In figure, two blocks are separated by a uniform strut attached to each block with frictionless pins, block $ A $ weighs $ 400N $ , block $ B $ weighs $ 300N $ and the strut $ AB $ weigh $ 200N $ . If $ \mu = 0.25 $ under $ B $ , determine the minimum coefficient of friction under $ A $ to prevent motion.
$ \left( A \right)0.4 \\
\left( B \right)0.2 \\
\left( C \right)0.8 \\
\left( D \right)0.1 \\ $
Answer
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Hint :In order to solve this question, we are first going to draw the free body diagrams for the three structures, the strut, the block at point $ A $ and that at the point $ B $ . After that, we are going to write the equilibrium equations for the three and try to find out the forces acting on the elements, then the coefficient of friction is found.
Formula used: The free body diagram and its equilibrium conditions can be used to solve this question.
The frictional force that is acting on the two blocks is given by the formula.
$ {F_{A}} = {\mu _A}{N_A} $
Complete Step By Step Answer:
Consider the free body diagram of the structure, for the strut and for the two blocks
For free body diagram of the strut, applying the equilibrium equations
$ {A_V} + {B_V} = 200N - - - \left( i \right) \\
{A_H} = {B_H} - - - - \left( {ii} \right) \\ $
Where $ {A_H} $ and $ {A_V} $ are the horizontal components of the forces due to $ A $
For the block $ B $
$ {B_H} + {F_B}\cos {60^ \circ } - {N_B}\sin {60^ \circ } = 0 \\
{N_B}cos{60^ \circ } - {B_V} - 300 + {F_V}sin{60^ \circ } = 0 \\ $
Now as we know that
$ {F_B} = 0.25{N_{B}} $
Thus the above equations become
$ {B_H} - 0.74{N_B} = 0.....(iii) \\
- {B_V} + 0.71{N_B} = 300.....(iv) \\ $
Now for the block $ A $
$ {F_A} - {A_H} = 0.....(v) \\
{N_{A}} - {A_V} = 400 \\ $
As we know that
$ {F_{A}} = {\mu _A}{N_A} $
Putting this in $ (v) $ , we get
$ \therefore {\mu _{A}}{N_A} - {A_H} = 0.....(vi) $
Thus, on solving these equations, we get
$ {N_A} = 650N $
$ {F_A} = 260N $
Now as we already know that
$ {F_{A}} = {\mu _A}{N_A} $
Therefore, we get
$ {\mu _A} = \dfrac{{260}}{{250}} = 0.4 $
Note :
It is important to note that you cannot just put the equations for the forces of friction, gravity and other directly to show the equilibrium conditions of the strut and the blocks, it is very important to have a free body diagram for the three to give us an insight of what the directions of the forces are and what effect they are having.
Formula used: The free body diagram and its equilibrium conditions can be used to solve this question.
The frictional force that is acting on the two blocks is given by the formula.
$ {F_{A}} = {\mu _A}{N_A} $
Complete Step By Step Answer:
Consider the free body diagram of the structure, for the strut and for the two blocks
For free body diagram of the strut, applying the equilibrium equations
$ {A_V} + {B_V} = 200N - - - \left( i \right) \\
{A_H} = {B_H} - - - - \left( {ii} \right) \\ $
Where $ {A_H} $ and $ {A_V} $ are the horizontal components of the forces due to $ A $
For the block $ B $
$ {B_H} + {F_B}\cos {60^ \circ } - {N_B}\sin {60^ \circ } = 0 \\
{N_B}cos{60^ \circ } - {B_V} - 300 + {F_V}sin{60^ \circ } = 0 \\ $
Now as we know that
$ {F_B} = 0.25{N_{B}} $
Thus the above equations become
$ {B_H} - 0.74{N_B} = 0.....(iii) \\
- {B_V} + 0.71{N_B} = 300.....(iv) \\ $
Now for the block $ A $
$ {F_A} - {A_H} = 0.....(v) \\
{N_{A}} - {A_V} = 400 \\ $
As we know that
$ {F_{A}} = {\mu _A}{N_A} $
Putting this in $ (v) $ , we get
$ \therefore {\mu _{A}}{N_A} - {A_H} = 0.....(vi) $
Thus, on solving these equations, we get
$ {N_A} = 650N $
$ {F_A} = 260N $
Now as we already know that
$ {F_{A}} = {\mu _A}{N_A} $
Therefore, we get
$ {\mu _A} = \dfrac{{260}}{{250}} = 0.4 $
Note :
It is important to note that you cannot just put the equations for the forces of friction, gravity and other directly to show the equilibrium conditions of the strut and the blocks, it is very important to have a free body diagram for the three to give us an insight of what the directions of the forces are and what effect they are having.
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