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In Fig. 16-43, an aluminum wire, of length Ll=60.0cm, cross1.00×10-2cm2-sectional area, and density2.60g/cm3, is joined to a steel wire, of densityrole="math" localid="1661166375385" 7.80g/cm3and the same cross-sectional area. The compound wire, loaded with a block of massm=10.0kg, is arranged so that the distanceL2from the joint to the supporting pulley is 86.6 cm. Transverse waves are set up on the wire by an external source of variable frequency; a node is located at the pulley. (a) Find the lowest frequency that generates a standing wave having the joint as one of the nodes. (b) How many nodes are observed at this frequency?

Short Answer

Expert verified

a) Lowest frequency that generates a standing wave having the joint as one of the nodes is 324 Hz

b) Eight nodes are observed in this frequency

Step by step solution

01

Given data

The length of aluminum wire,L1=60.0cmor0.6m

The length of steel wire,L2=86.6cmor0.866m

Cross-sectional area of both wires,A1=A2=1.00×10-2cm2or1.00×10-6m2

Density of aluminum wire,ÒÏ1=2.60gcm3or2.6×103kgm3

Density of steel wire,ÒÏ2=7.80gcm3or7.8×103kgm3

Mass of the block,m=10.0kg

02

Understanding the concept of free body diagram

From the free body diagram of the block, we can find the tension in the string. We are given enough information to calculate the mass densities of each wire. Using mass density and tension, we can find the velocity of the wave generated on these strings. Now as the same wave is generated on both the strings, using the above parameters, we can find the wavelength. Once we get the wavelength, we can find the frequency and nodes generated.

Formula:

The linear density of the string,μ=mL..........1

The mass of a body in terms of density,m=ÒÏ×Volume.............2

The volume of a body,Area×Length..............3

The velocity of a body,v=Tμ.............4

The velocity of a wave, v=λ×f............5

03

Step 3(a): Calculation of the lowest frequency that generates the standing wave

Free body diagram of the block,

So we can say that the tension of a body is:

T=mg=10×9.8=98N

So, from equation (1), we get that

μ1=m1L1andμ2=m2L2

Using equations (2) and (3), we get the masses of the wires as given:

m1=ÒÏ1×A1×L1m2=ÒÏ2×A2×L2

Substituting the values of masses in equation (1), we get the linear density of both the wires as given:

μ1=ÒÏ1×A1×L1L1=ÒÏ1×A1=2.6×103×1×10-6=2.6×10-3kg/mμ2=ÒÏ2×A2×L2L2=ÒÏ2×A2=7.8×103×1×10-6=7.8×10-3kg/m

Substituting values of tension and mass of aluminum wire in equation (4), we get the velocity as:

v1=982.6×10-3=194.195m/s

Substituting values of tension and mass of steel wire in equation (4), we get the velocity as:

v2=987.8×10-3=112.089m/s

Again, by using equation (5), we get the ratios of velocity as given:

v2v1=λ2×fλ1×f(since.thefrequencyofoscillationissame)λ2λ1=112.089194.195=0.577

Length of the wires representing the position of nth node of the standing wave can be given as:

localid="1661167705861" L1=n1λ12...........6L2=n2λ22...........7

Hence, the ration of the lengths of the wires can be given using equations (6) and (7) as:

L2L1=n2λ22n1λ12L2L1=n2n1×λ2λ10.8660.6=n2n1×0.577n2n1=52

From this we can say that,

The lowest values of nodes n1=2andn2=5.

Hence, from equation (6), the wavelength of aluminum wire can be given as:

λ1=2L1n1=2×0.62=0.6m

Hence, the value of frequency of aluminum wire is given as:

f=v1λ1=194.1950.6=323.6Hz≈324Hz

Hence, the value of the lowest frequency where standing node is observed is 324 Hz

04

Step 4(b): Calculation of number of nodes

At the frequency of 324 Hz , the number of antinodes is

Antinodes=n1+n2=2+5=7

Totalnumberofnodes=numberofantinodes+1=7+1=8

Hence, the total number of standing nodes is 8.

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Most popular questions from this chapter

The tension in a wire clamped at both ends is doubled without appreciably changing the wire’s length between the clamps. What is the ratio of the new to the old wave speed for transverse waves traveling along this wire?

Figure 16-25agives a snapshot of a wave traveling in the direction of positive xalong a string under tension. Four string elements are indicated by the lettered points. For each of those elements, determine whether, at the instant of the snapshot, the element is moving upward or downward or is momentarily at rest. (Hint:Imagine the wave as it moves through the four string elements, as if you were watching a video of the wave as it traveled rightward.) Figure 16-25bgives the displacement of a string element located at, say, x=0as a function of time. At the lettered times, is the element moving upward or downward or is it momentarily at rest?

The equation of a transverse wave traveling along a very long string is y=6.0sin(0.020Ï€³æ+4.0Ï€³Ù), where x andy are expressed in centimeters and is in seconds. (a) Determine the amplitude,(b) Determine the wavelength, (c)Determine the frequency, (d) Determine the speed, (e) Determine the direction of propagation of the wave, and (f) Determine the maximum transverse speed of a particle in the string. (g)What is the transverse displacement atx = 3.5 cmwhen t = 0.26 s?

These two waves travel along the same string:

y1(x,t)=(4.60mm)sin(2Ï€³æ-400Ï€³Ù)y2(x,t)=(5.60mm)sin(2Ï€³æ-400Ï€³Ù+0.80Ï€°ù²¹»å)

What is the amplitude (a) and (b) what is the phase angle (relative to wave 1) of the resultant wave? (c) If a third wave of amplitude 5.00 mmis also to be sent along the string in the same direction as the first two waves, what should be its phase angle in order to maximize the amplitude of the new resultant wave?

If a transmission line in a cold climate collects ice, the increased diameter tends to cause vortex formation in a passing wind. The air pressure variations in the vortexes tend to cause the line to oscillate (gallop), especially if the frequency of the variations matches a resonant frequency of the line. In long lines, the resonant frequencies are so close that almost any wind speed can set up a resonant mode vigorous enough to pull down support towers or cause the line to short outwith an adjacent line. If a transmission line has a length of 347 m, a linear density of 3.35 kg/m, and a tension of 65.2 MN. What are (a) the frequency of the fundamental mode and (b) the frequency difference between successive modes?

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