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To expose photographic film. photons of light dissociate silver bromide (AgBr) molecules. which requires an energy of \(1.2 \mathrm{eV}\). What limit does this impose on the wavelengths that may be recorded by photographic film?

Short Answer

Expert verified
The maximum wavelength of light that can be recorded by the photographic film is approximately 1031 nm.

Step by step solution

01

Convert Energy

Firstly, convert the energy from electronvolts to Joules using the conversion factor: \(1 \mathrm{eV} = 1.6 \times 10^{-19} \mathrm{J}\). Thus, the energy \(E = 1.2 \mathrm{eV} = 1.2 \times 1.6 \times 10^{-19} \mathrm{J}.\)
02

Apply Planck's Equation to find Wavelength

Planck's equation is given by E = hf = hc/λ. We're solving for λ, so rearranging gives us \(λ = \frac{hc}{E}\). Plug in all the known values: h (Planck's constant) = \(6.63 \times 10^{-34} \mathrm{m^2 kg / s}\), c (speed of light) = \(3 \times 10^8 \mathrm{m/s}\), E = \(1.2 \times 1.6 \times 10^{-19} \mathrm{J}\), and calculate Lambda.
03

Result

Calculate the wavelength λ. The result is the maximum wavelength of light that can be recorded by the photographic film. Please ensure the final answer is in nanometers for the commonly used wavelength unit in light-related problems.

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Key Concepts

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

Photon Energy
Photon energy is a fundamental concept when discussing light and its interaction with matter.
Photons are tiny packets of energy that travel at the speed of light. The energy of a photon is directly related to its frequency. The higher the frequency, the more energetic the photon is.
This relationship is crucial for understanding how light affects materials, such as in the case of photographic film where photons have enough energy to cause a chemical change.
  • Photon energy helps determine which wavelengths of light can trigger reactions.
  • Materials only respond to photons with sufficient energy to initiate changes.
Understanding photon energy is essential for applications ranging from capturing images to developing solar cells.
Planck's Equation
Planck's equation is used to calculate the energy of photons and is a vital tool in understanding light phenomena. The equation itself can be written as:
  • \[ E = hf \]
where:
  • \( E \) is the energy of the photon,
  • \( h \) is Planck's constant (\(6.63 \times 10^{-34} \mathrm{m^2 kg / s}\)), and
  • \( f \) is the frequency of the light.
In situations where frequency isn't directly given, you can use the speed of light (\( c \)) and wavelength (\( \lambda \)) to reformulate it as:
  • \[ E = \frac{hc}{\lambda} \]
This version of the equation is extremely helpful for finding either the wavelength or energy of light, which is crucial in materials sciences and quantum physics.
Planck's equation bridges the energy of photons with their measurable properties such as wavelength.
Light Wavelength
The wavelength of light is a key characteristic that determines its color and energy level.
It represents the distance between successive peaks of a light wave and is usually measured in nanometers (nm).
The electromagnetic spectrum covers a wide range of wavelengths, from the very short gamma rays to the long radio waves. Visible light is only a small portion, spanning approximately 400 nm to 700 nm.
  • Shorter wavelengths, like blue and violet light, carry more energy.
  • Longer wavelengths, like red light, have less energy.
When calculating the maximum wavelength that a photon can have to induce reactions, such as dissociating silver bromide in photographic film, understanding light wavelength becomes essential. This knowledge helps in various technological applications including photography and spectroscopy.
Silver Bromide Dissociation
Silver bromide (AgBr) is a chemical compound commonly used in photographic films due to its sensitivity to light.
When exposed to light, silver bromide undergoes a chemical change that is crucial for developing photographs.
Specifically, the energy from the photons dissociates the AgBr molecules, initiating a reaction that records the captured image.
  • The energy threshold for silver bromide dissociation is typically 1.2 electronvolts (eV).
  • Only photons with at least this amount of energy can cause dissociation.
This reaction is what allows light to be effectively recorded as an image on film. Understanding this process is essential for photography and related fields, where precise control over light exposure is crucial for capturing clear and vivid images.

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Most popular questions from this chapter

Show that the laws of momentum and enargy corservadion forbid the complete absorprion of a photon by a free electron. (Note: This is not the photoelectric effect In the pholoelectric effect, the electron is not free: the metal participates in momentum and eoergy onservation.)

A photon has the same momentum as an electron moving at \(10^{6} \mathrm{~m} / \mathrm{s}\). (a) Determine the photon's wavelength \(\mathrm{N}\). (b) What is the ratio of the kinetic energies of the two?

According to the energy-lime uncertainty principle. the lifetime \(\Delta f\) of a state and the uncertainty \(\Delta E\) in its energy are inversely proportional. Hydrogen's \(656 \mathrm{~nm}\) red spectral line is the result of an electron making a transition "downward" from a quantum state whose lifetime is about \(10^{-8} s\) (a) What inherent uncertainty in the energy of the emitted photon docs this imply? (Note: Unfortunately. we might use the symbol \(\Delta E\) for the energy difference - i.e., the energy of the photon - but here if means the uncertain in that energy difference.) (b) To what range in wavelengths does this correspond? (As noted in Exercise \(2.57\). the uncertainty principle is one contributor to the broadening of spectral lines.) (c) Obtain a general formula relating \(\Delta \lambda\) to \(\Delta t\).

A low-intensity beam of light is sent toward a narrow single slit. On the far side, individual flashes are seen sporadically at detectors over a broad area that is orders of magnitude wider than the slit width. What aspects of the experiment suggest a wave nature for light, and what aspects suggest a particle nature?

A function \(f(\alpha)\) is nonzero only in the region of width \(2 \delta\) centered at \(\alpha=0\) $$ f(\alpha)=\left\\{\begin{array}{ll} C & |\alpha| \leq \delta \\ 0 & |\alpha|>\delta \end{array}\right. $$ where \(C\) is a constant. (a) Find and plot versus \(\beta\) the Fourier transform \(A(\beta)\) of this function. (b) The function \(f \alpha\) ) might represent a pulse occupying either finite distance \((\alpha=\) position) or finite time \((\alpha\) = time). Comment on the wave number spectrum if \(\alpha\) is position and on the frequency spectrum if \(\alpha\) is time. Specifically address the dependence of the width of the spectrum on \(\delta\).

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