A nearly massless rod is pivoted at one end so that it can swing freely like a pendulum. Two masses \[m\] and \[2m\] are attached to it at distances \[b\] and \[3b\]respectively from the pivot. The rod is held horizontal and then released. The angular acceleration of the rod at the instant it is released is
\[(a)bg\]
\[(b)\dfrac{b}{g}\;\]
\[(c)bg + 5\;\]
\[(d)\dfrac{{5g}}{{11b}}\]
Answer
557.1k+ views
Hint:From the question, we can take that the masses separated by the given distances experience a torque when in rotation. This rotational torque is related to its angular acceleration by taking into consideration its moment of inertia and the distance between the two. Finally, by equating the two relations we will be able to obtain the value of the torque.
Complete step-by-step solution:
A nearly massless rod is pivoted at one end and is separated by distances \[b\] and \[3b\] which is as shown below such that it can swing freely like a pendulum attached to it of masses \[m\] and \[2m\]
When a torque is applied to an object it starts to rotate with an acceleration that is inversely proportional to its moment of inertia $I$. This relation is called Newton’s Second Law for rotation.
Initially, we find the torque that is given by
Torque$\tau = \,m \times r$ we get for different masses at distances
$\tau = \,(2mg \times b + \,mg \times 3b)$
$\tau = 5mgb$…..this is equation 1
Also, the moment of inertia for the rods could be derived and is given by $I = \,m{r^2}$
For masses \[m\] and \[2m\] at distances, \[b\] and \[3b\] we get the moment of inertia is
${I_1} = 2m{b^2}$
And ${I_2} = 9m{b^2}$
Therefore, $I = {I_1} + {I_2} = 11m{b^2}$……this is equation 2
If it's a frictionless pendulum that keeps on swinging forever (unless there's air friction), here we relate the angular acceleration to the moment of inertia and torque
Torque $\tau = \,I \times \alpha $
We get from the equation 1 and 2
$\tau = \,5m{b^2} \times \alpha $
$5mgb = 11m{b^2} \times \alpha $
From this equation, we conclude $\alpha = \dfrac{{5g}}{{11b}}$(option D)
Note:It is sure to obtain the required torque for the two masses that are being placed at different distances when it is taken as a pendulum that is freely rotating. This rotational inertia depends upon the mass of an object and how it is distributed to the axis of rotation. This also helps to determine how much force it would take to rotate a body.
Complete step-by-step solution:
A nearly massless rod is pivoted at one end and is separated by distances \[b\] and \[3b\] which is as shown below such that it can swing freely like a pendulum attached to it of masses \[m\] and \[2m\]
When a torque is applied to an object it starts to rotate with an acceleration that is inversely proportional to its moment of inertia $I$. This relation is called Newton’s Second Law for rotation.
Initially, we find the torque that is given by
Torque$\tau = \,m \times r$ we get for different masses at distances
$\tau = \,(2mg \times b + \,mg \times 3b)$
$\tau = 5mgb$…..this is equation 1
Also, the moment of inertia for the rods could be derived and is given by $I = \,m{r^2}$
For masses \[m\] and \[2m\] at distances, \[b\] and \[3b\] we get the moment of inertia is
${I_1} = 2m{b^2}$
And ${I_2} = 9m{b^2}$
Therefore, $I = {I_1} + {I_2} = 11m{b^2}$……this is equation 2
If it's a frictionless pendulum that keeps on swinging forever (unless there's air friction), here we relate the angular acceleration to the moment of inertia and torque
Torque $\tau = \,I \times \alpha $
We get from the equation 1 and 2
$\tau = \,5m{b^2} \times \alpha $
$5mgb = 11m{b^2} \times \alpha $
From this equation, we conclude $\alpha = \dfrac{{5g}}{{11b}}$(option D)
Note:It is sure to obtain the required torque for the two masses that are being placed at different distances when it is taken as a pendulum that is freely rotating. This rotational inertia depends upon the mass of an object and how it is distributed to the axis of rotation. This also helps to determine how much force it would take to rotate a body.
Recently Updated Pages
Which will be the least stable resonating structure class 11 chemistry CBSE

How many 5 digit telephone numbers can be construc-class-11-maths-CBSE

How do you find the angle of the resultant vector class 11 physics CBSE

Draw labelled diagram of the following i Gram seed class 11 biology CBSE

What is the need and importance of classification class 11 biology CBSE

The way in which the sparrows expressed their sorrow class 11 english CBSE

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

Find the value of the expression given below sin 30circ class 11 maths CBSE

1 Quintal is equal to a 110 kg b 10 kg c 100kg d 1000 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

