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Question: Two blocks \(A\) and \(B\) each of equal masses \(m\) are released from the top of a smooth fixed we...

Two blocks AA and BB each of equal masses mm are released from the top of a smooth fixed wedge as shown in the figure. Find the magnitude of the acceleration of the centre of mass of the two blocks.

Explanation

Solution

The acceleration of the centre of the mass is determined by using the vector equation of the acceleration of the two masses. The vector equation of the blockAA and the vector equation of the block BB is used to find the magnitude of the acceleration of the centre of mass.

Complete step by step answer:
Given that, the block AA and the block BB, both are having the same mass mm,the block AA is sliding in the inclination of the surface of 30{30^ \circ } and the block BB is sliding in the inclination of the surface of 60{60^ \circ }.Now, the force can be defined as the product of the mass of the object and the acceleration of the object.Let consider the inclination with respect to the x axis. So, the acceleration of the two mass in the vector form is,
The acceleration vector equation of the block AA is,
aA=mgsin30i^{\vec a_A} = mg\sin {30^ \circ }\hat i
The acceleration vector equation of the block BB is,
aB=mgsin60j^{\vec a_B} = mg\sin {60^ \circ }\hat j
Now, the acceleration of the centre of the mass of the two blocks can be written as,
acm=mgsin30i^+mgsin60j^mA+mB{\vec a_{cm}} = \dfrac{{mg\sin {{30}^ \circ }\hat i + mg\sin {{60}^ \circ }\hat j}}{{{m_A} + {m_B}}}
Here the mass of the two blocks are same, then

acm=mgsin30i^+mgsin60j^2m{\vec a_{cm}} = \dfrac{{mg\sin {{30}^ \circ }\hat i + mg\sin {{60}^ \circ }\hat j}}{{2m}}
From the trigonometry, the values of sin30=12\sin {30^ \circ } = \dfrac{1}{2} and the sin60=32\sin {60^ \circ } = \dfrac{{\sqrt 3 }}{2}, then the above equation is written as,
acm=mg(12)i^+mg(32)j^2m{\vec a_{cm}} = \dfrac{{mg\left( {\dfrac{1}{2}} \right)\hat i + mg\left( {\dfrac{{\sqrt 3 }}{2}} \right)\hat j}}{{2m}}
By taking the common terms from the above equation, then
acm=mg4m(i^+3j^){\vec a_{cm}} = \dfrac{{mg}}{{4m}}\left( {\hat i + \sqrt 3 \hat j} \right)
By cancelling the terms in the above equation, then
acm=g4(i^+3j^){\vec a_{cm}} = \dfrac{g}{4}\left( {\hat i + \sqrt 3 \hat j} \right)

By changing the vector equation to the magnitude, then
acm=g412+(3)2{a_{cm}} = \dfrac{g}{4}\sqrt {{1^2} + {{\left( {\sqrt 3 } \right)}^2}}
On further simplification in the above equation, then
acm=g44{a_{cm}} = \dfrac{g}{4}\sqrt 4
By taking the square root in the above equation, then
acm=g4×2{a_{cm}} = \dfrac{g}{4} \times 2
On dividing the terms in the above equation, then
acm=g2\therefore{a_{cm}} = \dfrac{g}{2}
Thus, the above equation shows the centre of the mass.

Note: When the two blocks are sliding in the inclined plane, then the acceleration of the centre of the mass of the two blocks is determined by using the trigonometric function. While using the trigonometric function, the students will give more concentration in the first step which shows the acceleration of the centre of the mass.