\;{\rm{m}}} \right)\\ + {R_C}\cos 30^\circ \left( {2\;{\rm{m}} + 2\;{\rm{m}}} \right) \end{array} \right] = 0\\ {R_C} = \frac{{12.5\;\;{\rm{kN}} \cdot {\rm{m}}}}{{4\cos 30^\circ \;{\rm{m}}}}\\ {R_C} = 3.61\;{\rm{kN}} \end{array}\]The horizontal force at joint A of the truss by equilibrium condition in horizontal direction is,
\[\begin{array}{c} \Sigma {F_x} = 0\\ {A_x} + {F_1} - {R_C}\sin \theta = 0 \end{array}\]Substitute the values in the above expression.
\[\begin{array}{c} {A_x} + \left( {3\;{\rm{kN}}} \right) - \left( {3.61\;{\rm{kN}}} \right)\sin 30^\circ = 0\\ {A_x} = - 1.20\;{\rm{kN}} \end{array}\]The vertical force at joint A of the truss by equilibrium condition in vertical direction is,
\[\begin{array}{c} \Sigma {F_y} = 0\\ {A_y} - {F_2} + {R_C}\cos \theta = 0 \end{array}\] Step 10Substitute the values in the above expression.
\[\begin{array}{c} {A_y} - \left( {4\;{\rm{kN}}} \right) + \left( {3.61\;{\rm{kN}}} \right)\cos 30^\circ = 0\\ {A_y} = - 0.87\;{\rm{kN}} \end{array}\]The free body diagram of forces acting at point A is:

The force on member AD by equilibrium condition is,
\[\begin{array}{c} \Sigma {F_y} = 0\\ {A_y} + {F_{AD}}\sin \phi = 0 \end{array}\]Substitute the values in the above expression.
\[\begin{array}{c} - 0.87\;{\rm{kN}} + {F_{AD}}\sin 36.87^\circ = 0\\ {F_{AD}} = 1.45\;{\rm{kN}}\left( {{\rm{Compression}}} \right) \end{array}\]The force on member AB by equilibrium condition is,
\[\begin{array}{c} \Sigma {F_x} = 0\\ {A_x} + {F_{AD}}\cos \phi + {F_{AB}} = 0 \end{array}\]Substitute the values in the above expression.
\[\begin{array}{c} - 1.20\;{\rm{kN}} - \left( {1.45\;{\rm{kN}}} \right)\cos 36.87^\circ + {F_{AB}} = 0\\ {F_{AB}} = 2.36\;{\rm{kN}}\left( {{\rm{Compression}}} \right) \end{array}\]The free body diagram of forces acting at point B is:

The force on member BD by equilibrium condition is,
\[ - {F_2} + {F_{BD}} = 0\]Substitute the values in the above expression.
\[\begin{array}{c} - 4\;{\rm{kN}} + {F_{BD}} = 0\\ {F_{BD}} = 4\;{\rm{kN}}\left( {{\rm{Compression}}} \right) \end{array}\]The force on member BC by equilibrium condition is,
\[ - {F_{AB}} + {F_{BC}} = 0\]Substitute the values in the above expression.
\[\begin{array}{c} - 2.36\;{\rm{kN}} + {F_{BC}} = 0\\ {F_{BC}} = 2.36\;{\rm{kN}}\left( {{\rm{Compression}}} \right) \end{array}\]The free body diagram of forces acting at point C is:

The force on member CD by equilibrium condition is,
\[{R_C}\cos \theta + {F_{CD}}\sin \phi = 0\]Substitute the values in the above expression.
\[\begin{array}{c} \left( {3.61\;{\rm{kN}}} \right)\cos 30^\circ + {F_{CD}}\sin 36.87^\circ = 0\\ {F_{CD}} = 5.21\;{\rm{kN}}\left( {{\rm{Compression}}} \right) \end{array}\]