The angle of the force is ![51.1^{\circ}](https://tex.z-dn.net/?f=51.1%5E%7B%5Ccirc%7D)
Explanation:
To solve this problem, we can apply Newton's second law along the horizontal direction of motion of the suitcase:
![\sum F_x = ma_x](https://tex.z-dn.net/?f=%5Csum%20F_x%20%3D%20ma_x)
where
is the net force along the x-axis
m is the mass of the suitcase
is the acceleration along the x-axis
The suitcase is moving at constant speed, so the acceleration is zero:
![a_x=0](https://tex.z-dn.net/?f=a_x%3D0)
Therefore the net force must also be zero:
(1)
We have two forces acting along the horizontal direction:
- The component of the push (forward) in the horizontal direction,
, with
F = 43 N
= angle of the force with the horizontal
- The force of friction,
, backward
So the net force can be written as
(2)
Combining (1) and (2),
![F cos \theta - F_f = 0](https://tex.z-dn.net/?f=F%20cos%20%5Ctheta%20-%20F_f%20%3D%200)
And so we can find the angle:
![\theta = cos^{-1}(\frac{F_f}{F})=cos^{-1}(\frac{27}{43})=51.1^{\circ}](https://tex.z-dn.net/?f=%5Ctheta%20%3D%20cos%5E%7B-1%7D%28%5Cfrac%7BF_f%7D%7BF%7D%29%3Dcos%5E%7B-1%7D%28%5Cfrac%7B27%7D%7B43%7D%29%3D51.1%5E%7B%5Ccirc%7D)
Learn more about Newton's second law:
brainly.com/question/3820012
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