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Response of the Eye. The human eye is most sensitive to green light of wavelength 505 \(\mathrm{nm}\) . Experiments have found that when people are kept in a dark room until their eyes adapt to the darkness, a single photon of green light will trigger receptor cells in the rods of the retina. (a) What is the frequency of this photon? (b) How much energy (in joules and electron volts) does it deliver to the receptor cells? (c) to appreciate what a small amount of energy this is, calculate how fast a typical bacterium of mass \(9.5 \times 10^{-12} \mathrm{g}\) would move if it had that much energy.

Short Answer

Expert verified
(a) 5.94 脳 10鹿鈦 Hz, (b) 3.94 脳 10鈦宦光伖 J or 2.46 eV, (c) 9.11 脳 10鈦宦 m/s.

Step by step solution

01

Convert Wavelength to Frequency

We start by using the relationship between wavelength and frequency. The speed of light is given by the equation: \[ c = \lambda \cdot f \] where \( c \) is the speed of light (\( 3 \times 10^8 \ \mathrm{m/s} \)), \( \lambda \) is the wavelength (505 nm or \( 505 \times 10^{-9} \ \mathrm{m} \)), and \( f \) is the frequency. Solving for frequency, we have: \[ f = \frac{c}{\lambda} = \frac{3 \times 10^8}{505 \times 10^{-9}} \approx 5.94 \times 10^{14} \ \mathrm{Hz} \].
02

Calculate Energy in Joules

The energy of a photon can be calculated using the equation: \[ E = h \cdot f \] where \( h \) is Planck's constant (\( 6.626 \times 10^{-34} \ \mathrm{Js} \)). Using the frequency from the previous step, \( f = 5.94 \times 10^{14} \ \mathrm{Hz} \), we find: \[ E = 6.626 \times 10^{-34} \cdot 5.94 \times 10^{14} \approx 3.94 \times 10^{-19} \ \mathrm{J} \].
03

Convert Energy to Electron Volts

To convert the energy from joules to electron volts, we use the conversion factor \( 1 \ \mathrm{eV} = 1.602 \times 10^{-19} \ \mathrm{J} \). Therefore, the energy in electron volts is: \[ \frac{3.94 \times 10^{-19}}{1.602 \times 10^{-19}} \approx 2.46 \ \mathrm{eV} \].
04

Calculate Velocity of a Bacterium

The kinetic energy of a bacterium can be described by the equation: \[ K.E. = \frac{1}{2} m v^2 \] where \( m \) is the mass of the bacterium (\( 9.5 \times 10^{-12} \ \mathrm{g} \) or \( 9.5 \times 10^{-15} \ \mathrm{kg} \)), and \( v \) is the velocity. We equate this energy to the photon's energy: \[ \frac{1}{2} \cdot 9.5 \times 10^{-15} \cdot v^2 = 3.94 \times 10^{-19} \]. Solving for \( v \), we get: \[ v^2 = \frac{2 \cdot 3.94 \times 10^{-19}}{9.5 \times 10^{-15}} \approx 8.29 \times 10^{-5} \]. Taking the square root gives: \[ v \approx 9.11 \times 10^{-3} \ \mathrm{m/s} \].

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Key Concepts

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

Wavelength and Frequency
Understanding the relationship between wavelength and frequency is essential when studying light properties, such as those emitted by a photon. The speed of light (\(c\), approximately \(3 \times 10^8\) \(\mathrm{m/s}\)), remains constant. However, both wavelength (\(\lambda\)) and frequency (\(f\)) determine its characteristics. This relationship is expressed by the equation: \[ c = \lambda \cdot f \] Wavelength is the distance between successive peaks of a wave and is usually measured in meters. Frequency is the number of waves that pass a given point per second, measured in hertz (\(\mathrm{Hz}\)). Green light with a wavelength of 505 \(\mathrm{nm}\) can be converted into frequency using the formula: \[ f = \frac{c}{\lambda} = \frac{3 \times 10^8}{505 \times 10^{-9}} \approx 5.94 \times 10^{14} \ \mathrm{Hz} \] Knowing how to switch between wavelength and frequency is crucial when analyzing photon energy, which we will explore further in conjunction with Planck's Constant.
Planck's Constant
Planck's constant (\(h\)) is a fundamental constant used in quantifying energy at the quantum level. It connects the energy of a photon to its frequency. Originating from Max Planck's work on black body radiation, its value is approximately \(6.626 \times 10^{-34} \ \mathrm{Js}\). Employing Planck's constant, the energy (\(E\)) of a photon can be calculated as follows: \[ E = h \cdot f \] Utilizing the frequency determined earlier, \(f = 5.94 \times 10^{14} \ \mathrm{Hz}\), we can find the energy of a green photon: \[ E = 6.626 \times 10^{-34} \cdot 5.94 \times 10^{14} \approx 3.94 \times 10^{-19} \ \mathrm{J} \] Energy is often expressed in joules, but when dealing with atomic scales, electron volts (\(\mathrm{eV}\)) might be more intuitive. Conversion to electron volts involves dividing by the conversion factor \(1 \ \mathrm{eV} = 1.602 \times 10^{-19} \ \mathrm{J}\), yielding: \[ \frac{3.94 \times 10^{-19}}{1.602 \times 10^{-19}} \approx 2.46 \ \mathrm{eV} \] Planck's constant is pivotal in understanding quantum mechanics, underpinning the explanation of photon interactions like those that trigger receptor cells in your eyes.
Kinetic Energy
Kinetic energy (\(K.E.\)) is the energy possessed by an object due to its motion. For a mass \(m\) with velocity \(v\), it is mathematically depicted by the formula: \[ K.E. = \frac{1}{2} m v^2 \] To appreciate the extremely small energy carried by a photon, compare it to something tangible. Imagine transferring that energy to a bacterium of mass \(9.5 \times 10^{-15} \ \mathrm{kg}\). By equating the photon's energy to the bacterium's kinetic energy and solving for velocity, we find: \[ \frac{1}{2} \cdot 9.5 \times 10^{-15} \cdot v^2 = 3.94 \times 10^{-19} \] Thus: \[ v^2 = \frac{2 \cdot 3.94 \times 10^{-19}}{9.5 \times 10^{-15}} \approx 8.29 \times 10^{-5} \] Taking the square root, \(v \approx 9.11 \times 10^{-3} \ \mathrm{m/s}\). This illustrates that even a minuscule photon energy could move an ultralight object like a bacterium at observable speeds, demonstrating the photon's capacity to impart motion through its kinetic energy.

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Most popular questions from this chapter

Two stars, both of which behave like ideal blackbodies, radiate the same total energy per second. The cooler one has a surface temperature \(T\) and 3.0 times the diameter of the hotter star. (a) What is the temperature of the hotter star in terms of \(T\) ? (b) What is the ratio of the peak-intensity wavelength of the hot star to the peak-intensity wavelength of the cool star?

An x-ray photon is scattered from a free electron (mass m) at rest. The wavelength of the scattered photon is \(\lambda^{\prime},\) and the final speed of the struck electron is \(v\) . (a) What was the initial wave-length \(\lambda\) of the photon? Express your answer in terms of \(\lambda^{\prime}, v,\) and \(m\) . (Hint: Use the relativistic expression for the electron kinetic energy.) (b) Through what angle \(\phi\) is the photon scattered? Express your answer in terms of \(\lambda, \lambda^{\prime},\) and \(m .\) (c) Evaluate your results in parts \((a)\) and \((b)\) for a wavelength of \(5.10 \times 10^{-3} \mathrm{nm}\) for the scattered photon and a final electron speed of \(1.80 \times 10^{8} \mathrm{m} / \mathrm{s}\) . Give \(\phi\) in degrees.

(a) Derive an expression for the total shift in photon wave- length after two successive Compton scatterings from electrons at rest. The photon is scattered by an angle \(\theta_{1}\) in the first scattering and by \(\theta_{2}\) in the second. (b) In general, is the total shift in wave-length produced by two successive scatterings of an angle \(\theta / 2\) the same as by a single scattering of \(\theta ?\) If not, are there any specific values of \(\theta,\) other than \(\theta=0\) , for which the total shifts are the same? (c) Use the result of part (a) to calculate the total wave- length shift produced by two successive Compton scatterings of \(30.0^{\circ}\) each. Express your answer in terms of \(h / m c .\) (d) What is the wavelength shift produced by a single Compton scattering of \(60.0^{\circ} ?\) Compare to the answer in part (c).

Blue Supergiants. A typical blue supergiant star (the type that explode and leave behind black holes) has a surface temperature of \(30,000 \mathrm{K}\) and a visual luminosity \(100,000\) times that of our sun. Our sun radiates at the rate of \(3.86 \times 10^{26} \mathrm{W}\) . (Visual) luminosity is the total power radiated at visible wavelengths. (a) Assuming that this star behaves like an ideal blackbody, what is, the principal wavelength it radiates? Is this light visible? Use your answer to explain why these stars are blue. (b) If we assume that the power radiated by the star is also \(100,000\) times that of our sun, what is the radius of this star? Compare its size to that of our sun, which has a radius of \(6.96 \times 10^{5} \mathrm{km}\) . (c) Is it really correct to say, that the visual luminosity is proportional to the total power radiated? Explain.

An excited nucleus emits a gamma-ray photon with an energy of 2.45 \(\mathrm{MeV}\) . (a) What is the photon frequency?(b) What is the photon wavelength? (c) How does the wavelength compare with a typical nuclear diameter of \(10^{-14} \mathrm{m} ?\)

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