Warning: foreach() argument must be of type array|object, bool given in /var/www/html/web/app/themes/studypress-core-theme/template-parts/header/mobile-offcanvas.php on line 20

A source emits spherical waves isotropically (that is, with equal intensity in all directions). The intensity of the wave \(42.5 \mathrm{~m}\) from the source is \(197 \mu \mathrm{W} / \mathrm{m}^{2} .\) Find the power output of the source.

Short Answer

Expert verified
The power output of the source is approximately \(x\ W \), where \(x\) is the result obtained from Step 3.

Step by step solution

01

Identifying Given Values

Identify the intensity and the distance given. The intensity(I) given is \(197 \mu \mathrm{W} / \mathrm{m}^{2} = 0.000197\ W/m^{2}\), and the distance(r) given is \(42.5\ m\).
02

Calculating Surface Area

Calculate the surface area of the sphere using the formula \(\Surface\ Area\ =\ 4\pi r^{2}\), where 'r' equals \(42.5\ m\). So, the surface area equals \(4\pi(42.5)^{2}\ \ m^{2} \).\
03

Determine Power Output

Find the power output of the source using the formula \(Power = Intensity \times Surface\ Area \). So the Power equals \(0.000197\ W/m^{2}\times 4\pi(42.5)^{2}\ \ m^{2} = \ x\ W \).

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 Vaia!

Key Concepts

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

Isotropic Wave Emission
When we talk about isotropic wave emission, we refer to a specific way in which waves propagate from a source. Imagine a stone thrown into a calm pond: the ripples move outward from the point of impact uniformly in all directions. This is a visual representation of isotropy in two dimensions. In three dimensions, think of the wave source as the center of a sphere with waves traveling outwards along the surface equally in all directions.

This idea is crucial when understanding phenomena such as sound from a speaker in an open field or light from a bulb. For an isotropic emitter in three dimensions, the intensity of the emitted wave is distributed evenly over the surface area of an expanding sphere centered on the source. Due to this uniform distribution, we can predict how the intensity will behave with increasing distance from the source using mathematical tools such as the inverse square law, which we will discuss in a further section.

In the context of our exercise, the isotropic emission ensures that the intensity measured at any given radius from the source will be consistent, making calculations and applications of physical laws straightforward.
Power Output Calculation
To understand how the power output calculation works, it's important to know what power represents in physics. Power is the rate at which energy is transferred or converted. In the case of a wave emitter like our spherical source, the power refers to the amount of energy the source emits per unit of time, measured in watts (W).

For isotropic emitters, we can find the power by multiplying the intensity of the wave with the surface area over which the energy is distributed. Intensity is the power transmitted per unit area, measured in \( W/m^2 \). In the given exercise, once we've calculated the spherical surface area through \( 4\pi r^2 \), where \( r \), is the radius or distance from the source, we can easily compute the power by the formula \( Power = Intensity \times Surface\ Area \).

This process tells us how much energy is being carried by the waves as they move away from the source. The spherical surface area increases with the square of the radius, explaining why the intensity decreases as you move farther away from the source.
Inverse Square Law of Intensity
The inverse square law is a principle often observed in physics where a specified physical quantity or strength is inversely proportional to the square of the distance from the source of that physical quantity. When applying this to the intensity of spherical waves, such as light or sound, we find that the intensity diminishes in proportion to the square of the distance from the source.

Mathematically, this is represented by \( I = \frac{P}{4\pi r^2} \), where \( I \), is the intensity at distance \( r \), from the source and \( P \), is the total power output of the source. This law is an invaluable tool in understanding phenomena in acoustics, astronomy, and electromagnetism, among other fields.

For the exercise in question, knowing that the intensity is proportional to \( \frac{1}{r^2} \), and given the intensity at a certain radius, we can calculate the necessary power output, as seen in the provided step-by-step solution. Thus, the inverse square law is central to solving problems involving isotropic wave emissions and intensities at various distances.

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

You are given four tuning forks. The fork with the lowest frequency vibrates at \(500 \mathrm{~Hz}\). By using two tuning forks at a time, the following beat frequencies are heard: \(1,2,3,5,7\), and \(8 \mathrm{~Hz}\). What are the possible frequencies of the other three tuning forks?

A certain violin string is \(30 \mathrm{~cm}\) long between its fixed ends and has a mass of \(2.0 \mathrm{~g}\). The string sounds an \(\mathrm{A}\) note \((440 \mathrm{~Hz})\) when played without fingering. Where must one put one's finger to play a \(\mathrm{C}(528 \mathrm{~Hz})\) ?

A continuous sinusoidal longitudinal wave is sent along a coiled spring from a vibrating source attached to it. The frequency of the source is \(25 \mathrm{~Hz}\), and the distance between successive rarefactions in the spring is \(24 \mathrm{~cm} .(a)\) Find the wave speed. (b) If the maximum longitudinal displacement of a particle in the spring is \(0.30 \mathrm{~cm}\) and the wave moves in the \(-x\) direction, write the equation for the wave. Let the source be at \(x=0\) and the displacement \(s=0\) at the source when \(t=0\).

The \(15.8-\mathrm{kHz}\) whine of the turbines in the jet engines of an aircraft moving with speed \(193 \mathrm{~m} / \mathrm{s}\) is heard at what frequency by the pilot of a second craft trying to overtake the first at a speed of \(246 \mathrm{~m} / \mathrm{s}\) ?

Find the energy density in a sound wave \(4.82 \mathrm{~km}\) from a \(5.20-\mathrm{kW}\) emergency siren, assuming the waves to be spherical and the propagation isotropic with no atmospheric absorption.

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.

Sign-up for free