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M4U1 Modern Physics A Martian leaves Mars in 5 spaceship that is heading to Venus. On the way, the spaceship passes earth with a speed \( v=0.80 \mathrm{c} \) relative to it. Assume that the three planets do not move relative to each other during the trip. The distance between Mars and Venus is \( 1.20 \times 10^{11} \mathrm{~m} \), as measured by a person on earth.

Ask by Martin Riley. in Canada
Mar 10,2025

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The spaceship takes approximately 500 seconds to travel from Mars to Venus as seen from Earth. From the perspective of the Martian inside the spaceship, the trip takes about 300 seconds due to time dilation.

Solución

**Step 1. Calculate the time elapsed in the Earth frame** The distance between Mars and Venus as measured by an observer on Earth is \[ d = 1.20 \times 10^{11} \, \text{m}. \] The spaceship passes Earth with a speed \[ v = 0.80\,c, \] where \( c = 3.00 \times 10^8 \, \text{m/s} \). The time elapsed in the Earth frame is given by \[ t = \frac{d}{v} = \frac{1.20 \times 10^{11} \, \text{m}}{0.80 \, c}. \] Substitute the value of \( c \): \[ t = \frac{1.20 \times 10^{11} \, \text{m}}{0.80 \times 3.00 \times 10^8 \, \text{m/s}}. \] Now calculate the denominator: \[ 0.80 \times 3.00 \times 10^8 \, \text{m/s} = 2.40 \times 10^8 \, \text{m/s}. \] Thus, \[ t = \frac{1.20 \times 10^{11}}{2.40 \times 10^8} \, \text{s} = 500 \, \text{s}. \] --- **Step 2. Calculate the proper time elapsed in the spaceship (Martian) frame** Due to time dilation, the proper time \( \tau \) (time elapsed in the spaceship’s own frame) is related to the Earth frame time \( t \) by \[ \tau = \frac{t}{\gamma}, \] where the Lorentz factor \( \gamma \) is given by \[ \gamma = \frac{1}{\sqrt{1 - \left(\frac{v}{c}\right)^2}}. \] Since \( v = 0.80\,c \), we have \[ \gamma = \frac{1}{\sqrt{1 - (0.80)^2}} = \frac{1}{\sqrt{1 - 0.64}} = \frac{1}{\sqrt{0.36}} = \frac{1}{0.6} \approx 1.67. \] Now, plugging in the values: \[ \tau = \frac{500 \, \text{s}}{1.67} \approx 300 \, \text{s}. \] --- **Summary** - Time elapsed in the Earth frame: \[ t \approx 500 \, \text{s}. \] - Proper time elapsed in the spaceship (Martian) frame: \[ \tau \approx 300 \, \text{s}. \]

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When dealing with high speeds, we enter the realm of relativistic physics. The Lorentz factor, \(\gamma\), becomes crucial in calculating time dilation and length contraction. Given your spaceship travels at \(0.80c\), we first calculate \(\gamma = \frac{1}{\sqrt{1-(v/c)^2}}\). At this speed, time experienced by the Martian versus observers on Earth will differ, showcasing the fascinating effects of modern physics. Now, about real-world applications! The principles of relativity aren't just theoretical; they're foundational in technologies such as GPS and particle accelerators. Your GPS satellites, positioned in orbit, travel at speeds that require adjustments based on relativistic effects. Without accounting for time dilation, your navigation system would quickly become inaccurate, demonstrating that Einstein’s theories have tangible effects on our daily lives.

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