Online Test — System of Particles and Rotational Motion
18 Questions • 15 min • Chapter MCQ
15:00
Question 1 of 18
The centre of mass of a system is the:
heaviest particle
mass-weighted average position
geometric corner
fastest particle
Explanation: By definition $\vec{r}_{cm}=\frac{\sum m_i \vec{r}_i}{\sum m_i}$.
Question 2 of 18
Masses 1 kg and 4 kg are 10 m apart. The CM is at a distance from the 1 kg mass of:
$2\ \text{m}$
$5\ \text{m}$
$8\ \text{m}$
$10\ \text{m}$
Explanation: $x_{cm}=\frac{4\times10}{5}=8\ \text{m}$ from the 1 kg mass.
Question 3 of 18
Total momentum of a system of particles equals:
$M\vec{a}_{cm}$
$M\vec{v}_{cm}$
$\sum m_i$
$M\vec{r}_{cm}$
Explanation: $\vec{P}=M\vec{v}_{cm}$.
Question 4 of 18
The centre of mass moves under the influence of:
internal forces
net external force only
no force
friction only
Explanation: $M\vec{a}_{cm}=\vec{F}_{ext}$; internal forces cancel.
Question 5 of 18
The magnitude of torque is given by:
$rF$
$rF\cos\theta$
$rF\sin\theta$
$rF\tan\theta$
Explanation: $\vec{\tau}=\vec{r}\times\vec{F}$, so $\tau=rF\sin\theta$.
Question 6 of 18
The SI unit of torque is:
$\text{N}$
$\text{J}$
$\text{N m}$
$\text{W}$
Explanation: Torque is measured in newton metre.
Question 7 of 18
A force of 10 N acts perpendicular at 0.5 m from the axis. The torque is:
$2\ \text{N m}$
$5\ \text{N m}$
$10\ \text{N m}$
$20\ \text{N m}$
Explanation: $\tau=rF\sin90^\circ=0.5\times10=5\ \text{N m}$.
Question 8 of 18
Moment of inertia is given by:
$\sum m_i r_i$
$\sum m_i r_i^2$
$\sum m_i^2 r_i$
$\sum m_i/r_i$
Explanation: $I=\sum m_i r_i^2$.
Question 9 of 18
The moment of inertia of a solid disc of mass $M$, radius $R$ about its axis is:
$MR^2$
$\frac{1}{2}MR^2$
$\frac{2}{5}MR^2$
$\frac{1}{12}MR^2$
Explanation: For a solid disc/cylinder $I=\frac{1}{2}MR^2$.
Question 10 of 18
The radius of gyration $k$ is defined by:
$I=Mk$
$I=Mk^2$
$I=M/k^2$
$I=k/M$
Explanation: $I=Mk^2$, so $k=\sqrt{I/M}$.
Question 11 of 18
Angular momentum of a rigid body about a fixed axis is:
$I\alpha$
$I\omega$
$\frac{1}{2}I\omega^2$
$\tau\theta$
Explanation: $L=I\omega$.
Question 12 of 18
When the net external torque is zero, the conserved quantity is:
kinetic energy
angular momentum
torque
moment of inertia
Explanation: $\frac{dL}{dt}=\tau_{ext}=0$, so $L$ is constant.
Question 13 of 18
An ice-skater pulling in the arms while spinning will:
slow down
stop
spin faster
stay the same
Explanation: $I$ decreases, so $\omega$ increases to keep $L=I\omega$ constant.
Question 14 of 18
The rotational analogue of Newton's second law is:
$L=I\omega$
$\tau=I\alpha$
$v=\omega R$
$KE=\frac{1}{2}I\omega^2$
Explanation: $\tau=I\alpha$ mirrors $F=ma$.
Question 15 of 18
The rotational kinetic energy of a body is:
$I\omega$
$\frac{1}{2}I\omega^2$
$\frac{1}{2}I\omega$
$I\omega^2$
Explanation: $KE_{rot}=\frac{1}{2}I\omega^2$.
Question 16 of 18
For rolling without slipping, the centre velocity satisfies:
$v=\omega/R$
$v=\omega R$
$v=R/\omega$
$v=\omega R^2$
Explanation: The contact point is at rest, giving $v=\omega R$.
Question 17 of 18
The total kinetic energy of a rolling body is:
$\frac{1}{2}mv^2$
$\frac{1}{2}I\omega^2$
$\frac{1}{2}mv^2+\frac{1}{2}I\omega^2$
$mv^2+I\omega^2$
Explanation: Rolling KE is the sum of translational and rotational parts.
Question 18 of 18
A solid sphere, a disc and a ring roll down the same incline. The one reaching the bottom first is the:
ring
disc
solid sphere
all together
Explanation: The sphere has the smallest $k^2/R^2$, hence the largest acceleration.