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An astronaut whose pulse frequency remains constant at 72 beats \( / \mathrm{min} \) is sent on a voyage. What would her pulse beat be, relative to Earth, when the ship is moving relative to Earth at (a) 0.10 c and (b) 0.90 c ? (Note: In this case, we are asking for the period, which is the time in the spaceship, 72 beats \( / \mathrm{min} \) is the frequency, the formula of period \( =1 / \mathrm{f} \) )

Ask by Ramirez Wheeler. in Canada
Mar 16,2025

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Answer

At 0.10c, the pulse rate is about 71.64 beats/min on Earth. At 0.90c, it's about 31.38 beats/min on Earth.

Solution

Let the astronaut’s proper pulse frequency be \[ f = 72\, \text{beats/min}. \] Thus, her proper period (time between beats) in the spaceship is \[ T = \frac{1}{f} = \frac{1}{72}\, \text{min/beat}. \] For an observer on Earth, time dilation must be taken into account. The time dilation factor is given by the Lorentz factor \[ \gamma = \frac{1}{\sqrt{1-\left(\frac{v}{c}\right)^2}}. \] In the Earth frame, the period of the astronaut’s pulse appears as \[ T' = \gamma T. \] The corresponding observed frequency is then \[ f' = \frac{1}{T'} = \frac{1}{\gamma T} = \frac{f}{\gamma}. \] We now consider the two cases: **(a) For \( v = 0.10c \):** First, calculate the Lorentz factor: \[ \gamma = \frac{1}{\sqrt{1-(0.10)^2}} = \frac{1}{\sqrt{1-0.01}} = \frac{1}{\sqrt{0.99}}. \] Approximating, \[ \sqrt{0.99} \approx 0.9950,\quad \text{so}\quad \gamma \approx 1.0050. \] Thus, the observed frequency is \[ f' = \frac{72}{1.0050} \approx 71.64\, \text{beats/min}. \] **(b) For \( v = 0.90c \):** First, calculate the Lorentz factor: \[ \gamma = \frac{1}{\sqrt{1-(0.90)^2}} = \frac{1}{\sqrt{1-0.81}} = \frac{1}{\sqrt{0.19}}. \] Approximating, \[ \sqrt{0.19} \approx 0.4359,\quad \text{so}\quad \gamma \approx 2.294. \] Thus, the observed frequency is \[ f' = \frac{72}{2.294} \approx 31.38\, \text{beats/min}. \] **Final Answers:** - (a) At \( v = 0.10c \), the pulse is observed to be about \( 71.64\, \text{beats/min} \) on Earth. - (b) At \( v = 0.90c \), the pulse is observed to be about \( 31.38\, \text{beats/min} \) on Earth.

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To find the pulse beat relative to Earth when the astronaut is moving at different speeds, we first need to calculate the period in the spaceship where the astronaut’s pulse frequency is 72 beats per minute. 1. The period \( T \) in the spaceship is given by: \[ T = \frac{1}{f} = \frac{1}{72/60} \approx 0.833 \text{ min} \] or about \( 50 \) seconds. 2. Now, when the astronaut is moving at relativistic speeds, time dilation needs to be considered. The time dilation factor \( \gamma \) is calculated using the formula: \[ \gamma = \frac{1}{\sqrt{1 - (v^2/c^2)}} \] For (a) \( v = 0.10c \): \[ \gamma = \frac{1}{\sqrt{1 - (0.10)^2}} \approx 1.005 \] The Earth observer would measure her pulse period as: \[ T' = \gamma T \approx 1.005 \times 50 \text{ seconds} \approx 50.25 \text{ seconds} \] For (b) \( v = 0.90c \): \[ \gamma = \frac{1}{\sqrt{1 - (0.90)^2}} \approx 2.294 \] The Earth observer would see the pulse period as: \[ T' = \gamma T \approx 2.294 \times 50 \text{ seconds} \approx 114.7 \text{ seconds} \] So, at (a) 0.10c, her pulse beats about every 50.25 seconds, and at (b) 0.90c, every 114.7 seconds, indicating that relativistic effects significantly impact the perception of time.

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