Why Does Density Increase When an Object Moves By?

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When an object moves past an observer, its density appears to increase due to Lorentz contraction, which reduces its volume while conserving mass. This phenomenon leads to a higher observed density in the moving reference frame compared to the object's rest frame. The density remains constant as the object approaches the observer, provided it is moving at a constant velocity. The relationship between the densities is quantitatively expressed using the Lorentz factor, gamma, which accounts for both volume contraction and energy transformation. Thus, the perceived increase in density is a result of relativistic effects on mass and volume as the object moves.
jgens
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When an object moves by you, I know that its density is supposed to increase (at least that's what I was told by my physics teacher); however, I don't understand why. I understand why the density is greater in a moving reference frame relative to an observer at rest, but why does it continue to increase as it moves by you?

Thanks.
 
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Your physics teacher is probably thinking that if a box of mass M and dimension x by y by z traveling in the z direction has its z dimension reduced by the Lorentz contraction. So the volume of the box has apparently shrunk. But mass is conserved.
 
I don't quite follow. I understand that the observer at rest would see the length of the box contract in its direction of motion, and that, assuming work was done on the box, the mass of the box appears to increase as well. However, I do not understand how the density continues to increase as the box approaches the observer.
 
If it approaches inertially then the density will be constant (but higher than the density in the rest frame).
 
That's what I thought. Perhaps that's what my teacher meant by density increasing as the block passes by you. Thanks.
 
As others have said, the mass-energy density rho' in the observer's frame is constant (if velocity is constant) and greater than the density rho as measured in a frame in which the stuff is at rest.

For completeness, I'll make things a bit quantitative, even though jgens does not need an answer at this level.

The two densities differ by two factors of gamma = 1/sqrt(1 - V^2 / c^2), roughly, one for Lorentz contraction and one for the transformation of energy between the two frames. Consequently,

rho' = rho/(1 - v^2 / c^2).

A more sophisticated way to look at it is that density is the zero-zero component of the stress-energy tensor, and there is a factor of gamma for each of the two indices.
 
MOVING CLOCKS In this section, we show that clocks moving at high speeds run slowly. We construct a clock, called a light clock, using a stick of proper lenght ##L_0##, and two mirrors. The two mirrors face each other, and a pulse of light bounces back and forth betweem them. Each time the light pulse strikes one of the mirrors, say the lower mirror, the clock is said to tick. Between successive ticks the light pulse travels a distance ##2L_0## in the proper reference of frame of the clock...

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