Problem 38
Question
A HeNe laser onboard a spaceship moving toward a remote space station emits a beam of red light toward the space station. The wavelength of the beam, as measured by a wavelength meter on board the spaceship, is \(632.8 \mathrm{nm}\). If the astronauts on the space station see the beam as a blue beam of light with a measured wavelength of \(514.5 \mathrm{nm},\) what is the relative speed of the spaceship with respect to the space station? What is the shift parameter \(z\) in this case?
Step-by-Step Solution
Verified Answer
Answer: The relative speed of the spaceship with respect to the space station is approximately \(1.881 * 10^8 ms^{-1}\), and the shift parameter \(z \approx -0.1869\).
1Step 1: Convert wavelengths to frequencies.
Using the formula \(c = \lambda f\), where \(c\) is the speed of light (\(3 * 10^8 ms^{-1}\)), \(\lambda\) is the wavelength, and \(f\) is the frequency, we can convert the given wavelengths to their corresponding frequencies. Let's calculate the emitted and observed frequencies.
Emitted wavelength (\(\lambda\)): \(632.8 nm\) = \(632.8 * 10^{-9} m\)
Emitted frequency (\(f\)): \(f = \frac{c}{\lambda} = \frac{3 * 10^8 ms^{-1}}{632.8 * 10^{-9} m} = 4.738 * 10^{14} Hz\)
Observed wavelength (\(\lambda'\)): \(514.5 nm\) = \(514.5 * 10^{-9} m\)
Observed frequency (\(f'\)): \(f' = \frac{c}{\lambda'} = \frac{3 * 10^8 ms^{-1}}{514.5 * 10^{-9} m} = 5.834 * 10^{14} Hz\)
2Step 2: Use the Doppler effect formula to find the relative velocity.
Now that we have the emitted and observed frequencies, we can use the Doppler effect formula to find the relative velocity of the spaceship with respect to the space station:
\(f' = \frac{f}{1+\frac{v}{c}}\)
Rearranging for \(v\): \(v = c (\frac{f}{f'} - 1)\)
Substitute the values of \(f, f', c\):
\(v = 3 * 10^8 ms^{-1} (\frac{4.738 * 10^{14} Hz}{5.834 * 10^{14} Hz} - 1)\)
\(v \approx -1.881 * 10^8 ms^{-1}\)
The negative sign indicates that the spaceship is moving towards the space station. Therefore, the relative speed of the spaceship with respect to the space station is approximately \(1.881 * 10^8 ms^{-1}\).
3Step 3: Compute the shift parameter \(z\).
Finally, we will compute the shift parameter \(z = \frac{\Delta\lambda}{\lambda}\), where \(\Delta\lambda = \lambda'-\lambda\).
\(\Delta\lambda = 514.5 nm - 632.8 nm = -118.3 nm\)
\(z = \frac{-118.3 nm}{632.8 nm} \approx -0.1869\)
The shift parameter \(z \approx -0.1869\).
Key Concepts
Relative VelocityWavelength ShiftFrequency Conversion
Relative Velocity
When we talk about relative velocity in the context of the Doppler Effect, we're referring to the speed at which an object is moving in relation to another. Here, it's the speed of the spaceship compared to the space station. The Doppler Effect in physics helps us understand how the frequency of a wave changes when the source and observer are in motion relative to each other.
In the exercise, we determined the relative speed by using the Doppler Effect formula:
In the exercise, we determined the relative speed by using the Doppler Effect formula:
- The emitted frequency of the laser light was calculated from the spaceship's perspective.
- The observed frequency was determined as the spaceship approached the space station.
- The change in frequency gives insight into the spaceship's speed compared to the space station.
Wavelength Shift
Wavelength shift happens when there is a change in the observed wavelength due to the relative motion of the source and the observer - a result of the Doppler Effect. For this problem, the red light emitted from the spaceship appeared blue to the astronauts on the space station.
Here's how it works:
The difference in wavelength, \(\Delta \lambda\), is computed by:\[\Delta \lambda = \lambda' - \lambda\]In our problem, this wavelength shift highlights the spaceship's quick approach towards the space station, evidenced by the shift towards the blue end of the spectrum.
Here's how it works:
- The original wavelength of the laser emitted from the spaceship was 632.8 nm.
- Upon reaching the space station, this wavelength was observed as 514.5 nm, a shorter wavelength associated with blue light.
The difference in wavelength, \(\Delta \lambda\), is computed by:\[\Delta \lambda = \lambda' - \lambda\]In our problem, this wavelength shift highlights the spaceship's quick approach towards the space station, evidenced by the shift towards the blue end of the spectrum.
Frequency Conversion
Frequency conversion is a critical step in resolving problems involving the Doppler Effect. To understand how waves change from one form (or frequency) to another, we use the speed of light equation:\(c = \lambda f\).
Here’s the breakdown:
Here’s the breakdown:
- Start with the emitted wavelength \(\lambda\) on the spaceship: 632.8 nm.
- Convert this into its frequency \(f\) by rearranging the formula, which gives us \(f = \frac{c}{\lambda}\).
- Next, take the observed wavelength\(\lambda'\) of 514.5 nm as seen by the station astronauts.
- Convert this to the observed frequency \(f'\) using the same formula: \(f' = \frac{c}{\lambda'}\).
Other exercises in this chapter
Problem 36
A meteor made of pure kryptonite (Yes, we know: There really isn't such a thing as kryptonite ...) is moving toward Earth. If the meteor eventually hits Earth,
View solution Problem 37
Radar-based speed detection works by sending an electromagnetic wave out from a source and examining the Doppler shift of the reflected wave. Suppose a wave of
View solution Problem 39
Sam sees two events as simultaneous: (i) Event \(A\) occurs at the point (0,0,0) at the instant 0: 00: 00 universal time; (ii) Event \(B\) occurs at the point \
View solution Problem 40
Use the relativistic velocity addition to reconfirm that the speed of light with respect to any inertial reference frame is \(c\). Assume one-dimensional motion
View solution