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Question 7
Two particles A and B, of mass 7 kg and 3 kg respectively, are attached to the ends of a light inextensible string. Initially B is held at rest on a rough fixed plan... show full transcript
Step 1
Answer
To find the acceleration, we analyze the forces acting on both particles A and B. For particle A:
The weight of A acts downwards (7g). Hence, the tension T in the string can be described by the equation:
For particle B: The forces are the tension T acting upwards and the weight of B and the friction force acting down the plane. The equations are:
where F is the friction force and is given by:
F = μR = rac{2}{3} R
The normal force R acting on B is given by:
We can substitute R into the friction equation:
F = rac{2}{3}(3g ext{cos}θ) = 2g ext{cos}θ
Substituting this into the equation for B:
We can solve the equations together:
By eliminating T from the two equations:
Re-arranging gives:
By substituting an θ = rac{5}{12}, we find the values of sin and cos:
ext{sin}θ = rac{5}{13}, ext{cos}θ = rac{12}{13}
Finally, substituting into the equation gives:
a = rac{2g}{5} ext{ or } 3.92 ext{ m/s}^2.
Step 2
Answer
Using the equations of motion for B:
The initial velocity u = 0, the distance s = 1 m, and the acceleration a is already calculated as rac{2g}{5}. The equation used here is:
Substituting our values:
v^2 = 0 + 2 imes rac{2g}{5} imes 1
Therefore:
ho{2g}{5} = 2.8 ext{ m/s}$$.
Step 3
Answer
When B has moved 1 m up the plane, the forces on B balance out:
The net force on B at this point is:
Therefore:
rac{2}{3} imes 3g ext{cos}θ + 3g ext{sin}θ = 3a
We substitute the known values:
rac{2}{3} imes 3g imes rac{12}{13} + 3g imes rac{5}{13} = 3(-a)
Simplifying gives us:
t = rac{2}{7} ext{ seconds} ext{ or } 0.286 ext{ seconds}.
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