/*! 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 51 Thickness of Human Hair. Althoug... [FREE SOLUTION] | 91Ó°ÊÓ

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Thickness of Human Hair. Although we have discussed single-slit diffraction only for a slit, a similar result holds when light bends around a straight, thin object, such as a strand of hair. In that case, \(a\) is the width of the strand. From actual laboratory measurements on a human hair, it was found that when a beam of light of wavelength 632.8 \(\mathrm{nm}\) was shone on a single strand of hair, and the diffracted light was viewed on a screen 1.25 \(\mathrm{m}\) away, the first dark fringes on either side of the central bright spot were 5.22 \(\mathrm{cm}\) apart. How thick was this strand of hair?

Short Answer

Expert verified
The strand of hair is approximately 30.3 \(\mu\text{m}\) thick.

Step by step solution

01

Identify the Key Formula

The formula for single-slit diffraction is:\[ a \sin \theta = m \lambda \]where \( a \) is the width of the strand, \( \theta \) is the angle of the dark fringe, \( m \) is the order of the fringe, and \( \lambda \) is the wavelength. For the first dark fringe, \( m = 1 \).
02

Calculate the Angle \( \theta \)

We know that \( \tan \theta \approx \sin \theta \approx \theta \) for small angles, and \( \theta = \frac{x}{L} \), where \( x \) is half the total distance between the first dark fringes (\( 5.22 \ \text{cm} \)), and \( L \) is the distance to the screen. Thus, we have:\[ \theta = \frac{0.0522 \ \text{m}}{2 \times 1.25 \ \text{m}} = 0.02088 \]
03

Apply the Diffraction Formula

Substitute \( \theta \) and other known values into the diffraction formula:\[ a \times 0.02088 = 1 \times 632.8 \times 10^{-9} \ \text{m} \]Solve for \( a \):\[ a = \frac{632.8 \times 10^{-9}}{0.02088} \]
04

Calculate the Thickness of the Hair

Calculate the value from the above equation:\[ a \approx \frac{632.8 \times 10^{-9}}{0.02088} \approx 3.03 \times 10^{-5} \ \text{m} \]Thus, the thickness of the hair is approximately \( 30.3 \ \mu \text{m} \).

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Key Concepts

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

Understanding Wavelength
Wavelength is a crucial concept in physics, especially when discussing light and its interactions. It is defined as the distance between consecutive peaks of a wave, and is usually denoted by the symbol \( \lambda \). Wavelength is measured in meters (m), but in optics, it often appears in nanometers (nm), where 1 nm equals \( 10^{-9} \) meters. This small unit size makes it convenient for dealing with the tiny scales of light waves.

The wavelength of light determines its color. For example, the light used in the original exercise has a wavelength of 632.8 nm, which falls within the red part of the visible spectrum. When light waves encounter obstacles or openings comparable in size to their wavelength, diffraction occurs, resulting in various interference patterns.

Understanding the wavelength helps us predict how light behaves in different situations, such as passing through a slit or around obstacles like a human hair. This concept is essential when solving problems about diffraction and interference in physics.
Diffraction Formula in Action
Diffraction is a beautiful phenomenon that occurs when waves bend around the edges of an obstacle or through an opening. The diffraction formula can help predict this behavior. It is given by:\[ a \sin \theta = m \lambda \]where:
  • \( a \) is the width of the obstacle or slit,
  • \( \theta \) is the angle of the diffraction pattern,
  • \( m \) represents the order of the fringe,
  • \( \lambda \) is the wavelength of the light.
For the first order fringe, we use \( m = 1 \).

In this specific physics problem, the strand of hair acts as the slit, and light bends around it, creating dark and bright spots on a screen. By applying this formula, we can solve for\( a \), which represents the hair's thickness. Each variable plays a vital role in determining the diffraction pattern, making the formula an essential tool for both theoretical and practical investigations of light behavior.
Physics Problem Solving Approach
To solve physics problems effectively, such as determining the thickness of human hair using diffraction, a structured approach is crucial. Here's how to tackle these problems:

1. **Identify the Requisite Formula:** Recognize the core principle or formula relevant to the problem. In single-slit diffraction problems, it's the diffraction formula \( a \sin \theta = m \lambda \).

2. **Break Down the Problem:** Understand what each term in the formula represents and how the known values relate to the scenario, like light wavelength or distance to the screen.

3. **Simplify Assumptions:** For small angles, it is reasonable to use approximations such as \( \tan \theta \approx \sin \theta \approx \theta \). This simplifies calculations and helps solve for unknowns.

4. **Calculate with Precision:** Ensure all measurements are accurate, such as distances and angles, as in the example using \( \theta = \frac{x}{L} \).

5. **Double-Check Results:** Once you've computed the needed variable, revisit your values and assumptions to ensure accuracy.

Being methodical in problem-solving can yield clear insights and accurate results, making even complex physics problems manageable.
Mastering Angle Calculation
Calculating angles in diffraction problems often involves understanding small angle approximations. In these cases, when the angle \( \theta \) is small, \( \tan \theta \) and \( \sin \theta \) can be approximated as \( \theta \) (in radians). This simplifies mathematical processes.

In the exercise, angle calculation involved measuring the distance between dark fringes (5.22 cm), which required finding half this distance (0.0522 m/2) to determine \( x \). The angle \( \theta \) was then calculated using \( \theta = \frac{x}{L} \) where \( L \) is the distance between the screen and the hair (1.25 m).

These steps ensure precision since a slight error in angle measurement can lead to incorrect deductions about how light diffracts and bends. By practicing precise angle calculations, you can enhance your ability to predict interference patterns. Whether you're a student or a seasoned scientist, mastering angle calculations is integral to understanding wave behavior in physics.

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Most popular questions from this chapter

Intensity Pattern of \(N\) Slits. (a) Consider an arrangement of \(N\) slits with a distance \(d\) between adjacent slits. The slits emit coherently and in phase at wavelength \(\lambda .\) Show that at a time \(t,\) the electric field at a distant point \(P\) is $$\begin{aligned} E_{P}(t)=& E_{0} \cos (k R-\omega t)+E_{0} \cos (k R-\omega t+\phi) \\\ &+E_{0} \cos (k R-\omega t+2 \phi)+\cdots \\ &+E_{0} \cos (k R-\omega t+(N-1) \phi) \end{aligned}$$ where \(E_{0}\) is the amplitude at \(P\) of the electric field due to an indi- vidual slit, \(\phi=(2 \pi d \sin \theta) / \lambda, \theta\) is the angle of the rays reaching \(P\) (as measured from the perpendicular bisector of the slit arrange- ment), and \(R\) is the distance from \(P\) to the most distant slit. In this problem, assume that \(R\) is much larger than \(d\) . (b) To carry out the sum in part (a), it is convenient to use the complex-number relationship $$e^{i z}=\cos z+i \sin z$$ where \(i=\sqrt{-1}\) . In this expression, cos \(z\) is the real part of the complex number \(e^{i z},\) and \(\sin z\) is its imaginary part. Show that the electric field \(E_{P}(t)\) is equal to the real part of the complex quantity $$\sum_{n=0}^{N-1} E_{0} e^{i(k R-\omega t+n \phi)}$$ (c) Using the properties of the exponential function that \(e^{A} e^{B}=e^{(A+B)}\) and \(\left(e^{A}\right)^{n}=e^{n A},\) show that the sum in part (b) can be written as $$E_{0}\left(\frac{e^{i N \phi}-1}{e^{i \phi}-1}\right) e^{i(k R-\omega t)}\( \)\quad=E_{0}\left(\frac{e^{i N \phi / 2}-e^{-i N \phi / 2}}{e^{i \phi / 2}-e^{-i \phi / 2}}\right) e^{i[k R-\omega t+(N-1) \phi}$$ Then, using the relationship \(e^{i z}=\cos z+i \sin z,\) show that the (real) electric field at point \(P\) is $$I=I_{0}\left[\frac{\sin (N \phi / 2)}{\sin (\phi / 2)}\right]^{2}$$ where \(I_{0}\) is the maximum intensity for an individual slit. (e) Check the result in part (d) for the case \(N=2 .\) It will help to recall that \(\sin 2 A=2 \sin A \cos A .\) Explain why your result differs from Eq. \((35.10),\) the expression for the intensity in two-source interfer- ence, by a factor of \(4 .\) Hint: Is \(I_{0}\) defined in the same way in both expressions?

A glass sheet is covered by a very thin opaque coating. In the middle of this sheet there is a thin scratch 0.00125 \(\mathrm{mm}\) thick. The sheet is totally immersed beneath the surface of a liquid. Parallel rays of monochromatic coherent light with wavelength 612 \(\mathrm{nm}\) in air strike the sheet perpendicular to its surface and pass through the scratch. A screen is placed in the liquid a distance of 30.0 \(\mathrm{cm}\) away from the sheet and parallel to it. You observe that the first dark fringes on either side of the central bright fringe on the screen are 22.4 \(\mathrm{cm}\) apart. What is the refractive index of the liquid?

A diffraction grating has 650 slits/mm. What is the highest order that contains the entire visible spectrum? (The wavelength range of the visible spectrum is approximately \(380-750 \mathrm{nm.}\) )

If a diffraction grating produces its third-order bright band at an angle of \(78.4^{\circ}\) for light of wavelength \(681 \mathrm{nm},\) find (a) the number of slits per centimeter for the grating and (b) the angular location of the first-order and second-order bright bands. (c) Will there be a fourth-order bright band? Explain.

The light from an iron arc includes many different wavelengths. Two of these are at \(\lambda=587.9782 \mathrm{nm}\) and \(\lambda=\) 587.8002 \(\mathrm{nm} .\) You wish to resolve these spectral lines in first order using a grating 1.20 \(\mathrm{cm}\) in length. What minimum number of slits per centimeter must the grating have?

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