Answer:
[tex]56.3^{\circ}[/tex]
Explanation:
The figure is missing, find it in attachment.
The figure shows the velocity along the x-axis, [tex]v_x[/tex], versus time. The slope of the line gives us the acceleration along the x-axis, which is therefore given by:
[tex]a_x = \frac{\Delta v_x}{\Delta t}=\frac{5-2}{3-2}=3 m/s^2[/tex]
Now we can apply Newton's second law along the x-axis:
[tex]F_x = m a_x[/tex]
where
[tex]F_x[/tex] is the resultant force along the x-axis
m = 4 kg is the mass of the disk
[tex]a_x = 3 m/s^2[/tex] is the acceleration along this axis
Solving,
[tex]F_x = (4)(3)=12 N[/tex]
So now we know that this is the component of resultant force along the x-axis. The resultant force is given by two forces:
F1, which acts along the x-direction
F2, which acts at a certain angle [tex]\theta[/tex]
So the component of the resultant along the x-axis can be written as
[tex]F_x = F_1 + F_2 cos \theta[/tex]
where we know:
[tex]F_1 = 7 N\\F_2 = 9 N[/tex]
Solving for [tex]\theta[/tex], we find:
[tex]cos \theta = \frac{F_x-F_1}{F_2}=\frac{12-7}{9}=0.555\\\theta =cos^{-1}(0.555)=56.3^{\circ}[/tex]