In an experiment with a beam balance on unknown mass $m$ is balanced by two known mass $m$ is balanced by two known masses of $16\;{\rm{kg}}$ and $4\;{\rm{kg}}$ as shown in figure. Find the value of unknown mass $m$ in $kg$.
Answer
648.9k+ views
Hint: 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
$\begin{array}{c}
\tau = \overrightarrow r \times \overrightarrow F \\
= rF\sin \theta
\end{array}$
where $r$ is the perpendicular distance from the line of application of force $F$ to the point of rotation and $\theta $ is the angle between $\overrightarrow r $ and $\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 $\theta = 90^\circ $. Hence, the torque due to a particular mass $M$ can be written as
$
\begin{align*}
\tau &= rF\sin 90^\circ \\
\Rightarrow &rF
\end{align*}
$
Since $F = Mg$,
$\tau = Mgr$
In the first figure, let ${m_1} = 16\;{\rm{kg}}$. Then, we say that the spring balance is balanced by two masses ${m_1}$ and $m$. 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
${\tau _m} = {\tau _1}$
Here ${\tau _m}$ is the moment of force due to mass $m$ and ${\tau _1}$ is the moment of force due to mass ${m_1}$. So, similar to the torque equation $\tau = Mgr$, we write
$mg{l_2} = {m_1}g{l_1}$
$m{l_2} = {m_1}{l_1}$
Since ${m_1} = 16\;{\rm{kg}}$, we get
$m{l_2} = 16{l_1}$ ……(1)
Similarly, for the second figure, let ${m_2} = 4\;{\rm{kg}}$. Applying the principle of moments, we get
$m{l_1} = {m_2}{l_2}$
Since ${m_2} = 4\;{\rm{kg}}$,
$m{l_1} = 4{l_2}$
$\dfrac{{{l_1}}}{{{l_2}}} = \dfrac{4}{m}$ ……(2)
Now, we will divide equation (1) by (2). Hence, we get
m=8
Therefore, the value of mass $m$ is $8\;{\rm{kg}}$.
Note:If ${m_1}$ and ${m_2}$ are two masses hanging from two points of a balanced body and ${r_1}$ and ${r_2}$ are the distances of the masses from the axis of rotation of the body, then ${m_1}{r_1} = {m_2}{r_2}$. We can directly apply this equation in problems which mention that the body is balanced.
Complete step by step answer:The moment of force about a point of rotation can be written as
$\begin{array}{c}
\tau = \overrightarrow r \times \overrightarrow F \\
= rF\sin \theta
\end{array}$
where $r$ is the perpendicular distance from the line of application of force $F$ to the point of rotation and $\theta $ is the angle between $\overrightarrow r $ and $\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 $\theta = 90^\circ $. Hence, the torque due to a particular mass $M$ can be written as
$
\begin{align*}
\tau &= rF\sin 90^\circ \\
\Rightarrow &rF
\end{align*}
$
Since $F = Mg$,
$\tau = Mgr$
In the first figure, let ${m_1} = 16\;{\rm{kg}}$. Then, we say that the spring balance is balanced by two masses ${m_1}$ and $m$. 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
${\tau _m} = {\tau _1}$
Here ${\tau _m}$ is the moment of force due to mass $m$ and ${\tau _1}$ is the moment of force due to mass ${m_1}$. So, similar to the torque equation $\tau = Mgr$, we write
$mg{l_2} = {m_1}g{l_1}$
$m{l_2} = {m_1}{l_1}$
Since ${m_1} = 16\;{\rm{kg}}$, we get
$m{l_2} = 16{l_1}$ ……(1)
Similarly, for the second figure, let ${m_2} = 4\;{\rm{kg}}$. Applying the principle of moments, we get
$m{l_1} = {m_2}{l_2}$
Since ${m_2} = 4\;{\rm{kg}}$,
$m{l_1} = 4{l_2}$
$\dfrac{{{l_1}}}{{{l_2}}} = \dfrac{4}{m}$ ……(2)
Now, we will divide equation (1) by (2). Hence, we get
m=8
Therefore, the value of mass $m$ is $8\;{\rm{kg}}$.
Note:If ${m_1}$ and ${m_2}$ are two masses hanging from two points of a balanced body and ${r_1}$ and ${r_2}$ are the distances of the masses from the axis of rotation of the body, then ${m_1}{r_1} = {m_2}{r_2}$. We can directly apply this equation in problems which mention that the body is balanced.
Recently Updated Pages
Write structures of the following compounds i 2 Chloro3methylpentane class 11 chemistry CBSE

What is BLO What is the full form of BLO class 8 social science CBSE

Explain the Treaty of Vienna of 1815 class 10 social science CBSE

A Paragraph on Pollution in about 100-150 Words

XIX+XXX A 49 B 51 C 55 D 44 class 5 maths CBSE

If x a + bt + ct2 where x is in meters and t is in class 11 physics CBSE

Trending doubts
One Metric ton is equal to kg A 10000 B 1000 C 100 class 11 physics CBSE

Draw a diagram of nephron and explain its structur class 11 biology CBSE

10 examples of friction in our daily life

Proton was discovered by A Thomson B Rutherford C Chadwick class 11 chemistry CBSE

Bond order ofO2 O2+ O2 and O22 is in order A O2 langle class 11 chemistry CBSE

Draw a labelled diagram of the neuron and describe class 11 biology CBSE

