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Displacement Function in Simple Harmonic Motion

The displacement function in simple harmonic motion is given by the equation D(t) = Acos(wt), where A represents the amplitude of the oscillation and w represents the angular frequency of the motion. This equation describes the position of an object undergoing simple harmonic motion at any given time, t.

Understanding Simple Harmonic Motion

Simple harmonic motion (SHM) is a type of periodic motion that occurs when a restoring force is proportional to the displacement from an equilibrium position. It is characterized by a repetitive back-and-forth motion around a stable equilibrium point. Examples of systems exhibiting SHM include a mass-spring system and a pendulum.

Displacement-Time Graph in Simple Harmonic Motion

The displacement-time graph in simple harmonic motion represents the variation in position of the object as a function of time. It provides insights into the amplitude, frequency, and phase of the oscillation.

Deriving the Displacement Function

The displacement function, D(t) = Acos(wt), can be derived using the principles of SHM. Here's a step-by-step explanation:

1. Start with the general equation for SHM: F = -kx, where F is the restoring force, k is the spring constant, and x is the displacement from equilibrium.
2. Apply Newton's second law of motion, F = ma, where m is the mass of the object and a is the acceleration.
3. Since acceleration is the second derivative of displacement with respect to time (a = d²x/dt²), we can rewrite the equation as m(d²x/dt²) = -kx.
4. Divide both sides of the equation by m to obtain (d²x/dt²) = -(k/m)x.
5. Notice that the left side of the equation represents the second derivative of x with respect to time, which can be written as d²x/dt² = w²x, where w is the angular frequency.
6. Substitute this expression into the equation to get w²x = -(k/m)x.
7. Simplify the equation by canceling out x on both sides: w² = -(k/m).
8. Solve for w to obtain w = sqrt(k/m).
9. The general solution to the differential equation is x = Acos(wt) + Bsin(wt), where A and B are constants.
10. Since the cosine function represents the amplitude and phase of the oscillation, we can rewrite the equation as D(t) = Acos(wt), where D(t) represents the displacement as a function of time.

Conclusion

The displacement function in simple harmonic motion is given by D(t) = Acos(wt), where A represents the amplitude of the oscillation and w represents the angular frequency. This equation describes the position of an object undergoing simple harmonic motion at any given time. It is derived from the principles of SHM, involving the relationship between the restoring force, displacement, and acceleration. The displacement-time graph provides valuable information about the characteristics of the oscillation, such as amplitude, frequency, and phase.
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Attempt All sub parts from each question.Damping: When an analog instrument is used to measure a physical parameter, a deflecting torque is applied to the moving system which is deflected from its initial position and should move steadily to the deflected position. But due to inertia, the moving system keeps on oscillating about equilibrium. To remove the oscillation of the moving system a damping torque is required. The damping torque should be of such that the pointer quickly comes to its final steady position, without overshooting. If the instrument is underdamped, the moving system will oscillate about the final steady position with a decreasing amplitude and will take some time before it comes to rest. When the moving system moves rapidly but smoothly to its final steady position, the instrument is said to be critically damped or deadbeat. If the damping torque is more than what is required for critical damping, the instrument is said to be overdamped. In an overdamped instrument, the moving system moves slowly to its final steady position in a lethargic fashion.Methods of producing damping torque:(i) Air friction damping(ii) Fluid friction damping(iii) Eddy current dampingAir Friction Damping: A light piston is attached to the moving system. This piston moves in an air chamber closed at one end. When there is an oscillation, the piston moves in and out of the chamber. When the piston moves into the chamber, the air inside is compressed and an air pressure is built up which opposes the motion of the piston and thus the moving system faces a damping torque which ultimately reduces the oscillation. Fluid Friction Damping: In this type of damping oil is used in place of air. Viscosity of the oil being greater, the damping torque is also more. A disc is attached to the moving system which is completely dipped into the oil. When the moving system oscillates, the disc moves in oil and a frictional drag is produced. This frictional drag opposes the oscillation. Eddy Current Damping: The moving system is connected to an aluminium disc which rotates in a magnetic field. Rotation in magnetic field induces an emf in it and if the path is closed, a current (known as eddy current) flows. This current interacts with the magnetic field to produce an electromagnetic torque which opposes the motion. This torque is proportional to the oscillation of the moving system. This electromagnetic torque ultimately reduces the oscillation. Air friction damping provides a very simple and cheap method of damping. The disadvantages of fluid friction damping are that it can be used only for instruments which are in vertical position. Eddy current damping is the most efficient form of damping.Q. In Fluid Friction Damping the amount of damping torque

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