Chapter 15: Problem 47
Consider the tale of the physicist who is ticketed for running a red light and argues that because he was approaching the intersection, the red light was Doppler shifted and appeared green. How fast would he have to have been going? \(\left(\lambda_{\text {red }} \approx 650 \mathrm{nm} \text { and } \lambda_{\text {green }} \approx 530 \mathrm{nm} .\right)\)
Short Answer
Step by step solution
Understand the Doppler Effect
Express the Relativistic Doppler Shift Equation
Substitute Known Values into the Equation
Isolate the Relativistic Factor \( \beta \)
Solve for \( \beta \)
Calculate Speed \( v \)
Conclusion
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Relativistic Doppler Shift
When either the observer or the source is moving at a speed close to the speed of light, we use the relativistic Doppler shift formula to calculate the observed changes in wavelength.
This phenomenon can occur with all waves, but it is often associated with light waves and has important implications in fields like astrophysics and cosmology. In this particular scenario, a physicist claims that a red light appeared green due to this effect while moving towards the light source. In other words, due to the motion, the observed wavelength differs from the emitted wavelength. This happens because the light waves bunch up if the observer (or source) is moving toward the other, resulting in a shift to shorter wavelengths.
Wavelength Change
When an object moves towards a source of light, the wavelengths become shorter, causing a shift towards the blue end of the spectrum (blue-shift).
Conversely, when an object moves away, wavelengths lengthen, resulting in a red-shift.For the physicist to perceive the red light as green, the wavelength of the perceived light must match that of green light, which in this case, is shorter than the original red wavelength.
This requires calculating the observed wavelength using the relativistic Doppler shift equation, \[ \lambda_{o} = \lambda_{s} \sqrt{\frac{1 + \beta}{1 - \beta}}. \]Here, \( \lambda_{o} \) is the green light's wavelength \( 530 \, \text{nm} \), and \( \lambda_{s} \) is the red light's wavelength \( 650 \, \text{nm} \).
Consequently, the change from red to green light is a shift to shorter wavelengths.
Light Waves
Light waves are electromagnetic waves that travel through a vacuum at a constant speed, known as the speed of light.
These waves possess different wavelengths corresponding to various colors in the visible spectrum, ranging from reds with longer wavelengths to blues and purples with shorter wavelengths. In the scenario involving the physicist, the red light with a wavelength of approximately 650 nanometers appears green at about 530 nanometers.
This transformation occurs as the physicist moves towards the light source, resulting in a compression of the light waves in the direction of movement.
This compression changes the wavelength and alters the color perceived by the observer due to the Doppler Effect.
Speed of Light
It is crucial in the calculation of the relativistic Doppler shift.In the given problem, the speed of light comes into play when calculating how fast the physicist must travel to cause the requested wavelength change.
The formula used involves the term \( \beta = \frac{v}{c} \) where \( v \) is the velocity of the observer relative to the speed of light.
Understanding this relationship is vital for comprehending how velocity affects wave perception.To make the red light appear green, the physicist would need to travel at a high fraction of the speed of light, illustrating the extreme velocities required for significant relativistic wavelength transformation.
Such speeds are typically beyond the capacity of everyday travel, underscoring the impossibility of achieving this color change with current technology.