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Question 6
A box of mass 30 kg is being pulled along rough horizontal ground at a constant speed using a rope. The rope makes an angle of 20° with the ground, as shown in Figur... show full transcript
Step 1
Answer
To find the force P, we start by analyzing the forces acting on the box in the vertical direction. The normal force R and the weight of the box must balance the vertical component of the tension in the rope:
The weight of the box is calculated as:
The vertical component of the tension P can be expressed as:
The equation in the vertical direction can be set up as:
The horizontal forces also include the frictional force, which is given by:
Therefore:
We know that the box moves at a constant speed, which means the net force is zero. We can combine the two previous equations:
Now we can substitute R from the friction equation to find P:
Technically, we would solve for R first:
R = rac{P ext{cos}(20°)}{μ}
Plugging this back into our equations and solving gives:
P ext{cos}(20°) + rac{P ext{cos}(20°)}{0.4} = 30g
Rearranging and solving for P leads to:
P ext{cos}(20°) imes (1 + rac{1}{0.4}) = 30 imes 9.81
Computing gives:
P = rac{294.3}{3.5 ext{cos}(20°)}
Step 2
Answer
With the tension increased to 150 N, we can now analyze the forces acting on the box once more to find the acceleration.
The normal force R in this case can again be derived from the forces:
Re-arranging to find R gives:
We substitute for R in the friction equation:
The net force acting on the box gives:
By using Newton’s second law, we can state:
Knowing that the mass m = 30 kg, we can express:
a = rac{150 ext{cos}(20°) - μR}{m}
Plugging in the values from the previous sections allows us to calculate:
a = rac{150 ext{cos}(20°) - 0.4(30g - 150 ext{sin}(20°))}{30}
Finally, work through the calculations to arrive at a value for acceleration around 1.5 m/s² (or approximately 1.46).
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