:D
The proper title of this post should be: How to induce relativistic effects in a stationary object.
I will be the first to admit the impracticality of this approach. However, I found it interesting enough to post.
Consider a mass m oscillating at frequency w and amplitude A. The oscillation is described simply by:
x = A sin(wt)
v = Aw cos(wt)
a = -Aw^2 sin(wt) = -w^2 x
F = ma = -mxw^2
U = kinetic energy = .5 mv^2 = .5 mA^2 w^2 cos^2(wt)
E = potential energy = -[integral] F dx = -(-mw^2 [integral] x dx) = -(-.5 mw^2 x^2) = .5 m w^2 A^2 sin^2(wt)
Etot = total energy = E + U = .5 m w^2 A^2(sin^2(wt) + cos^2(wt)) = .5 m w^2 A^2
vavg = average velocity
Etot = .5 m vavg^2
vavg = sqr(2 Etot / m) = sqr(2(.5)m w^2 A^2 / m) = wA
m*avg = average relativistic mass = m0 / sqr(1 - (v/c)^2) = m0 / sqr(1 - (wA/c)^2)
Thus, by vibrating or oscillating an object, its mass should increase slightly, and there should be minute time dilation effects. However, in practice, it would probably be too small to measure.
The proper title of this post should be: How to induce relativistic effects in a stationary object.
I will be the first to admit the impracticality of this approach. However, I found it interesting enough to post.
Consider a mass m oscillating at frequency w and amplitude A. The oscillation is described simply by:
x = A sin(wt)
v = Aw cos(wt)
a = -Aw^2 sin(wt) = -w^2 x
F = ma = -mxw^2
U = kinetic energy = .5 mv^2 = .5 mA^2 w^2 cos^2(wt)
E = potential energy = -[integral] F dx = -(-mw^2 [integral] x dx) = -(-.5 mw^2 x^2) = .5 m w^2 A^2 sin^2(wt)
Etot = total energy = E + U = .5 m w^2 A^2(sin^2(wt) + cos^2(wt)) = .5 m w^2 A^2
vavg = average velocity
Etot = .5 m vavg^2
vavg = sqr(2 Etot / m) = sqr(2(.5)m w^2 A^2 / m) = wA
m*avg = average relativistic mass = m0 / sqr(1 - (v/c)^2) = m0 / sqr(1 - (wA/c)^2)
Thus, by vibrating or oscillating an object, its mass should increase slightly, and there should be minute time dilation effects. However, in practice, it would probably be too small to measure.