Chapter 7: Problem 4
Some radioactive particles are traveling at \(0.999 c .\) If their lifetime is \(10^{-20}\) s when they are at rest, what is their lifetime at this speed? How far do they travel in that time (as viewed in the frame at which they are moving at \(0.999 c ?\)
Short Answer
Expert verified
The lifetime is approximately \(2.24 \times 10^{-19}\) s, and the distance traveled is \(6.72 \times 10^{-11}\) m.
Step by step solution
01
- Understand the Relativistic Time Dilation Formula
Time dilation in special relativity is given by the formula: \[ t = \frac{t_0}{\sqrt{1 - \left(\frac{v}{c}\right)^2}} \] where \( t \) is the dilated time, \( t_0 \) is the proper time, \( v \) is the velocity, and \( c \) is the speed of light.
02
- Plug in Given Values
Given that the rest lifetime (proper time) \( t_0 \) is \( 10^{-20} \) s and the velocity \( v \) is \( 0.999 c \), substitute these into the time dilation formula: \[ t = \frac{10^{-20}}{\sqrt{1 - (0.999)^2}} \]
03
- Calculate the Time Dilation Factor
First, calculate the factor under the square root: \[ 1 - (0.999)^2 = 1 - 0.998001 = 0.001999 \] Now find the square root: \[ \sqrt{0.001999} \approx 0.0447 \]
04
- Compute the Dilated Lifetime
Substitute \( \sqrt{0.001999} \) into the time dilation formula: \[ t = \frac{10^{-20}}{0.0447} \approx 2.24 \times 10^{-19} \text{ s} \]
05
- Calculate the Distance Traveled
The distance traveled in the observer's frame is given by: \[ d = v \times t \] Substitute \( v = 0.999 c \) and \( t \approx 2.24 \times 10^{-19} \) s: \[ d = 0.999 c \times 2.24 \times 10^{-19} = 2.24 \times 10^{-19} c \]
06
- Finalize Calculation of Distance
Since \( c \approx 3 \times 10^8 \) m/s, \[ d = 2.24 \times 10^{-19} \times 3 \times 10^8 \text{ m} = 6.72 \times 10^{-11} \text{ m} \]
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
time dilation formula
Time dilation is a phenomenon predicted by Einstein's theory of Special Relativity. It describes how time can appear to slow down for an object moving at high speeds relative to an observer. The equation used to calculate this is:
\[ t = \frac{t_0}{\sqrt{1 - \left(\frac{v}{c}\right)^2}} \] where:
When the velocity \( v \) of an object approaches the speed of light \( c \), the term \(\sqrt{1 - (v/c)^2}\) becomes very small. This causes the dilated time \( t \) to increase significantly. This effect is incredibly pronounced at speeds close to the speed of light, where even small increases in velocity lead to substantial time dilation.
\[ t = \frac{t_0}{\sqrt{1 - \left(\frac{v}{c}\right)^2}} \] where:
- \( t \) is the dilated time experienced by the moving object.
- \( t_0 \) is the proper time, the time experienced by the object at rest.
- \( v \) is the velocity of the moving object.
- \( c \) is the speed of light (approximately \(3\times10^8 \) meters per second).
When the velocity \( v \) of an object approaches the speed of light \( c \), the term \(\sqrt{1 - (v/c)^2}\) becomes very small. This causes the dilated time \( t \) to increase significantly. This effect is incredibly pronounced at speeds close to the speed of light, where even small increases in velocity lead to substantial time dilation.
proper time
Proper time, denoted by \( t_0 \), is the time interval measured by a clock that is at rest relative to the observer. In other words, it is the time experienced directly by an object or system. For example, if you are sitting at rest, the time you experience is your proper time.
In the context of the given exercise:
This forms the basis for calculating how their perceived lifetime changes when they move at high speeds. Proper time is always the shortest time interval between two events as measured in the frame of reference in which the events occur at the same location.
In the context of the given exercise:
- The proper time \( t_0 \) for the radioactive particles at rest is given as \(10^{-20}\) seconds.
This forms the basis for calculating how their perceived lifetime changes when they move at high speeds. Proper time is always the shortest time interval between two events as measured in the frame of reference in which the events occur at the same location.
speed of light
The speed of light, denoted by \( c \), is a fundamental constant in physics. It is approximately \(3 \times 10^8\) meters per second (\(m/s\)). It is essential in the study of relativity as it represents the maximum speed at which information or matter can travel.
In the formula for time dilation, \( c \) acts as a benchmark to compare the object's speed \( v \) against. When the object’s speed \( v \) approaches \( c \), time dilation effects become very significant.
A notable property of the speed of light is its invariance; it remains constant in all frames of reference, regardless of the observer's relative motion. This unique characteristic is a cornerstone of Einstein’s Special Relativity.
In the formula for time dilation, \( c \) acts as a benchmark to compare the object's speed \( v \) against. When the object’s speed \( v \) approaches \( c \), time dilation effects become very significant.
- For particles moving at \(0.999c\), the dilated time is computed using this constant.
A notable property of the speed of light is its invariance; it remains constant in all frames of reference, regardless of the observer's relative motion. This unique characteristic is a cornerstone of Einstein’s Special Relativity.
distance traveled in relativistic frame
In a relativistic frame, the distance traveled by an object moving at high speeds can be calculated by considering both its velocity and the dilated time experienced by that object.
Given in the exercise:
The distance \( d \) traveled in the observer's frame can be calculated using the formula:
\[ d = v \times t \]
So, plugging in the known values:
\[ d = 0.999 c \times 2.24 \times 10^{-19} \approx 6.72 \times 10^{-11} \text{ meters} \]
This distance is the actual path length observed in the frame where the particles are moving at high speed. It vividly illustrates how even tiny time dilations can result in significant distances traveled for objects moving near the speed of light.
Given in the exercise:
- Velocity \( v = 0.999c \)
- Dilated time \( t \approx 2.24 \times 10^{-19} \) seconds
The distance \( d \) traveled in the observer's frame can be calculated using the formula:
\[ d = v \times t \]
So, plugging in the known values:
\[ d = 0.999 c \times 2.24 \times 10^{-19} \approx 6.72 \times 10^{-11} \text{ meters} \]
This distance is the actual path length observed in the frame where the particles are moving at high speed. It vividly illustrates how even tiny time dilations can result in significant distances traveled for objects moving near the speed of light.