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Ch 37: Special Relativity
Young & Freedman Calc - University Physics 14th Edition
Young & Freedman Calc14th EditionUniversity PhysicsISBN: 9780321973610Non è quello che usi tu?Cambia libro di testo
Capitolo 37, Problema 29b

A force is applied to a particle along its direction of motion. At what speed is the magnitude of force required to produce a given acceleration twice as great as the force required to produce the same acceleration when the particle is at rest? Express your answer in terms of the speed of light.

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Start by recalling the relativistic expression for force: \( F = \frac{dp}{dt} \), where \( p \) is the relativistic momentum given by \( p = \frac{mv}{\sqrt{1 - \frac{v^2}{c^2}}} \). Here, \( m \) is the rest mass of the particle, \( v \) is its velocity, and \( c \) is the speed of light.
For a given acceleration \( a \), the force can be expressed as \( F = \frac{d}{dt} \left( \frac{mv}{\sqrt{1 - \frac{v^2}{c^2}}} \right) \). However, for simplicity, we can use the effective mass concept: \( F = ma_{\text{eff}} \), where \( a_{\text{eff}} = \frac{a}{(1 - \frac{v^2}{c^2})^{3/2}} \).
At rest (\( v = 0 \)), the force required to produce the acceleration \( a \) is \( F_0 = ma \), since \( (1 - \frac{v^2}{c^2})^{3/2} = 1 \).
When the particle is moving at a velocity \( v \), the force required becomes \( F_v = \frac{ma}{(1 - \frac{v^2}{c^2})^{3/2}} \). The problem states that \( F_v = 2F_0 \), so substitute \( F_0 = ma \) into this equation: \( \frac{ma}{(1 - \frac{v^2}{c^2})^{3/2}} = 2ma \).
Simplify the equation to solve for \( v \): \( \frac{1}{(1 - \frac{v^2}{c^2})^{3/2}} = 2 \). Raise both sides to the power of \( -2/3 \) to isolate \( 1 - \frac{v^2}{c^2} \), and then solve for \( v \) in terms of \( c \).

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Newton's Second Law states that the force acting on an object is equal to the mass of that object multiplied by its acceleration (F = ma). This principle is fundamental in understanding how forces affect the motion of particles, particularly in determining the relationship between force, mass, and acceleration in both stationary and moving states.
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As an object's speed approaches the speed of light, relativistic effects become significant, altering the relationship between mass, force, and acceleration. Specifically, the effective mass of an object increases with speed, which means that more force is required to achieve the same acceleration as the object moves faster, a concept crucial for understanding the problem at hand.
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