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P the Maximum Speed and Acceleration of a Particle Executing Simple Harmonic Motion Are 10 Cm S−1 and 50 Cm S−2. Find the Position(S) of the Particle When the Speed is 8 Cm S−1. - Physics

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प्रश्न

The maximum speed and acceleration of a particle executing simple harmonic motion are 10 cm/s and 50 cm/s2. Find the position(s) of the particle when the speed is 8 cm/s.

योग
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उत्तर

It is given that:
Maximum speed of the particle, \[v_{Max}\]= `10 "cm"^(- 1)`

Maximum acceleration of the particle,

\[a_{Max}\]= 50 cms−2
The maximum velocity of a particle executing simple harmonic motion is given by,
\[v_{Max} = A\omega\]
where \[\text { omega is angular frequency, and }\]
is amplitude of the particle.
Substituting the value of \[v_{Max}\]in the above expression,
we get :
 = 10     \[. . . (1)\]
\[\Rightarrow \omega^2 = \frac{100}{A^2}\] 
 
aMax = ω2A = 50 cms−1

\[\Rightarrow \omega^2 = \frac{50}{A} . . . (2)\]

\[\text { From the equations (1) and (2), we get:} \]

\[\frac{100}{A^2} = \frac{50}{A}\]

\[ \Rightarrow A = 2 cm\]

\[ \therefore \omega = \sqrt{\frac{100}{A^2}} = 5 \sec^{- 1}\]

To determine the positions where the speed of the particle is 8 ms-1, we may use the following formula:
      v2 = ω2 (A2 − y2)

where y is distance of particle from the mean position, and
                 v is velocity of the particle.

On substituting the given values in the above equation, we get:
      64 = 25 (4 − y2)

\[\Rightarrow \frac{64}{25} = 4 - y^2\]

⇒ 4 − y2 = 2.56
⇒       y2 = 1.44
⇒​       y  = \[\sqrt{1 . 44}\]

⇒        y = ± 1.2 cm   (from the mean position)

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Energy in Simple Harmonic Motion
  क्या इस प्रश्न या उत्तर में कोई त्रुटि है?
अध्याय 12: Simple Harmonics Motion - Exercise [पृष्ठ २५२]

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एचसी वर्मा Concepts of Physics Vol. 1 [English] Class 11 and 12
अध्याय 12 Simple Harmonics Motion
Exercise | Q 4 | पृष्ठ २५२

संबंधित प्रश्न

A particle is in linear simple harmonic motion between two points, A and B, 10 cm apart. Take the direction from A to B as the positive direction and give the signs of velocity, acceleration and force on the particle when it is

(a) at the end A,

(b) at the end B,

(c) at the mid-point of AB going towards A,

(d) at 2 cm away from B going towards A,

(e) at 3 cm away from A going towards B, and

(f) at 4 cm away from B going towards A.


A particle executes simple harmonic motion with an amplitude of 10 cm. At what distance from the mean position are the kinetic and potential energies equal?


The block of mass m1 shown in figure is fastened to the spring and the block of mass m2 is placed against it. (a) Find the compression of the spring in the equilibrium position. (b) The blocks are pushed a further distance (2/k) (m1 + m2)g sin θ against the spring and released. Find the position where the two blocks separate. (c) What is the common speed of blocks at the time of separation?


In following figure k = 100 N/m M = 1 kg and F = 10 N. 

  1. Find the compression of the spring in the equilibrium position. 
  2. A sharp blow by some external agent imparts a speed of 2 m/s to the block towards left. Find the sum of the potential energy of the spring and the kinetic energy of the block at this instant. 
  3. Find the time period of the resulting simple harmonic motion. 
  4. Find the amplitude. 
  5. Write the potential energy of the spring when the block is at the left extreme. 
  6. Write the potential energy of the spring when the block is at the right extreme.
    The answer of b, e and f are different. Explain why this does not violate the principle of conservation of energy.


The springs shown in the figure are all unstretched in the beginning when a man starts pulling the block. The man exerts a constant force F on the block. Find the amplitude and the frequency of the motion of the block.


Find the elastic potential energy stored in each spring shown in figure, when the block is in equilibrium. Also find the time period of vertical oscillation of the block.


Solve the previous problem if the pulley has a moment of inertia I about its axis and the string does not slip over it.


Consider the situation shown in figure . Show that if the blocks are displaced slightly in opposite direction and released, they will execute simple harmonic motion. Calculate the time period.


A 1 kg block is executing simple harmonic motion of amplitude 0.1 m on a smooth horizontal surface under the restoring force of a spring of spring constant 100 N/m. A block of mass 3 kg is gently placed on it at the instant it passes through the mean position. Assuming that the two blocks move together, find the frequency and the amplitude of the motion.


Discuss in detail the energy in simple harmonic motion.


When a particle executing S.H.M oscillates with a frequency v, then the kinetic energy of the particle? 


When the displacement of a particle executing simple harmonic motion is half its amplitude, the ratio of its kinetic energy to potential energy is ______.


A body is executing simple harmonic motion with frequency ‘n’, the frequency of its potential energy is ______.


A body is performing S.H.M. Then its ______.

  1. average total energy per cycle is equal to its maximum kinetic energy.
  2. average kinetic energy per cycle is equal to half of its maximum kinetic energy.
  3. mean velocity over a complete cycle is equal to `2/π` times of its π maximum velocity. 
  4. root mean square velocity is times of its maximum velocity `1/sqrt(2)`.

Find the displacement of a simple harmonic oscillator at which its P.E. is half of the maximum energy of the oscillator.


A mass of 2 kg is attached to the spring of spring constant 50 Nm–1. The block is pulled to a distance of 5 cm from its equilibrium position at x = 0 on a horizontal frictionless surface from rest at t = 0. Write the expression for its displacement at anytime t.


A particle undergoing simple harmonic motion has time dependent displacement given by x(t) = A sin`(pit)/90`. The ratio of kinetic to the potential energy of this particle at t = 210s will be ______.


The total energy of a particle, executing simple harmonic motion is ______.

where x is the displacement from the mean position, hence total energy is independent of x.


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