/*! 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} Problem 28 In the 25 -ft Space Simulator fa... [FREE SOLUTION] | 91Ó°ÊÓ

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In the 25 -ft Space Simulator facility at NASA's Jet Propulsion Laboratory, a bank of overhead arc lamps can produce light of intensity \(2500 \mathrm{~W} / \mathrm{m}^{2}\) at the floor of the facility. (This simulates the intensity of sunlight near the planet Venus.) Find the average radiation pressure (in pascals and in atmospheres) on (a) a totally absorbing section of the floor and (b) a totally reflecting section of the floor. (c) Find the average momentum density (momentum per unit volume) in the light at the floor.

Short Answer

Expert verified
The average radiation pressure is \(8.33 \times 10^{-6}\) Pa for absorbing and \(1.67 \times 10^{-5}\) Pa for reflecting. The average momentum density is \(2.78 \times 10^{-14}\) kg/(m³s).

Step by step solution

01

Understanding Radiation Pressure

Radiation pressure is the force exerted by light on a surface per unit area. The formula to calculate radiation pressure depends on whether the surface is absorbing or reflecting. For a totally absorbing surface, the pressure \( P \) is given by \( P = \frac{I}{c} \), where \( I \) is the intensity of the light and \( c \) is the speed of light (approximately \( 3 \times 10^8 \) m/s). For a totally reflecting surface, the pressure is \( 2 \times \frac{I}{c} \) because the light momentum is reversed upon reflection.
02

Calculating Radiation Pressure on a Totally Absorbing Surface

Using the formula \( P = \frac{I}{c} \), where \( I = 2500 \text{ W/m}^2 \):\[ P = \frac{2500}{3 \times 10^8} = 8.33 \times 10^{-6} \text{ Pa}. \]
03

Converting to Atmospheres

To convert the pressure from pascals to atmospheres, use the conversion factor \( 1 \text{ atm} = 1.01325 \times 10^5 \text{ Pa} \):\[ P_{atm} = \frac{8.33 \times 10^{-6}}{1.01325 \times 10^5} \approx 8.22 \times 10^{-11} \text{ atm}. \]
04

Calculating Radiation Pressure on a Totally Reflecting Surface

For a totally reflecting surface, the pressure is given by \( 2 \times \frac{I}{c} \):\[ P = 2 \times \frac{2500}{3 \times 10^8} = 1.67 \times 10^{-5} \text{ Pa}. \]Converting to atmospheres:\[ P_{atm} = \frac{1.67 \times 10^{-5}}{1.01325 \times 10^5} \approx 1.65 \times 10^{-10} \text{ atm}. \]
05

Calculating Average Momentum Density

The average momentum density (momentum per unit volume) in light is given by \( \frac{I}{c^2} \):\[ \frac{2500}{(3 \times 10^8)^2} = 2.78 \times 10^{-14} \text{ kg/(m}^3\text{s}). \]

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Key Concepts

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

Light Intensity
Light intensity refers to the amount of energy that hits a surface per unit area and is measured in watts per square meter (\( \text{W/m}^2 \)). In the context of radiation pressure, the specific intensity of light plays a critical role in determining the force that light exerts on a surface. For our particular example, the intensity has been given as \( 2500 \, \mathrm{W/m}^{2} \). This simulates the natural sunlight experience near Venus, providing a realistic setup to study radiation pressure effects.
Light intensity is fundamental in calculating radiation pressure since the higher the intensity, the greater the influence on the surface it strikes. This intensity directly affects whether the surface absorbs or reflects the light, impacting the momentum transfer and consequently the radiation pressure exerted.
Understanding light intensity is essential because it not only helps us model the pressure light will exert but also aids in comprehending solar radiation interactions with various surfaces, like satellites or planetary atmospheres.
Momentum Density
Momentum density is a concept used to describe the amount of momentum in a unit volume of space occupied by light. It might sound complex, but it's quite simple when broken down. Momentum, in this context, refers to the product of light's energy and its velocity. The average momentum density in light can be calculated using the formula \( \frac{I}{c^2} \), where \( I \) is the light intensity, and \( c \) is the speed of light.
By applying this formula, we find that the momentum density is \( 2.78 \times 10^{-14} \text{ kg/(m}^3\text{s}) \). This value represents how much momentum each cubic meter of the light's volume holds, offering insight into the force distribution in the scenario. This is crucial for calculations involving light-matter interactions, especially when assessing the effects of light on free-floating objects or gases in space.
Understanding momentum density helps explain the mechanics behind photonic thrust and its impact on spacecraft or even understanding stellar phenomena like radiation-driven stellar winds.
Photonic Pressure
The concept of photonic pressure, or radiation pressure, is all about the effect when light exerts a force on a surface. Imagine tiny particles of light, photons, hitting a surface and forcing it in some direction. The photonic pressure is derived from the light's intensity and depends on whether the light is absorbed or reflected. Light's interaction with surfaces behaves differently based on their properties:
  • For an absorptive surface, photonic pressure is calculated using \( P = \frac{I}{c} \).
  • For a reflective surface, the pressure is higher, \( P = 2 \times \frac{I}{c} \), because the photons bounce back, doubling their momentum transfer.
In our context, the photonic pressure on a totally absorbing section of a floor is \( 8.33 \times 10^{-6} \) pascals, while a reflective section experiences \( 1.67 \times 10^{-5} \) pascals. These differences illustrate how reflection can significantly amplify the pressure applied by light.
Photonic pressure is not just theoretical; it has practical uses in science and engineering, like designing solar sails for space exploration, which rely on exploiting this pressure to propel spacecraft.
Reflective and Absorptive Surfaces
Reflective and absorptive surfaces react distinctively when they interact with incoming light, affecting radiation pressure substantially. Absorptive surfaces take in light energy without returning it to the environment. This means they absorb photons’ momentum, reducing it to radiation pressure calculated directly as \( P = \frac{I}{c} \).
Reflective surfaces, conversely, rebound the photons. This reflection implies the surfaces double the momentum exchange, as the incoming and outgoing momenta both influence the force felt. Thus, their radiation pressure is calculated as \( P = 2 \times \frac{I}{c} \).
For the exercise's scenario, understanding these surface interactions clarifies why reflective materials encounter more significant photonic forces than absorptive ones. Additionally, choice of surface type plays a crucial role in practical applications:
  • Reflective surfaces are often used in mirrors to maximize light manipulation and in solar sails to harness radiation pressure for propulsion.
  • Absorptive materials are utilized where light needs to be converted into heat energy, such as solar panels.
Grasping the implications of these interactions is vital for designing technologies suited for light-based applications.

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Most popular questions from this chapter

Very short pulses of high-intensity laser beams are used to repair detached portions of the retina of the eye. The brief pulses of energy absorbed by the retina weld the detached portions back into place. In one such procedure, a laser beam has a wavelength of \(810 \mathrm{~nm}\) and delivers \(250 \mathrm{~mW}\) of power spread over a circular spot \(510 \mu \mathrm{m}\) in diameter. The vitreous humor (the transparent fluid that fills most of the eye) has an index of refraction of \(1.34\). (a) If the laser pulses are each \(1.50 \mathrm{~ms}\) long. how much energy is delivered to the retina with each pulse? (b) What average pressure does the pulse of the laser beam exert on the retina as it is fully absorbed by the circular spot? (c) What are the wavelength and frequency of the laser light inside the vitreous humor of the eye? (d) What are the maximum values of the electric and magnetic fields in the laser beam? ?

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