Question
A particle executes simple harmonic motion (amplitude $= A$) between $x = - A$ and $x = + A$. The time taken for it to go from $0$ to $A/2$ is ${T_1}$ and to go from $A/2$ to $A$ is ${T_2}$. Then

Answer

(a)Using $x = A\sin \omega t$
For $x = A/2,\;\;\sin \omega {T_1} = 1/2 \Rightarrow {T_1} = \frac{\pi }{{6\omega }}$
For $x = A,\;\sin \omega ({T_1} + {T_2}) = 1 \Rightarrow {T_1} + {T_2} = \frac{\pi }{{2\omega }}$
$ \Rightarrow {T_2} = \frac{\pi }{{2\omega }} - {T_1} = \frac{\pi }{{2\omega }} - \frac{\pi }{{6\omega }} = \frac{\pi }{{3\omega }} $

$i.e.\;{T_1} < {T_2}$

Alternate method : In S.H.M., velocity of particle also oscillates simple harmonically. Speed is more near the mean position and less near the extreme position. Therefore the time taken for the particle to go from $0$ to $\frac{A}{2}$ will be less than the time taken to go from $\frac{A}{2}$ to $A$.

Hence ${T_1} < {T_2}.$

Need a full question paper?

Generate a complete, print-ready paper with questions like this in minutes — across 16+ boards, with answer keys.

Start Generating Free

Similar questions

To prepare a print the time taken is $5\, sec$ due to lamp of $60\, watt$ at $0.25\, m $ distance. If the distance is increased to $40 \,cm$ then what is the time taken to prepare the similar print......$sec$
A rectangular region $A B C D$ contains a uniform magnetic field $B_0$ directed perpendicular to the plane of the rectangle. A narrow stream of charged particles moving perpendicularly to the side $AB$ enters this region and is ejected through the adjacent side $B C$ suffering a deflection through $30^{\circ}$. In order to increase this deflection to $60^{\circ}$, the magnetic field has to be
A small air bubble is at the inner surface of the bottom of a beaker filled with cold water. Now water of the beaker is heated. The size of bubble increases. The reason for this may be
The electrical resistance of depletion layer is large because
The deceleration experienced by a moving motor boat, after its engine is cut-off is given by $\frac{{dv}}{{dt}} =  - k{v^3}$ , where $k$ is constant. If $v_0$ is the magnitude of the velocity at cut-off, the magnitude of the velocity at a time $t$ after the cut-off is
A particle moves along an arc of a circle of radius $R$ . Its velocity depends on the distance covered as $v = a\sqrt s$ , where $a$ is a constant then the angle $\alpha $ between the vector of the total acceleration and the vector of velocity as a function of $s$ will be
Different physical quantities are given in Column - $\mathrm{I}$ and their dimensional formula are given in Column - $\mathrm{II}$. Match them appropriately.
Column - $\mathrm{I}$ Column - $\mathrm{II}$
$(a)$ Viscous force $(i)$ $\left[ {{M^1}{L^1}{T^{ - 2}}} \right]$
$(b)$ Coefficient of viscosity $(ii)$ $\left[ {{M^1}{L^{ - 1}}{T^{ - 1}}} \right]$
  $(iii)$ $\left[ {{M^1}{L^{ - 1}}{T^{ - 2}}} \right]$
A silver sphere of radius $1\ cm$ and work function $4.7 \ eV$ is suspended from an insulating thread in free-space. It is under continuous illumination of $200 \ nm$ wavelength light. As photoelectrons are emitted, the sphere gets charged and acquires a potential. The maximum number of photoelectrons emitted from the sphere is $A \times 10^2$ (where $1 < A < 10$ ). The value of  $'Z '$ is
If the rate of the reaction,

$[Image]$

is fastest, then $Z$ is

Black Hole is