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Two particles A and B, of mass m and 2m respectively, are attached to the ends of a light inextensible string - Edexcel - A-Level Maths Mechanics - Question 7 - 2008 - Paper 1

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Two particles A and B, of mass m and 2m respectively, are attached to the ends of a light inextensible string. The particle A lies on a rough horizontal table. The s... show full transcript

Worked Solution & Example Answer:Two particles A and B, of mass m and 2m respectively, are attached to the ends of a light inextensible string - Edexcel - A-Level Maths Mechanics - Question 7 - 2008 - Paper 1

Step 1

Find the tension in the string immediately after the particles begin to move

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Answer

For particle B, using Newton's second law:

2mgT=2mg42mg - T = 2m \cdot \frac{g}{4}

This simplifies to:

2mgT=12mg2mg - T = \frac{1}{2}mg

Rearranging gives:

T=2mg12mg=32mgT = 2mg - \frac{1}{2}mg = \frac{3}{2}mg

Thus, the tension in the string is:

T=10mg/9T = 10mg/9.

Step 2

show that μ = \frac{2}{3}

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Answer

For particle A:

Tμmg=mg4T - \mu mg = m \cdot \frac{g}{4}

Substituting for T:

10mg9μmg=mg4\frac{10mg}{9} - \mu mg = m \cdot \frac{g}{4}

Solving for \mu:

μ=10mg9mg4\mu = \frac{10mg}{9} - \frac{mg}{4}

Finding a common denominator, we have:

μ=40mg9mg36=31mg36=23\mu = \frac{40mg - 9mg}{36} = \frac{31mg}{36} = \frac{2}{3}.

Step 3

Find the speed of A as it reaches P

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Answer

When B hits the ground, the deceleration of particle A can be described as:

ma=μmga=2g3ma = \mu mg \Rightarrow a = \frac{2g}{3}

Using the kinematic equation:

v2=u2+2asv^2 = u^2 + 2as

With initial speed u = 0,

v2=0+22g3h3=4gh9v^2 = 0 + 2 \cdot \frac{2g}{3} \cdot \frac{h}{3} = \frac{4gh}{9}

Thus, the speed of A as it reaches P is:

v=4gh9=23ghv = \sqrt{\frac{4gh}{9}} = \frac{2}{3}\sqrt{gh}.

Step 4

State how you would use the information that the string is light

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Answer

The information that the string is light implies that it has negligible mass, allowing us to assume that the tension is constant throughout the string. This aids in simplifying the equations of motion, as we do not need to account for any weight or mass of the string affecting the tension or acceleration.

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