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A wave pulse is travelling on a string with a speed \(v\) towards the positive \(X\) -axis. The shape of the string at \(t=0\) is given by \(g(x)=A \sin (x / a)\), where \(A\) and \(a\) are constants. (a) What are the dimensions of \(A\) and \(a ?\) (b) Write the equation of the wave for a general time \(t\), if the wave speed is \(v\)

Short Answer

Expert verified
The dimension of \(A\) is \([L]\) and \(a\) is \([L]\). The wave equation is \(f(x, t) = A \sin \left(\frac{x - vt}{a}\right)\).

Step by step solution

01

Determine the Dimension of A

To find the dimension of \(A\), observe that \(g(x)\) represents a displacement, typically measured in meters. Since \(A \sin(x/a)\) represents a displacement, and \(\sin(x/a)\) being dimensionless, \(A\) must have the dimensions of displacement. Therefore, the dimension of \(A\) is \([L]\), where \(L\) stands for length.
02

Determine the Dimension of a

Next, let's determine the dimension of \(a\). The argument of the sine function \(x/a\) must be dimensionless. This means \(\frac{x}{a}\) has no units, so \(x\) and \(a\) must have the same dimensions. Since \(x\) is a position, its dimension is \([L]\). Therefore, \(a\) also has the dimension \([L]\).
03

Write the Equation of the Wave at General Time t

Since the wave pulse travels with a speed \(v\) along the positive \(X\)-axis, the general equation for a wave moving in this direction is given by the function displaced by \(vt\) in time. Thus, the displacement function becomes \(f(x - vt) = g(x - vt)\). Substitute the given initial shape function to get the general wave equation: \[ f(x, t) = A \sin \left(\frac{x - vt}{a}\right) \].
04

Finalize the Wave Equation

The equation for the wave traveling to the right is now complete. Make sure units and dimensions are consistent: amplitude \(A\) is in meters (\([L]\)), and the argument of the sine function is dimensionless due to the form \((x - vt)/a\). The wave equation is: \[ f(x, t) = A \sin \left(\frac{x - vt}{a}\right) \].

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Dimensions of Physical Quantities
Understanding the dimensions of physical quantities is crucial in physics as it helps ensure equations and solutions are physically meaningful and consistent. Dimensions are essentially the units associated with a quantity that define its nature, such as length, mass, or time. For example, in wave physics:
  • Displacement, like the wave amplitude, has dimensions of length \( [L] \).
  • Speed is a measure of how fast something moves, having dimensions of \( [LT^{-1}] \) due to the relation between length and time.
In our wave equation on a string, we identify the dimensions of quantities like \( A \) and \( a \). Here, \( A \), representing amplitude, directly involves displacement, hence having dimensions of \( [L] \). Similarly, since \( a \) is involved in creating a dimensionless argument inside the sine function, because \( \frac{x}{a} \) has no unit, \( a \) must share its dimension with \( x \), which is also \( [L] \). These dimensions critically help keep the sine argument dimensionless, where the functionality depends on this nature.
Trigonometric Functions in Physics
Trigonometric functions like sine and cosine are extensively utilized in physics to model periodic phenomena such as waves. These functions help describe a wide variety of waveforms, including light, sound, and ocean waves.A sine function \( \sin(x) \) is often used because it naturally oscillates between -1 and 1, representing repeating cycles which are central to wave behaviors.In physics:
  • Sine functions capture oscillations that translate spatial wave patterns, such as those on a string.
  • They are dimensionless, meaning their argument (e.g., \( \frac{x}{a} \)) must also be without dimension.
This property aids in maintaining consistency within wave equations when adopting initial conditions or transformations over time.For example, in the wave equation \( f(x, t) = A \sin \left(\frac{x - vt}{a}\right) \), the argument \( \frac{x - vt}{a} \) remains dimensionless, allowing the trigonometric sine efficiently model the wave motion over time without distorting physical units.
Wave Motion on a String
Wave motion on a string is a classic illustration of transverse waves in physics. In transverse waves, the displacement of the medium (the string) is perpendicular to the direction of wave travel. Key characteristics include:
  • Speed (\( v \)): This defines how quickly the wave pulse travels along the string.
  • Amplitude (\( A \)): This represents the maximum displacement from the equilibrium position, indicating wave energy.
  • Wavelength, related to \( a \): Distance over which the wave shape repeats. This aligns with the initial shape function variable \( a \).
In context:- The string at time \( t = 0 \) starts as \( g(x) = A \sin(x / a) \), showing the shape.- Over time, this pattern translates along the string maintained by the wave speed \( v \), forming \( f(x, t) = A \sin \left(\frac{x - vt}{a}\right) \).Through visual modeling or mathematical representation, these factors give insight into how energy is transferred through a medium without physically moving the medium itself. Transverse wave studies help illustrate principles in fields like optics and acoustics, where similar wave properties apply.

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Most popular questions from this chapter

A pulse travelling on a string is represented by the function $$ y=\frac{a^{3}}{(x-v t)^{2}+a^{2}} $$ where \(a=5 \mathrm{~mm}\) and \(v=20 \mathrm{~cm} \mathrm{~s}^{-1} .\) Sketch the shape of the string at \(t=0,1 \mathrm{~s}\) and \(2 \mathrm{~s}\). Take \(x=0\) in the middle of the string.

A block of mass \(m\) moves on a horizontal circle against the wall of a cylindrical room of radius \(R\). The floor of the room on which the block moves is smooth but the friction coefficient between the wall and the block is \(\mu\). The block is given an initial speed \(v_{0}\). As a function of the speed \(v\) write (a) the normal force by the wall on the block, (b) the frictional force by the wall and (c) the tangential acceleration of the block. (d) Integrate the tangential acceleration \(\left(\frac{d v}{d t}=v \frac{d v}{d s}\right)\) to obtain the speed of the block after one revolution.

In a children's park a heavy rod is pivoted at the centre and is made to rotate about the pivot so that the rod always remains horizontal. Two kids hold the rod near the ends and thus rotate with the rod (figure 7-E2). Let the mass of each kid be \(15 \mathrm{~kg}\), the distance between the points of the rod where the two kids hold it be \(3 \cdot 0 \mathrm{~m}\) and suppose that the rod rotates at the rate of 20 revolutions per minute. Find the force of friction exerted by the rod on one of the kids.

A steel wire fixed at both ends has a fundamental frequency of \(200 \mathrm{~Hz}\). A person can hear sound of maximum frequency \(14 \mathrm{kHz}\). What is the highest harmonic that can be played on this string which is audible to the person?

Three resonant frequencies of a string are 90,150 and \(210 \mathrm{~Hz} .\) (a) Find the highest possible fundamental frequency of vibration of this string. (b) Which harmonics of the fundamental are the given frequencies ? (c) Which overtones are these frequencies ? (d) If the length of the string is \(80 \mathrm{~cm}\), what would be the speed of a transverse wave on this string ?

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