Let's examine whether or not the law of conservation of momentum is true in all reference frames if we use the Newtonian definition of momentum: px = mux. Consider an object A of mass 3m at rest in reference frame S. Object A explodes into two pieces: object B, of mass m, that is shot to the left at a speed of c/2 and object C, of mass 2m, that, to conserve momentum, is shot to the right at a speed of c/4. Suppose this explosion is observed in reference frame S' that is moving to the right at half the speed of light. Use the Lorentz velocity transformation to find the velocities and the Newtonian momenta of B and C in S'.
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35. Special Relativity
Lorentz Transformations
Problem 37.15
Textbook Question
An observer in frame S′ is moving to the right (+x-direction) at speed u = 0.600c away from a stationary observer in frame S. The observer in S′ measures the speed v′ of a particle moving to the right away from her. What speed v does the observer in S measure for the particle if (a) v′ = 0.400c; (b) v′ = 0.900c; (c) v′ = 0.990c?

1
Step 1: Recognize that this problem involves relativistic velocity addition. The formula for relativistic velocity transformation is: , where is the velocity of the particle as measured in frame S′, is the relative velocity between frames S and S′, and is the speed of light.
Step 2: Substitute the given values into the formula. For all parts of the problem, is given as . For part (a), is . For part (b), is . For part (c), is . Plug these values into the formula one at a time.
Step 3: Simplify the numerator of the formula for each case. For example, in part (a), the numerator becomes , which simplifies to . Repeat this process for parts (b) and (c).
Step 4: Simplify the denominator of the formula for each case. For part (a), the denominator becomes , which simplifies to . Repeat this process for parts (b) and (c).
Step 5: Divide the simplified numerator by the simplified denominator for each case to find the speed as measured by the observer in frame S. This step completes the calculation for each part of the problem.

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Key Concepts
Here are the essential concepts you must grasp in order to answer the question correctly.
Relativity of Velocity
In the framework of special relativity, the velocity of an object as measured in different inertial frames is not simply additive. Instead, the relativistic velocity addition formula must be used, which accounts for the effects of time dilation and length contraction at speeds close to the speed of light. This formula ensures that the resultant speed never exceeds the speed of light, c.
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Lorentz Transformation
The Lorentz transformation equations relate the space and time coordinates of events as observed in different inertial frames moving relative to each other at a constant velocity. These transformations are essential for converting measurements from one frame to another, particularly when dealing with high velocities, and they incorporate the effects of time dilation and length contraction.
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Lorentz Transformations of Velocity
Speed of Light as a Cosmic Speed Limit
According to Einstein's theory of relativity, the speed of light in a vacuum is the ultimate speed limit in the universe, denoted as c. No object with mass can reach or exceed this speed. This principle is fundamental in understanding how velocities combine in relativistic contexts, ensuring that the calculated speeds remain below c, regardless of the relative motion of observers.
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Speed Distribution & Special Speeds of Ideal Gases
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