Sign in
12thPass logo
New chatPYQ LibraryDoubtsRank report
Sign in to see Recents

Your guest activity stays on this device

Sign in to save progress →
Sign in

Simple Harmonic Motion question

2010 · Shift 1 · Q57
Guest · filters and generic practice availableBrowsing as a guest · PYQ filters and generic practice are available. Sign in only for personalised features and saved progress.
  1. PYQ Library
  2. /JEE Advanced
  3. /Physics
  4. /Simple Harmonic Motion
  5. /2010 · Shift 1 · Q57

Simple Harmonic Motion question

2010 · Shift 1 · Q57

JEE AdvancedPhysicsSimple Harmonic MotionNumerical+3 / −1
A 0.1 kg mass is suspended from a wire of negligible mass. The length of the wire is 1 m and its crosssectional area is 4.9 ×\times× 10-7 m2. If the mass is pulled a little in the vertically downward direction and released, it performs simple harmonic motion of angular frequency 140 rad s−1. If the Young’s modulus of the material of the wire is n ×\times× 109 Nm-2, the value of n is
Numerical answer
View written solutionFree

Correct answer: 4

Step-by-step Derivation

  1. Understanding the System and SHM: When the mass m is pulled down by a small distance x from its equilibrium position and released, it oscillates. The restoring force is provided by the tension in the wire. This setup results in Simple Harmonic Motion (SHM). The angular frequency ω of this SHM is given by the formula: ω=kmω = \sqrt{\frac{k}{m}}ω=mk​​ where k is the effective spring constant of the system (in this case, the wire).

  2. Relating Angular Frequency and Spring Constant: From the SHM formula, we can express the spring constant k in terms of mass m and angular frequency ω: ω2=km  ⟹  k=mω2ω^2 = \frac{k}{m} \implies k = mω^2ω2=mk​⟹k=mω2

  3. Relating Spring Constant and Young's Modulus: The wire acts like a spring. The Young's modulus Y of the material of the wire is defined as the ratio of stress to strain: Y=StressStrain=F/AΔL/LY = \frac{\text{Stress}}{\text{Strain}} = \frac{F/A}{\Delta L/L}Y=StrainStress​=ΔL/LF/A​ where F is the force applied, A is the cross-sectional area, L is the original length, and ΔL is the extension.

    Rearranging this formula to find the force F required to produce an extension ΔL: F=(YAL)ΔLF = \left(\frac{YA}{L}\right) \Delta LF=(LYA​)ΔL This is in the form of Hooke's Law, F = kx, where the displacement x is the extension ΔL. By comparing these two equations, we can identify the effective spring constant k of the wire: k=YALk = \frac{YA}{L}k=LYA​

  4. Solving for Young's Modulus (Y): We now have two expressions for the spring constant k. By equating them, we can solve for Y: mω2=YALmω^2 = \frac{YA}{L}mω2=LYA​ Y=mω2LAY = \frac{mω^2L}{A}Y=Amω2L​

  5. Substituting the Given Values: We are given:

    • Mass, m = 0.1 kg
    • Length, L = 1 m
    • Cross-sectional area, A=4.9×10−7A = 4.9 × 10^{-7}A=4.9×10−7 m²
    • Angular frequency, ω = 140 rad s⁻¹

    Now, substitute these values into the equation for Y: Y=(0.1 kg)×(140 rad s−1)2×(1 m)4.9×10−7 m2Y = \frac{(0.1 \text{ kg}) \times (140 \text{ rad s}^{-1})^2 \times (1 \text{ m})}{4.9 \times 10^{-7} \text{ m}^2}Y=4.9×10−7 m2(0.1 kg)×(140 rad s−1)2×(1 m)​ Y=0.1×196004.9×10−7 Nm−2Y = \frac{0.1 \times 19600}{4.9 \times 10^{-7}} \text{ Nm}^{-2}Y=4.9×10−70.1×19600​ Nm−2 Y=19604.9×10−7 Nm−2Y = \frac{1960}{4.9 \times 10^{-7}} \text{ Nm}^{-2}Y=4.9×10−71960​ Nm−2 Y=1960049×107 Nm−2Y = \frac{19600}{49} \times 10^7 \text{ Nm}^{-2}Y=4919600​×107 Nm−2

  6. Final Calculation: Since 196=4×49196 = 4 \times 49196=4×49, we have 19600 / 49 = 400. Y=400×107 Nm−2Y = 400 \times 10^7 \text{ Nm}^{-2}Y=400×107 Nm−2 Y=4×102×107 Nm−2Y = 4 \times 10^2 \times 10^7 \text{ Nm}^{-2}Y=4×102×107 Nm−2 Y=4×109 Nm−2Y = 4 \times 10^9 \text{ Nm}^{-2}Y=4×109 Nm−2

  7. Determining the Value of n: The problem states that the Young's modulus is n×109Nm−2n × 10^9 Nm⁻²n×109Nm−2. Comparing this with our calculated value: n×109=4×109n \times 10^9 = 4 \times 10^9n×109=4×109 Therefore, the value of n is 4.

PreviousNext

More from Simple Harmonic Motion

  • When a particle of mass m moves on the x-axis in a potential of the form V(x) = kx2, it performs simple harmonic motion. The corresponding time period is proportional to km​​, as can be seen easily using dimensional… Includes diagram2010 · MCQ
  • When a particle of mass m moves on the x-axis in a potential of the form V(x) = kx2, it performs simple harmonic motion. The corresponding time period is proportional to km​​, as can be seen easily using dimensional… Includes diagram2010 · MCQ
  • When a particle of mass m moves on the x-axis in a potential of the form V(x) = kx2, it performs simple harmonic motion. The corresponding time period is proportional to km​​, as can be seen easily using dimensional… Includes diagram2010 · MCQ
  • The x-t graph of a particle undergoing simple harmonic motion is shown in the figure. The acceleration of the particle at t=4/3 s is Includes diagram2009 · MCQ
  • The mass M shown in the figure below oscillates in simple harmonic motion with amplitude A. The amplitude of the point P is Includes diagram2009 · MCQ
  • A uniform rod of length L and mass M is pivoted at the centre. Its two ends are attached to two springs of equal spring constants k. The springs are fixed to rigid supports as shown in the figure, and the rod is free to oscillate in the… Includes diagram2009 · MCQ
  • A student performed the experiment to measure the speed of sound in air using resonance air-column method. Two resonances in the air-column were obtained by lowering the water level. The resonance with the shorter air-column is the first…2009 · Multiple correct
  • Column I gives a list of possible set of parameters measured in some experiments. The variations of the parameters in the form of graphs are shown in Column II. Match the set of parameters given in Column I with the graphs given in Column… Includes table Includes diagram2008 · MCQ