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\(\bullet\) At the floor of a room, the intensity of light from bright overhead lights is 8.00 \(\mathrm{W} / \mathrm{m}^{2} .\) Find the radiation pressure on a totally absorbing section of the floor.

Short Answer

Expert verified
The radiation pressure is \(2.67 \times 10^{-8} \, \mathrm{N/m^2}\).

Step by step solution

01

Understanding Radiation Pressure

Radiation pressure, which is the pressure exerted by light, depends on the intensity of the light and the nature of the surface it falls on. For a totally absorbing surface, the radiation pressure can be calculated using the formula: \( P = \frac{I}{c} \), where \( P \) is the radiation pressure, \( I \) is the intensity of light, and \( c \) is the speed of light in a vacuum (approximately \( 3 \times 10^8 \mathrm{m/s} \)).
02

Substituting Known Values

In this problem, the intensity \( I \) is given as 8.00 \( \mathrm{W/m^2} \). We substitute \( I = 8.00 \, \mathrm{W/m^2} \) and \( c = 3.00 \times 10^8 \, \mathrm{m/s} \) into the formula: \[ P = \frac{8.00}{3.00 \times 10^8} \].
03

Performing the Calculation

Calculate the value of \( P \) using the substituted values: \[ P = \frac{8.00}{3.00 \times 10^8} = 2.67 \times 10^{-8} \, \mathrm{N/m^2} \]. This is the radiation pressure exerted on a totally absorbing section of the floor.

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Key Concepts

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

Intensity of Light
The intensity of light refers to the amount of energy that light transfers to a surface per unit area in a given time period. It is denoted by the symbol \( I \) and measured in watts per square meter (\( \mathrm{W/m^2} \)). The concept of light intensity is crucial when calculating radiation pressure, especially on a surface that either absorbs or reflects light. In the given exercise, the intensity of light is provided as 8.00 \( \mathrm{W/m^2} \), which serves as a key value for determining how much pressure the light exerts on a surface.Understanding light intensity helps to assess how energy from light sources—like lamps, the sun, or lasers—affects surfaces they hit. This measurement can vary according to the source's distance and output power, affecting radiation pressure calculations.
Speed of Light
The speed of light, represented by the symbol \( c \), is a fundamental constant in physics. In a vacuum, the speed of light is approximately \( 3.00 \times 10^8 \mathrm{m/s} \). This value is crucial when calculating the radiation pressure as it relates to how quickly light energy travels through space to meet a surface.The speed of light not only influences radiation pressure calculations but also plays a vital role in other physics phenomena like time dilation and length contraction in relativity. In our problems related to radiation pressure, the speed of light acts as a divisor in the formula \( P = \frac{I}{c} \), because the quicker light moves, the less pressure it inherently exerts over an infinitesimally small time.
Totally Absorbing Surface
A totally absorbing surface is one that captures all the incoming light energy without reflecting any of it. When light hits such a surface, it translates all of its energy into either heat or another form of energy.In the context of radiation pressure, understanding how materials absorb light is very important. For a surface that absorbs everything, the calculation of radiation pressure is straightforward because all the light energy contributes to the pressure. The formula used for a totally absorbing surface is \( P = \frac{I}{c} \). This contrasts with a perfectly reflecting surface, where the pressure would be doubled, as the light bounces back, exerting additional force.
Radiation Pressure Calculation
Radiation pressure is the force per unit area exerted by light on a surface. It results from the momentum carried by photons, the particles of light, being transferred to the surface. It's a small quantity but is significant in settings like solar sails in space or very sensitive scientific instruments.To calculate radiation pressure on a totally absorbing surface, use the formula: \[ P = \frac{I}{c} \]Here, \( P \) is the radiation pressure in \( \mathrm{N/m^2} \), \( I \) is the intensity of light, and \( c \) is the speed of light. For the given exercise, where \( I = 8.00 \, \mathrm{W/m^2} \) and \( c = 3.00 \times 10^8 \, \mathrm{m/s} \), the calculation goes as follows:\[ P = \frac{8.00}{3.00 \times 10^8} = 2.67 \times 10^{-8} \, \mathrm{N/m^2} \]This formula simplifies understanding by showing the direct proportionality of radiation pressure to light intensity, while inversely proportional to the speed at which light travels.

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Most popular questions from this chapter

\(\bullet\) Fields from a lightbulb. We can reasonably model a 75 \(\mathrm{W}\) incandescent lightbulb as a sphere 6.0 \(\mathrm{cm}\) in diameter. Typically, only about 5\(\%\) of the energy goes to visible light; the rest goes largely to nonvisible infrared radiation. (a) What is the visible light intensity (in \(\mathrm{W} / \mathrm{m}^{2} )\) at the surface of the bulb? (b) What are the amplitudes of the electric and magnetic fields at this surface, for a sinusoidal wave with this intensity?

\(\bullet\) Light inside the eye. The vitreous humor, a transparent, gelatinous fluid that fills most of the eyeball, has an index of refraction of 1.34 . Visible light ranges in wavelength from 400 \(\mathrm{nm}\) (violet) to \(700 \mathrm{nm}(\mathrm{red}),\) as measured in air. This light travels through the vitreous humor and strikes the rods and cones at the surface of the retina. What are the ranges of (a) the wavelength, (b) the frequency, and (c) the speed of the light just as it approaches the retina within the vitreous humor?

\(\bullet$$\bullet\) You want to support a sheet of fireproof paper horizontally, using only a vertical upward beam of light spread uniformly over the sheet. There is no other light on this paper. The sheet measures 22.0 \(\mathrm{cm}\) by 28.0 \(\mathrm{cm}\) and has a mass of 1.50 \(\mathrm{g}\) . (a) If the paper is black and hence absorbs all the light that hits it, what must be the intensity of the light beam? (b) For the light in part (a), what are the maximum values of its electric and magnetic fields? (c) If the paper is white and hence reflects all the light that hits it, what intensity of light beam is needed to support it? (d) To see if it is physically reasonable to expect to support a sheet of paper this way, calculate the intensity in a typical 0.500 \(\mathrm{mW}\) laser beam that is 1.00 \(\mathrm{mm}\) in diameter and compare this value with your answer in part (a).

\(\bullet$$\bullet\) A plane sinusoidal electromagnetic wave in air has a wave- length of 3.84 \(\mathrm{cm}\) and an \(\vec{\boldsymbol{E}}\) field amplitude of 1.35 \(\mathrm{V} / \mathrm{m}\) . (a) What is the frequency of the wave? (b) What is the \(\vec{\boldsymbol{B}}\) field amplitude? (c) What is the intensity? (d) What average force does this radiation exert perpendicular to its direction of propagation on a totally absorbing surface with area 0.240 \(\mathrm{m}^{2}\) ?

\(\bullet\) A glass plate having parallel faces and a refractive index of 1.58 lies at the bottom of a liquid of refractive index \(1.70 . \mathrm{A}\) ray of light in the liquid strikes the top of the glass at an angle of incidence of \(62.0^{\circ} .\) Compute the angle of refraction of this light in the glass.

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