
Two particles A and B, each of mass m are kept stationary by applying a horizontal force F = mg on particle B as shown in figure. Then:
${\text{A}}{\text{. tan}}\beta {\text{ = 2tan}}\alpha $
${\text{B}}{\text{. 2}}{{\text{T}}_1} = 5{{\text{T}}_2}$
${\text{C}}{\text{. }}\sqrt 2 {{\text{T}}_1} = \sqrt 5 {{\text{T}}_2}$
${\text{D}}{\text{.}}$ None of these
Answer
607.5k+ views
Hint: At first draw a free body diagram for particles A and B and then resolve the forces into their components along X- axis and Y- axis.
Formula used - ${T_1}\sin \alpha = {T_2}\sin \beta $ , ${T_1}\cos \alpha = {T_2}\cos \beta + mg$ , ${T_2}\cos \beta = mg$ , ${T_2}\sin \beta = mg$
Complete Step-by-Step solution:
Let us first draw the free body diagram (FBD) for both the particles A and B.
Refer the image shown (FBD)-
Here $a = \alpha ,b = \beta $ .
Now resolving these forces into their components along X- axis and Y- axis, we get-
From the FBD of A,
${T_1}\sin \alpha = {T_2}\sin \beta - (1)$
${T_1}\cos \alpha = {T_2}\cos \beta + mg - (2)$
Now from the FBD of B,
${T_2}\cos \beta = mg - (3)$
${T_2}\sin \beta = mg - (4)$
now dividing equation 4 by equation 3 we get-
$\dfrac{{{T_2}\sin \beta }}{{{T_2}\cos \beta }} = \dfrac{{mg}}{{mg}}$
So, we get- $\tan \beta = 1$
Using equation (4) in (1) and equation (3) in (2),
$T\sin \alpha = mg$ and $T\cos \alpha = 2mg$
So, dividing these two we get-
$\tan \alpha = \dfrac{1}{2}$
We can also write,
$
2\tan \alpha = 1 \\
\Rightarrow 2\tan \alpha = \tan \beta \{ \because \tan \beta = 1\} \\
$
It means option A is correct.
Now using $\alpha $ and $\beta $ values in (1) we get-
${T_1}\sin \alpha = {T_2}\sin \beta $
$\sqrt 2 {{\text{T}}_1} = \sqrt 5 {{\text{T}}_2}$ (option C)
Therefore, options A and C are correct.
Note – Whenever such types of questions appear then always write the things given in the question and then by drawing the FBD of A and B solve the question, as done in the solution, the forces are resolved into components and then we have found the correct options by using the equations mentioned in the solution.
Formula used - ${T_1}\sin \alpha = {T_2}\sin \beta $ , ${T_1}\cos \alpha = {T_2}\cos \beta + mg$ , ${T_2}\cos \beta = mg$ , ${T_2}\sin \beta = mg$
Complete Step-by-Step solution:
Let us first draw the free body diagram (FBD) for both the particles A and B.
Refer the image shown (FBD)-
Here $a = \alpha ,b = \beta $ .
Now resolving these forces into their components along X- axis and Y- axis, we get-
From the FBD of A,
${T_1}\sin \alpha = {T_2}\sin \beta - (1)$
${T_1}\cos \alpha = {T_2}\cos \beta + mg - (2)$
Now from the FBD of B,
${T_2}\cos \beta = mg - (3)$
${T_2}\sin \beta = mg - (4)$
now dividing equation 4 by equation 3 we get-
$\dfrac{{{T_2}\sin \beta }}{{{T_2}\cos \beta }} = \dfrac{{mg}}{{mg}}$
So, we get- $\tan \beta = 1$
Using equation (4) in (1) and equation (3) in (2),
$T\sin \alpha = mg$ and $T\cos \alpha = 2mg$
So, dividing these two we get-
$\tan \alpha = \dfrac{1}{2}$
We can also write,
$
2\tan \alpha = 1 \\
\Rightarrow 2\tan \alpha = \tan \beta \{ \because \tan \beta = 1\} \\
$
It means option A is correct.
Now using $\alpha $ and $\beta $ values in (1) we get-
${T_1}\sin \alpha = {T_2}\sin \beta $
$\sqrt 2 {{\text{T}}_1} = \sqrt 5 {{\text{T}}_2}$ (option C)
Therefore, options A and C are correct.
Note – Whenever such types of questions appear then always write the things given in the question and then by drawing the FBD of A and B solve the question, as done in the solution, the forces are resolved into components and then we have found the correct options by using the equations mentioned in the solution.
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