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Figure 16-46 shows transverse accelerationayversus time tof the point on a string at x=0, as a wave in the form ofy(x,t)=ymsin(kx-Ó¬³Ù+Ï•)passes through that point. The scale of the vertical axis is set byas=400m/s2. What isÏ•? (Caution:A calculator does not always give the proper inverse trig function, so check your answer by substituting it and an assumed value ofÓ¬intoy(x,t)and then plotting the function.

Short Answer

Expert verified

The value ofϕ is 2.9 rad or -3.4 rad.

Step by step solution

01

The given data

i) Transverse acceleration (ay) vs t graph at x=0.

ii) The wave equation is yx,t=ymsinkx-Ó¬t+Ï•.

iii) The scale of the vertical axis is set by, as=400m/s2.

02

Understanding the concept of the wave equation

We can find the equation of the wave at x = 0 as given in the graph. From the slope of the graph, we can predict the approximate value of the phase constant. Then, from the expression for the acceleration of the given wave at t = 0, we can easily get the value of the phase constant.

03

Calculation of phase constant

The equation of the wave is given as,

y=ymsin(kx-Ó¬t+Ï•)

At x = 0, it becomes,

y=ymsin(-Ó¬t+Ï•) (1)

At x = 0, acceleration is maximum. Hence,

ay=amay=-Ó¬2y (a)

From equation (1), the acceleration of the wave is given as:


ay=-Ó¬2ysin(-Ó¬t+Ï•)

This is the equation for the given graph.

The slope of the graph is given as:

daydt=ddt-Ó¬2ymsin-Ó¬t+Ï•=Ó¬2ymcos-Ó¬t+Ï•

From the given graph, we can conclude that the slope of the graph at t = 0 is negative. Hence,

Ӭ2ymcos-Ӭ0+ϕ<0Ӭ3ymcosϕ<0

From this, we can infer that,

cosϕ<0

This implies thatϕis in betweenπ2and π or πand 3π2rad.

From the graph, we can write that,
am=400ms2anday=100ms2.

Hence, From equation (a), we get,

ay=-400sinϕ-100m/s2=-400sinϕϕ=sin-114=0.25rad

Since,

sinϕ=sinπ-ϕϕ=2.9rad

Also,

ϕ=2.9-2π=-3.38≅-3.4rad

Therefore, the value of ϕis 2.9 rad or -3.5 rad.

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A continuous traveling wave with amplitude Ais incident on a boundary. The continuous reflection, with a smaller amplitude B, travels back through the incoming wave. The resulting interference pattern is displayed in Fig. 16-51. The standing wave ratio is defined to beSWR=A+BA-B

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