(a) 34.6 N
To solve the problem, we have to analyze the forces acting along the horizontal direction.
We have:
- Forward: the component of the pull parallel to the ground, which is
[tex]F cos \theta[/tex]
where
F is the magnitude of the pull
[tex]\theta=30^{\circ}[/tex] is the angle
- Backward: the force of friction, which is
[tex]F_f = 30 N[/tex]
So, the equation of motion is
[tex]F cos \theta - F_f = ma[/tex]
where
m = 20 kg is the mass of the wagon
a is the acceleration
In this part, the wagon is moving at constant speed, so a =0 and the equation becomes
[tex]F cos \theta - F_f = 0[/tex]
Therefore, we can find the pulling force:
[tex]F=\frac{F_f}{cos \theta}=\frac{30}{cos 30}=34.6 N[/tex]
(b) 43.9 N
In this case, the acceleration is
[tex]a=0.40 m/s^2[/tex]
So, the equation of motion in this case is
[tex]F cos \theta - F_f = ma[/tex]
So this time we have to take into account the term (ma).
Using the same data as before:
m = 20 kg
[tex]\theta=30^{\circ}[/tex]
[tex]F_f = 30 N[/tex]
We find the new magnitude of F:
[tex]F=\frac{ma+F_f}{cos \theta}=\frac{(20)(0.40)+30}{cos 30}=43.9 N[/tex]