/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Q18E 18 A 1.50m string of weight 0.01... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

18 A 1.50m string of weight 0.0125N is tied to the ceiling at its upper end, and the lower end supports a weight W. Ignore the very small variation in tension along the length of the string that is produced by the weight of the string. When you pluck the string slightly, the waves traveling up the string obey the equation

y (x, t) = (8.50 mm) cos (172 rad/mx 4830 rad/s t)

Assume that the tension of the string is constant and equal to W. (a) How much time does it take a pulse to travel the full length of the string? (b) What is the weight W? (c) How many wavelengths are on the string at any instant of time? (d) What is the equation for waves traveling down the string?

Short Answer

Expert verified

Therefore, the time taken for a pulse to travel the full length of the string is 0.053s, the weight (W) is 0.671N, the number of wavelengths on the string at any instant of time is 41.1 and the equation of motion for waves travelling down the string is y(x,t)=(8.50mm)cos(172m-1x+4830s-1t).

Step by step solution

01

Determination of the formula in Mechanical Waves

The wave function y (x, t) of a sinusoidal wave which describes the displacement of individual particles in the medium is:

y(x,t)=Acos(kx∓Ӭt)--(1)

Where A, k andÓ¬are constants.

The minus sign is used when the wave is traveling in positive X-direction and the plus sign is used when the wave is traveling in the negative X-direction.


The relation between the wave number k and the wavelengthλ:

λ=2πk--(2)

The relation between the wave speed v and the wave angular speedÓ¬is :

v=Ó¬k--(3)

And the wave speed in a string in terms of the tension T and the linear mass densityμ:

V=Tμ--(4)


The length of the string is l = 1.50m, its weight is Tg = 0.0125N, the tension in the string is T = W and the wave function of the wave traveling in the string is:

y(x,t)=(8.50mm)cos(172m-1x-4830s-1t)

02

Application of the formula of Mechanical Waves

Compare the wave function of the string with the wave function in equation (1),
The wave amplitude is:

A=8.50×10-3m

The wave number is:

k=172m-1

The angular speed is:

Ó¬=4830s-1


Put in the values forÓ¬ and k into equation (3):

v=4830s-1172m-1=28.1mls


The mass of the string is:

m=Fgg=0.0125N9.8m/s2=1.28×10−3kg

The linear mass density is the mass length, so the linear of the string is:

μ=ml=1.28×10−3kg1.50m=8.50×10−4kg/m

03

Calculation of the time (t), weight (W), n (number of wavelengths)

The speed of any motion in terms of the distance travelled x and the time interval t is:

v=xtt=xv



Substitute v and x = l, therefore the time it takes for the wave to travel the full length of the string:

role="math" localid="1668150737173" t=1.50m28.1mls=0.053st=0.053s



Put in the values for v, T andμinto equation (4) and solve for W:

28.08m/s=W8.50×10−4kg/mW=(28.08)2×8.50×10−4=0.671N

W=0.671N


Put in the value for k into equation (2), so we get the wavelength W:

λ=2π172m-1=0.037m

The number of wavelengths on the string at any instant of time can be calculated from the following relations:

n=ThelengthofthestringThewavelength=lλ

Now, put in the values for λand l:

n=1.500.037m=411

n = 41.1wavelengths

04

Determination of the equation of waves travelling down the string

The minus sign in the cosine function for the upward direction means that the positive direction is upward.

If the wave is traveling downward (the negative direction), then same wave equation is used but with plus sign inside the cosine function:

y(x,t)=(8.50mm)cos(172m-1x+4830s-1t)


Therefore, the time taken for a pulse to travel the full length of the string is 0.053s, the weight (W) is 0.671N, the number of wavelengths on the string at any instant of time is 41.1 and the equation of motion for waves travelling down the string is y(x,t)=(8.50mm)cos(172m-1x+4830s-1t).

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with 91Ó°ÊÓ!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

A transverse wave on a string has amplitude 0.300 cm, wavelength 12.0 cm, and speed 6.00 cm/s. It is represented by y(x,t) as given in Exercise 15.12.

(a) At time t = 0, compute y at 1.5-cm intervals of x(that is, at x = 0, x = 1.5 cm, x = 3.0 cm, and so on) from x= 0 to x = 12.0 cm. Graph the results. This is the shape of the string at time t = 0.

(b) Repeat the calculations for the same values of x at times t = 0.400 s andt = 0.800 s. Graph the shape of the string at these instants. In what direction is the wave traveling?

A piano wire with mass 3.00 g and length 80.0 cm is stretched with a tension of 25.0 N. A wave with frequency 120.0 Hz and amplitude 1.6 mm travels along the wire. (a) Calculate the average power carried by the wave. (b) What happens to the average power if the wave amplitude is halved?

Two waves travel on the same string. Is it possible for them to have (a) different frequencies; (b) different wavelengths; (c) different speeds; (d) different amplitudes; (e) the same frequency but different wavelengths? Explain your reasoning.

Longitudinal Waves on a Spring. A long spring such as a SlinkyTMis often used to demonstrate longitudinal waves. (a) Show that if a spring that obeys Hooke’s law has mass m, length L, and force constant k′, the speed of longitudinal waves on the spring is v=Lk'm

(see Section 16.2). (b) Evaluate v for a spring with m = 0.250 kg, L = 2.00 m, and k′ = 1.50 N/m.

15.4. BIO Ultrasound Imaging. Sound having frequencies above the range of human hearing (about 20,000 Hz) is called ultrasound. Waves above this frequency can be used to penetrate the body and to produce images by reflecting from surfaces. In a typical ultrasound scan, the waves travel through body tissue with a speed of 1500 m/s . For a good, detailed image, the wavelength should be no more than 1.0 mm. What frequency sound is required for a good scan?

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.