Answer:
The magnitude of the acceleration of the box is [tex]2.291\,\frac{m}{s^{2}}[/tex].
Explanation:
The free body diagram of the crate is included as attachment, whose equations of equilibrium are described below:
[tex]\Sigma F_{x} = P\cdot \cos 20^{\circ} - \mu_{k}\cdot N = \left(\frac{W}{g}\right)\cdot a[/tex]
[tex]\Sigma F_{y} = P\cdot \sin 20^{\circ} + N - W = 0[/tex]
From second equation of equilibrium we find an expression for the normal force and find the respective value:
[tex]N = W - P \cdot \sin 20^{\circ}[/tex]
[tex]N = 930\,N - 400\cdot \sin 20^{\circ}\,N[/tex]
[tex]N = 793.192\,N[/tex]
Lastly, the acceleration experimented by the crate during pushing is cleared in the first equation of equilibrium and consequently calculated:
[tex]a = \frac{P\cdot \cos 20^{\circ}-\mu_{k}\cdot N}{\frac{W}{g} }[/tex]
[tex]a = \frac{400\cdot \cos 20^{\circ}\,N-0.20\cdot (793.192\,N)}{\frac{930\,N}{9.807\,\frac{m}{s^{2}} } }[/tex]
[tex]a = 2.291\,\frac{m}{s^{2}}[/tex]
The magnitude of the acceleration of the box is [tex]2.291\,\frac{m}{s^{2}}[/tex].