Question

A uniform horizontal meter scale of mass m is suspended by two vertical strings attached to its two ends. A body of mass $2m$ is placed on the $75cm$ mark. The tensions in the two strings are in the ratio:
$\left( a \right){\text{ 1:2}}$
$\left( b \right){\text{ 1:3}}$
$\left( c \right){\text{ 2:3}}$
$\left( d \right){\text{ 3:4}}$

Answer 1

Hint So here to solve this type of problem, we should have the basic knowledge of the tension. Firstly we will take out the rotational equilibrium which will be corresponding to the $T1$. And in the same way, we will find them $T2$ , and then we will be able to find the ratio of the tension in the string.

Complete Step By Step Solution First of all we all know, according to the question the net tension produced will be equal to the sum of the two tension applied to it.

Here,
$\Rightarrow T1 + T2 = 2mg + 1mg$
So it will be equal to the
$\Rightarrow T1 + T2 = 3mg$
Now taking tension about the left side of the plank, we will get
$\Rightarrow 0.5mg + 0.75 \times 2mg = 1 \times T2$
And from here, on solving the above equation we will the values as
$\Rightarrow T2 = 2mg$
And similarly, another torque will be
$\Rightarrow T1 = mg$
Now we have to find the ratios, therefore the ratio of the tension will be given by
$\Rightarrow \dfrac{{T1}}{{T2}} = \dfrac{{mg}}{{2mg}}$
And on solving the above, we will get
$\Rightarrow \dfrac{{T1}}{{T2}} = \dfrac{1}{2}$
Therefore, we can say that
$\dfrac{1}{2}$, will be the ratio of the tension in the strings.

Hence, the option $\left( a \right)$ is correct.

Note As we know the pressure force is the total force compressed matter exerts longitudinally - i.e. the sum of pressure x cross-section area across all parts of the total cross-section. (In math terms, the integral of pressure across the total cross-section.)
So the tension is just the opposite: The integral of tensile stress across the total cross-section. In other words, the total force that tries to stretch a body of matter.
So we can say that the pressure or, respectively, tensile stress (the difference is only in the sign) in the matter is commonly called stress.