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Question: In an experiment with a beam balance on unknown mass \(m\) is balanced by two known mass \(m\) is ba...

In an experiment with a beam balance on unknown mass mm is balanced by two known mass mm is balanced by two known masses of 16  kg16\;{\rm{kg}} and 4  kg4\;{\rm{kg}} as shown in figure. Find the value of unknown mass mm in kgkg.

Explanation

Solution

Here, we will use the principle of moments. We will apply this principle for the balance in both the figures and solve the obtained equations.

Complete step by step answer: The moment of force about a point of rotation can be written as
τ=r×F =rFsinθ\begin{array}{c} \tau = \overrightarrow r \times \overrightarrow F \\\ = rF\sin \theta \end{array}

where rr is the perpendicular distance from the line of application of force FF to the point of rotation and θ\theta is the angle between r\overrightarrow r and F\overrightarrow F .

In the given spring balance, two masses are hanged from the ends of the bar. Moment of force or torque acts about the point of rotation due to each mass. In the case of the spring balance, we see that θ=90\theta = 90^\circ . Hence, the torque due to a particular mass MM can be written as
$

τ=rFsin90 rF\begin{aligned} \tau &= rF\sin 90^\circ \\\ \Rightarrow &rF \end{aligned}

Since SinceF = Mg$,

τ=Mgr\tau = Mgr

In the first figure, let m1=16  kg{m_1} = 16\;{\rm{kg}}. Then, we say that the spring balance is balanced by two masses m1{m_1} and mm. The moment due to one mass acts in the clockwise direction and the moment due to the other mass acts in the anticlockwise direction.

From the principle of moments, the moment of force acting in the clockwise direction is equal to the moment acting in the anticlockwise direction for a balanced body. Hence, we write

τm=τ1{\tau _m} = {\tau _1}

Here τm{\tau _m} is the moment of force due to mass mm and τ1{\tau _1} is the moment of force due to mass m1{m_1}. So, similar to the torque equation τ=Mgr\tau = Mgr, we write

mgl2=m1gl1mg{l_2} = {m_1}g{l_1}
ml2=m1l1m{l_2} = {m_1}{l_1}

Since m1=16  kg{m_1} = 16\;{\rm{kg}}, we get
ml2=16l1m{l_2} = 16{l_1} ……(1)
Similarly, for the second figure, let m2=4  kg{m_2} = 4\;{\rm{kg}}. Applying the principle of moments, we get
ml1=m2l2m{l_1} = {m_2}{l_2}
Since m2=4  kg{m_2} = 4\;{\rm{kg}},
ml1=4l2m{l_1} = 4{l_2}
l1l2=4m\dfrac{{{l_1}}}{{{l_2}}} = \dfrac{4}{m} ……(2)
Now, we will divide equation (1) by (2). Hence, we get
m=8

Therefore, the value of mass mm is 8  kg8\;{\rm{kg}}.

Note: If m1{m_1} and m2{m_2} are two masses hanging from two points of a balanced body and r1{r_1} and r2{r_2} are the distances of the masses from the axis of rotation of the body, then m1r1=m2r2{m_1}{r_1} = {m_2}{r_2}. We can directly apply this equation in problems which mention that the body is balanced.