Exams › JEE Main › Physics › Oscillations
205 questions with worked solutions.
Answer: ((M + m)/M)^(1/2)
The correct option is derived from the conservation of energy principle in simple harmonic motion. When the smaller mass m is added to the block of mass M at the equilibrium position, the total mass increases, which reduces the amplitude of oscillation. The new amplitude A2 is related to the original amplitude A1 by the ratio of the square root of the total mass to the original mass, leading to the expression A1/A2 = (M + m)/M.
Answer: (1/2π)√(A²γP0/(MV0))
For an adiabatic small displacement x, dP = -(gamma*P0/V0)*A*x, so restoring force = -(gamma*P0*A^2/V0)*x. Then omega^2 = gamma*P0*A^2/(M*V0) and f = (1/2pi)*sqrt(A^2*gamma*P0/(M*V0)).
Answer: 1/(m(ω0² - ω²))
For a forced oscillator (neglecting damping), steady-state displacement amplitude is proportional to 1/(m*(w0^2 - w^2)).
Answer: K0 and K0
Taking the given K0 as the (maximum) kinetic energy, the total energy equals K0, and the maximum potential energy also equals the total energy, so both are K0.
Answer: √(5/6) T
From y = t^2, acceleration = d^2y/dt^2 = 2 m/s^2 upward, so effective gravity = g + a = 12 m/s^2. New period T' = T*sqrt(g/g_eff) = T*sqrt(10/12) = sqrt(5/6) T.
Answer: 0.729
Amplitude decays as A = A0*e^(-bt). In each 5 s interval it multiplies by 0.9. After 15 s total (3 intervals): (0.9)^3 = 0.729 of the initial amplitude.
Answer: 5 cm, π/10 s
After collision v = (0.5*3)/1.5 = 1 m/s, combined mass 1.5 kg. omega = sqrt(600/1.5) = 20 rad/s. A = v/omega = 1/20 = 0.05 m = 5 cm; T = 2pi/20 = pi/10 s.
Answer: 1/15 ln3
The damping constant can be determined using the relationship between the initial and final energy of the damped pendulum over a certain number of oscillations. The formula for energy decay in a damped system shows that the energy decreases exponentially, and by applying this to the given energies and oscillations, we find that the damping constant is correctly calculated as 1/15 ln3.
Answer: y = 0.1 sin (4t + π/4)
(1/2)*0.1*w^2*(0.1)^2 = 8*10^-3 -> w^2 = 16 -> w = 4 rad/s. Amplitude is 0.1 m, so y = 0.1 sin(4t + pi/4).
Answer: [(TM/T)² - 1] A / Mg
The correct option relates the change in time period due to the added mass to the material properties of the wire, specifically Young's modulus. The formula shows how the increase in time period affects the elongation of the wire, which is directly linked to its Young's modulus, thus providing a relationship between the mechanical properties and the pendulum's behavior.
Answer: when the amplitude reaches g/ω²
The coin will lose contact with the plate when the upward acceleration of the plate equals the acceleration due to gravity. This occurs when the amplitude of the oscillation reaches g/ω², as this is the point where the maximum upward acceleration of the plate is insufficient to keep the coin pressed against it.
Answer: t = 2t0
Effective gravity in water g' = g(1 - rho_water/rho_bob) = g(1 - 1000/1333.3) = g/4. Since T is proportional to 1/sqrt(g), t/t0 = sqrt(g/g') = sqrt(4) = 2, so t = 2*t0.
Answer: 1/6 s
From mean position x = A sin(wt). KE = 0.75 E means PE = 0.25 E -> x = A/2 -> sin(wt)=1/2 -> wt = pi/6. With T = 2 s (w = pi), t = (pi/6)/pi = 1/6 s.
Answer: 4/1
KE at equilibrium = total energy = (1/2)kA^2. PE at x=A/2 = (1/2)k(A/2)^2 = (1/8)kA^2. Ratio = (1/2)/(1/8) = 4/1.
Answer: 12/25
k ~ 1/T^2, and combining forces adds the constants: 1/T^2 = 1/T1^2 + 1/T2^2 = (5/4)^2 + (5/3)^2 = 25/16 + 25/9. This gives T^2 = 144/625, so T = 12/25 s.
Answer: all of the above
The damping force coefficient b is influenced by the viscosity of the medium, which affects resistance, as well as the dimensions and geometry of the block, which determine how the block interacts with the fluid. Therefore, all these factors collectively influence the value of b.
Answer: mg l (1 - cos θ)
The greatest kinetic energy of the pendulum bob occurs at the lowest point of its swing, where all the potential energy converted from the height is transformed into kinetic energy. The potential energy at the maximum height is given by mg l (1 - cos θ), which equals the kinetic energy at the lowest point.
Answer: None of these
The correct option is 'None of these' because the oscillation period of the charged sphere in an electric field is influenced by both gravitational and electric forces, leading to a more complex relationship than those presented in the other options.
Answer: (π/4)√(LC)
Charge q = q0*cos(wt) with w = 1/sqrt(LC); capacitor (electric) energy is proportional to q^2. Equal sharing needs q^2 = q0^2/2, i.e. cos^2(wt) = 1/2, so wt = pi/4 and t = (pi/4)*sqrt(LC).
Answer: Q/√2
Total energy = Q^2/(2C). Equal sharing means capacitor energy = Q^2/(4C) = q^2/(2C), giving q^2 = Q^2/2, so q = Q/sqrt(2).
Answer: x = 0.1 sin(6t + π/4)
KE at mean = (1/2)m*omega^2*A^2 = 18e-3 gives (1/2)(0.1)(0.01)omega^2 = 0.018, so omega^2 = 36, omega = 6 rad/s. With initial phase 45 deg, x = 0.1 sin(6t + pi/4).
Answer: 5k/2
The spring constant of a segment is inversely proportional to its length. Since segment A is shorter than segment B, it will have a higher spring constant. Given the ratio of lengths, the spring constant for segment A can be calculated as 5k/2.
Answer: 25°C; α = 1.85 × 10^−5/°C
The pendulum clock's timekeeping is affected by temperature changes, with the clock being slow at higher temperatures and fast at lower temperatures. The correct option indicates that at 25°C, the effects of thermal expansion balance out, allowing the clock to keep accurate time, and the linear expansion coefficient reflects the material's response to temperature changes.
Answer: T² = t1² + t2²
For springs in series 1/k = 1/k1 + 1/k2. Since T^2 is proportional to 1/k, T^2 = t1^2 + t2^2.
Q25. The total energy of a particle, executing simple harmonic motion is
Answer: independent of x
In simple harmonic motion, the total energy is the sum of kinetic and potential energy, both of which vary with position. However, when combined, these energies result in a constant total energy that does not depend on the displacement from the equilibrium position.
Answer: 1 / [m(ω² - ω0²)]
The steady-state amplitude of a driven oscillator is F0/[m(omega0^2 - omega^2)], so the displacement is proportional to 1/[m(omega^2 - omega0^2)] (the sign is just a phase). The stored choice puts m in the numerator, which is wrong; mass must appear in the denominator.
Answer: ω1 < ω2
In forced oscillation, the amplitude is maximized at the resonance frequency, which is lower than the frequency at which energy is maximized due to damping effects. When damping is small, the system can respond more effectively at a lower frequency, leading to the condition where ω1 is less than ω2.
Answer: -π/6
Velocity phase of 1 = pi/3 + pi/2; velocity phase of 2 (from y2=cos = sin(+pi/2)) = pi/2 + pi/2. Difference = (5pi/6) - (pi) = -pi/6.
Q29. The function sin²(ωt) represents
Answer: a periodic, but not simple harmonic motion with a period π/ω
Writing sin^2(wt) = (1 - cos 2wt)/2 shows it is periodic with period pi/w, but it is not a simple harmonic motion (its mean position is offset and it is not of the pure form A sin/cos about the origin). Hence it is periodic, not SHM, with period pi/w.
Answer: first increase and then decrease to the original value
As water drains, the centre of mass of the water (and hence the effective pendulum length) first lowers then rises back to the centre, so the period first increases and then decreases to its original value.
Q31. If a simple harmonic motion is represented by d²x/dt² + αx = 0, its time period is
Answer: 2π/√α
Comparing d^2x/dt^2 + alpha x = 0 with d^2x/dt^2 + omega^2 x = 0 gives omega = sqrt(alpha). Time period T = 2pi/omega = 2pi/sqrt(alpha).
Answer: 0.01 s
The maximum velocity in simple harmonic motion is given by the formula v_max = Aω, where A is the amplitude and ω is the angular frequency. Given the amplitude and maximum velocity, we can find the angular frequency and then use it to calculate the period, which is the inverse of the frequency.
Answer: 1/6 s
KE is 75% of total when PE is 25%, i.e. x = A/2. Starting from the mean position x = A sin(wt), so sin(wt)=1/2, wt = pi/6. With w = 2*pi/T = pi, t = (pi/6)/pi = 1/6 s.
Answer: A = x0ω², δ = 3π/4
The acceleration of the particle can be derived from the displacement function by taking the second derivative with respect to time. This results in an expression that shows the amplitude as A = x0ω² and a phase shift of δ = 3π/4, indicating that the acceleration is out of phase with the displacement.
Answer: π/3
The phase difference of π/3 indicates that when one particle is at its maximum displacement, the other is at a position that allows them to be separated by the maximum distance of X0 + A. This relationship arises from the properties of simple harmonic motion and the geometry of their oscillations.
Answer: ((M + m)/M)^(1/2)
The correct option reflects the conservation of energy and the relationship between the amplitudes before and after the mass m is added. When the small mass m is placed on the block, the total mass increases, which reduces the amplitude of the system due to the increased inertia, leading to the derived ratio of amplitudes as ((M + m)/M)^(1/2).
Answer: 2/b
The average life of the pendulum is determined by the damping effect, which reduces the amplitude over time. The factor of 2 in the expression 2/b arises from the relationship between the damping force and the exponential decay of amplitude, leading to the time it takes for the amplitude to decrease to 1/e of its initial value.
Answer: 0.729
The amplitude of a damped oscillator decreases exponentially over time. Given that it decreases to 0.9 of its original value in 5 seconds, we can use the exponential decay formula to find the amplitude after an additional 10 seconds, resulting in a decrease to approximately 0.729 of its original magnitude.
Answer: 1/(2π) √(A²γP0/(MV0))
Displacing the piston by x changes gas pressure; for adiabatic isolation the restoring force is F = -(gamma*P0*A^2/V0)*x. So omega = sqrt(gamma*P0*A^2/(M*V0)) and f = (1/2pi) sqrt(A^2*gamma*P0/(M*V0)).
Answer: time period of oscillations is 6τ
The particle's motion is characterized by its displacement over time, and the distances traveled in successive intervals suggest a specific relationship between time and distance in simple harmonic motion. Given that the distances traveled are in a ratio of 1:2, this indicates that the total distance covered in the first two intervals corresponds to a complete cycle, leading to the conclusion that the time period of oscillations is 6τ.
Answer: [(TM/T)² - 1] A/(Mg)
Adding mass M stretches the wire by dL = MgL/(AY), so T_M^2/T^2 = (L+dL)/L = 1 + Mg/(AY). Hence Mg/(AY) = (T_M/T)^2 - 1, giving 1/Y = [(T_M/T)^2 - 1]*A/(Mg).
Answer: 7A/3
At x = 2A/3, v^2 = w^2(A^2 - 4A^2/9) = 5w^2A^2/9. Tripling speed gives v'^2 = 9*v^2 = 5w^2A^2. New amplitude: 5w^2A^2 = w^2(A'^2 - 4A^2/9) -> A'^2 = 49A^2/9 -> A' = 7A/3.
Answer: 7.1 N/m
Mass of one Ag atom = 108/(6.02e23) g = 1.79e-25 kg. Force constant k = m*omega^2 = m*(2*pi*f)^2 = 1.79e-25*(2*pi*1e12)^2 = 7.1 N/m.
Answer: 178.2 Hz
The fundamental frequency of a vibrating wire can be calculated using the formula that incorporates the tension, length, density, and elasticity of the material. Given the parameters for the steel wire and the specified elastic strain, the calculations yield a fundamental frequency of 178.2 Hz, confirming option B as the correct answer.
Answer: Q/√2
At the point where the energy is equally distributed between the electric field of the capacitor and the magnetic field of the inductor, the charge on the capacitor is at a value of Q/√2. This is derived from the relationship between energy stored in the capacitor and inductor, where the total energy remains constant.
Answer: (π/4)√LC
Capacitor energy ~ q^2 = q0^2*cos^2(wt) with w=1/sqrt(LC). Equal sharing of energy needs cos^2(wt)=1/2, i.e. wt=pi/4, so t = (pi/4)*sqrt(LC).
Answer: L corresponds to m, C corresponds to k, and R corresponds to b
The damped LCR-oscillator analogy is L corresponds to mass m, R corresponds to damping b, and inverse capacitance 1/C corresponds to spring constant k. Among the choices the one pairing L with m and R with b is correct.
Answer: (3) time period of oscillations is 6τ
The particle's distances traveled in successive time intervals indicate a quadratic relationship, characteristic of simple harmonic motion. The total distance covered suggests that the time period is 6τ, as the distances align with the expected behavior of a harmonic oscillator.
Answer: [(Tm/T)² - 1] A/(Mg)
The correct option is derived from the relationship between the time period of a pendulum and the properties of the material, where the change in time period due to the added mass can be expressed in terms of Young's modulus, cross-sectional area, and gravitational force. This option accurately reflects how the increase in mass affects the time period, leading to the derived formula.
Answer: 7A/3
When the speed of the particle is increased while it is at a distance of 2A/3 from the equilibrium, the total mechanical energy of the system increases. Since the total energy in simple harmonic motion is proportional to the square of the amplitude, the new amplitude can be calculated using the relationship between the initial and final speeds and positions, leading to the result of 7A/3.