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4. (a) Two particles of masses 5 kg and 7 kg are connected by a taut, light, inextensible string which passes over a smooth light pulley - Leaving Cert Applied Maths - Question 4 - 2010

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4.-(a)-Two-particles-of-masses-5-kg-and-7-kg-are-connected-by-a-taut,-light,-inextensible-string-which-passes-over-a-smooth-light-pulley-Leaving Cert Applied Maths-Question 4-2010.png

4. (a) Two particles of masses 5 kg and 7 kg are connected by a taut, light, inextensible string which passes over a smooth light pulley. The system is released fro... show full transcript

Worked Solution & Example Answer:4. (a) Two particles of masses 5 kg and 7 kg are connected by a taut, light, inextensible string which passes over a smooth light pulley - Leaving Cert Applied Maths - Question 4 - 2010

Step 1

Find (i) the common acceleration of the particles

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Answer

To find the common acceleration of the system, we set up the equations of motion based on Newton's second law.

For the 5 kg particle:

  1. The net force acting on it is given as: T5g=5aT - 5g = 5a

For the 7 kg particle:

  1. The net force acting on it is given as: 7gT=7a7g - T = 7a

Where:

  • ( g \approx 10 , \text{m/s}^2 )
  • ( T ) is the tension in the string and ( a ) is the common acceleration.

Adding these two equations will help eliminate the tension:

7g5g=5a+7a7g - 5g = 5a + 7a

Substituting ( g ):

2g=12a2g = 12a

Thus,

a=2g12=g6=106=53 m/s2a = \frac{2g}{12} = \frac{g}{6} = \frac{10}{6} = \frac{5}{3} \text{ m/s}^2

Step 2

Find (ii) the tension in the string

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Answer

To find the tension in the string, we substitute ( a ) into one of the original equations. Using the equation for the 5 kg particle:

T5g=5aT - 5g = 5a

Substituting the known values:

T5×10=5×53T - 5 \times 10 = 5 \times \frac{5}{3}

This simplifies to:

T50=253T - 50 = \frac{25}{3}

Adding 50 to both sides:

T=253+50=253+1503=175358.3NT = \frac{25}{3} + 50 = \frac{25}{3} + \frac{150}{3} = \frac{175}{3} \approx 58.3 \, \text{N}

Step 3

Find (i) Show on separate diagrams the forces acting on each particle

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Answer

For the 8 kg mass on a rough horizontal plane:

  • The forces acting on the mass are:
    • Weight (8g downward)
    • Normal reaction force (R upwards)
    • Tension (T to the right)
    • Frictional force (( \mu R ) to the left)

The force diagram will depict these forces.

For the 10 kg mass on the inclined plane:

  • The forces acting on the mass are:
    • Weight (10g downward)
    • Normal reaction force (R upwards, at 30 degrees to the plane)
    • Tension (T upwards along the plane)

The angles and direction of these forces should also be noted in the force diagram.

Step 4

Find (ii) the common acceleration of the masses

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Answer

For the 8 kg mass on the horizontal plane:

Using the equation of motion:

  1. The forces acting on the mass can be summarized as: TμR=8aT - \mu R = 8a with ( R = 8g ) because it is on a horizontal surface: Therefore, Tμ(8g)=8aT - \mu (8g) = 8a

For the 10 kg mass on the inclined plane:

  1. Setting up the equation for the 10 kg mass: 10gsin(30)T=10a10g \sin(30^\circ) - T = 10a where ( \sin(30^\circ) = \frac{1}{2} ): Thus, 5T=10a5 - T = 10a

Now solve the two equations simultaneously. From the first equation, substituting for T gives:

T=10gsin(30)10a=510aT = 10g \sin(30^\circ) - 10a = 5 - 10a

Combining this with the equation from the 8 kg mass leads to:

Solving will yield the common acceleration ( a ).

Step 5

Find (iii) the tension in the string

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Answer

Using the values determined for ( a ) in the second part, substitute back into the equation for T:

From the mass on the horizontal plane: T=8a+μRT = 8a + \mu R

Calculating ( R ) gives you: R=8g=80NR = 8g = 80 \, \text{N} Thus: T=8×a+μ×80T = 8 \times a + \mu \times 80

Substituting known values for ( a ) and ( \mu ) will give the result for the tension in the string.

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