Problem 20
Question
Coherent sources \(A\) and \(B\) emit electromagnetic waves with wavelength 2.00 \(\mathrm{cm} .\) Point \(P\) is 4.86 \(\mathrm{m}\) from \(A\) and 5.24 \(\mathrm{m}\) from B. What is the phase difference at \(P\) between these two waves?
Step-by-Step Solution
Verified Answer
The phase difference at point P is 0 radians.
1Step 1: Calculate the Path Difference
The path difference between the two sources at point \(P\) is given by the distance from \(B\) to \(P\) minus the distance from \(A\) to \(P\). Therefore, the path difference \(\Delta d\) is \(5.24 \, \text{m} - 4.86 \, \text{m} = 0.38 \, \text{m}\).
2Step 2: Relate Path Difference to Wavelength
The relationship between the path difference \(\Delta d\) and the wavelength \(\lambda\) is found by dividing the path difference by the wavelength. So, \( \frac{\Delta d}{\lambda} = \frac{0.38 \, \text{m}}{0.02 \, \text{m}} = 19\). This means the path difference is 19 wavelengths.
3Step 3: Calculate the Phase Difference
Now that we know the path difference in terms of the number of wavelengths, we can calculate the phase difference using the formula \( \Delta \phi = 2\pi \times \frac{\Delta d}{\lambda}\). Therefore, \(\Delta \phi = 2\pi \times 19 = 38\pi\, \text{radians}\). Since phase difference is usually expressed within a range of \(0\) to \(2\pi\), we need to use modulo operation: \(38\pi \mod 2\pi = 0\).
Key Concepts
Coherent SourcesPath DifferencePhase DifferenceElectromagnetic Waves
Coherent Sources
Coherent sources are crucial in understanding wave interference. They are sources that emit waves with a constant phase difference and the same frequency. This means the waves are synchronized over time, maintaining a consistent phase relationship.
In practical terms, coherent sources produce wave patterns that can either constructively or destructively interfere. Constructive interference occurs when the phase difference is a multiple of \(2\pi\), leading to amplified waves. Destructive interference happens at odd multiples of \(\pi\), causing the waves to cancel each other out.
In practical terms, coherent sources produce wave patterns that can either constructively or destructively interfere. Constructive interference occurs when the phase difference is a multiple of \(2\pi\), leading to amplified waves. Destructive interference happens at odd multiples of \(\pi\), causing the waves to cancel each other out.
- Synchronized wave emission
- Same frequency
- Constant phase difference
Path Difference
Path difference refers to the difference in lengths between the paths taken by two waves from their sources to a specific point. The calculation of path difference is foundational in determining how waves will interfere at a given location.
In the exercise, the path difference \(\Delta d\) was found by subtracting the distance from source \(A\) to point \(P\) from the distance from source \(B\) to point \(P\). The calculation of path difference is given by:
\[\Delta d = 5.24 \, \text{m} - 4.86 \, \text{m} = 0.38 \, \text{m}\]
In the exercise, the path difference \(\Delta d\) was found by subtracting the distance from source \(A\) to point \(P\) from the distance from source \(B\) to point \(P\). The calculation of path difference is given by:
\[\Delta d = 5.24 \, \text{m} - 4.86 \, \text{m} = 0.38 \, \text{m}\]
- Relates directly to constructive or destructive interference
- Measured in meters
- Essential for calculating phase difference
Phase Difference
Phase difference is a measure of how "in-step" or "out-of-step" two waves are, relative to each other. It's typically expressed in radians or degrees. In the context of wave interference, the phase difference determines whether waves will constructively or destructively interfere.
For the exercise, using the determined path difference and wavelength, the phase difference \(\Delta \phi\) is calculated by:
\[\Delta \phi = 2\pi \times \frac{\Delta d}{\lambda}\ = 2\pi \times 19 = 38\pi\, \text{radians}\]
Phase difference influences wave behavior greatly:
For the exercise, using the determined path difference and wavelength, the phase difference \(\Delta \phi\) is calculated by:
\[\Delta \phi = 2\pi \times \frac{\Delta d}{\lambda}\ = 2\pi \times 19 = 38\pi\, \text{radians}\]
Phase difference influences wave behavior greatly:
- Constructive interference if \((\Delta \phi\) is multiple of \(2\pi\))
- Destructive interference if \((\Delta \phi\) is odd multiple of \(\pi\))
Electromagnetic Waves
Electromagnetic waves are waves that propagate through the electromagnetic field, which encompasses electric and magnetic components. These waves travel at the speed of light in a vacuum and are fundamental to our understanding of classical and quantum physics.
Electromagnetic waves include visible light, radio waves, microwaves, and more. Each type of wave is characterized by its wavelength and frequency. In our exercise, we dealt with electromagnetic waves having a wavelength of 2.00 cm.
Electromagnetic waves include visible light, radio waves, microwaves, and more. Each type of wave is characterized by its wavelength and frequency. In our exercise, we dealt with electromagnetic waves having a wavelength of 2.00 cm.
- Consists of oscillating electric and magnetic fields
- Propagates through vacuum at speed of light \((c = 3 \times 10^8\, \text{m/s})\)
- Encompasses a broad spectrum from gamma rays to radio waves
Other exercises in this chapter
Problem 18
Coherent light of frequency \(6.32 \times 10^{14} \mathrm{Hz}\) passes through two thin slits and falls on a screen 85.0 \(\mathrm{cm}\) away. You observe that
View solution Problem 19
In a two-slit interference pattern, the intensity at the peak of the central maximum is \(I_{0}\) . (a) At a point in the pattern where the phase difference bet
View solution Problem 21
Coherent light with wavelength 500 nm passes through narrow slits separated by 0.340 \(\mathrm{mm} .\) At a distance from the slits large compared to their sepa
View solution Problem 22
Two slits spaced 0.260 \(\mathrm{mm}\) apart are placed 0.700 \(\mathrm{m}\) from a screen and illuminated by coherent light with a wavelength of 660 nm. The in
View solution