How does the mass on a horizontal spring behave?

In summary, "mass on a horz. spring" refers to a physical system consisting of a mass attached to a horizontal spring which oscillates due to the spring's force. The motion is described by simple harmonic motion and is affected by the mass, spring constant, and amplitude. The energy of the system changes between potential and kinetic as it oscillates, and it is commonly used in mechanical and scientific applications.
  • #1
mattmannmf
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A 53 gram mass is attached to a massless spring and allowed to oscillate around an equilibrium according to:
y(t) = 1.2*sin( 3.1415*t ) where y is measured in meters and t in seconds

(a) What is the spring constant in N/m ?

(b) What is the total Mechanical Energy in the mass/spring system?

(c) What is the maximum Kinetic Energy of the mass?

(d) What is the maximum velocity of the mass in m/s ?
 
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What are your thoughts on how to approach it?
 
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(a) The spring constant can be calculated using the equation k = mω^2, where m is the mass in kg and ω is the angular frequency in radians per second. In this case, the mass is 53 grams, or 0.053 kg, and the angular frequency is 3.1415 radians per second. Plugging these values into the equation, we get k = (0.053 kg)(3.1415 rad/s)^2 = 0.53 N/m.

(b) The total mechanical energy in the system can be calculated using the equation E = (1/2)kA^2, where k is the spring constant and A is the amplitude of oscillation. In this case, the amplitude can be found by taking the absolute value of the coefficient in front of the sine function, which is 1.2 meters. Plugging in the values, we get E = (1/2)(0.53 N/m)(1.2 m)^2 = 0.38 J.

(c) The maximum kinetic energy of the mass occurs at the equilibrium point, where all of the potential energy is converted into kinetic energy. The maximum kinetic energy can be calculated using the equation KE = (1/2)mv^2, where m is the mass in kg and v is the velocity in meters per second. In this case, the mass is 0.053 kg and the velocity can be found by taking the derivative of the position equation with respect to time. This gives us v = 1.2*3.1415*cos(3.1415*t) = 3.7695*cos(3.1415*t) m/s. At the equilibrium point, t = 0, so the maximum velocity is 3.7695 m/s. Plugging this into the equation, we get KE = (1/2)(0.053 kg)(3.7695 m/s)^2 = 0.38 J.

(d) The maximum velocity can be found using the same equation as in part (c). At the maximum displacement, the velocity is 0, so we can set the position equation equal to 0 and solve for t. This gives us t = 0.3183 seconds. Plugging this value into the velocity equation, we get v = 3.7695*cos(3.1415*0.3183) = 3.7695 m
 

Related to How does the mass on a horizontal spring behave?

1. What is the definition of "mass on a horz. spring"?

The term "mass on a horz. spring" refers to a physical system consisting of a mass attached to a horizontal spring, which is able to oscillate back and forth due to the force of the spring.

2. How is the motion of a mass on a horz. spring described?

The motion of a mass on a horz. spring is described by simple harmonic motion, which is a type of periodic motion where the restoring force is directly proportional to the displacement of the mass from its equilibrium position.

3. What factors affect the period of a mass on a horz. spring?

The period of a mass on a horz. spring is affected by the mass of the object, the spring constant of the spring, and the amplitude of the motion. The period is inversely proportional to the square root of the spring constant and directly proportional to the square root of the mass and the amplitude.

4. How does the energy of a mass on a horz. spring change during its motion?

The energy of a mass on a horz. spring changes between potential energy and kinetic energy as it oscillates. At the equilibrium position, the energy is entirely potential, and at the maximum displacement, the energy is entirely kinetic. The total energy remains constant throughout the motion.

5. What real-world applications involve a mass on a horz. spring?

Masses on horz. springs are commonly used in mechanical systems such as shock absorbers, car suspensions, and watches. They are also used in scientific instruments, such as seismographs, to measure vibrations and earthquakes.

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