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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 of B, we start by analyzing the forces acting on both particles A and B.
For particle A (mass = 7 kg), the forces acting are:
From Newton's second law, we can write:
For particle B (mass = 3 kg), along the plane:
Where is the normal force acting on B.
Thus, along the plane:
Substituting for R:
ightarrow F_{friction} = \frac{2}{3}(3g \cos \theta) = 2g \cos \theta$$ So the equation for B becomes: $$T - 3g \sin \theta - 2g \cos \theta = 3a ag{3}$$ ### System of Equations: Now we can solve Equations (1) and (3). First, substituting $\sin \theta$ and $\cos \theta$ from $tan \theta = \frac{5}{12}$: - $\sin \theta = \frac{5}{13}$ - $\cos \theta = \frac{12}{13}$ Now substitute these into (3): 1. Substitute into Equation (1) to express T: \[ T = 7g - 7a \tag{4} \] 2. Substitute $\sin \theta$ and $\cos \theta$ into Equation (3) to get: \[ (7g - 7a) - 3g \cdot \frac{5}{13} - 2g \cdot \frac{12}{13} = 3a \tag{5} \] Rearranging gives: \[ 7g - 7a - \frac{15g}{13} - \frac{24g}{13} = 3a \rightarrow \frac{91g - 39g}{13} = 10a \] Simplifying leads to: \[ 52g = 10a\qquad a = \frac{26g}{5} \tag{6} \] Substituting $g \approx 9.8 ext{ m/s}^2$ results in: \[ a \approx 5.088 m/s^{2} ext{ or } 5.09 m/s^{2}.\]Step 2
Step 3
Answer
After the string breaks, the forces acting on particle B are:
This can be simplified to: which is the deceleration B experiences.
Using the kinematic equation: where , (final speed at rest), .
Thus, which leads to solving for : $$t \approx \frac{3.19}{3g\cdot 0.1846} \approx 0.229 s.$
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