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A cop pulls you over and asks what speed you were going. “Well, officer, I cannot tell a lie: the speedometer read 4×108m/s.” He gives you a ticket, because the speed limit on this highway is 2.5×108m/s . In court, your lawyer (who, luckily, has studied physics) points out that a car’s speedometer measures proper velocity, whereas the speed limit is ordinary velocity. Guilty, or innocent?

Short Answer

Expert verified

The driver is innocent.

Step by step solution

01

Expression for the relationship between proper velocity and ordinary velocity:

Write the relationship between proper and ordinary velocity.

u=11-η2c2η …… (1)

Here, ηis the proper velocity, u is the ordinary velocity, and c is the speed of light.

02

Determine that the driver is guilty or innocent:

Substitute 4×108m/sforη and3×108m/s forc in equation (1).

u-11-4×108m/s23×108m/s24×108m/su-0.6×4×102m/su-2.4×108m/s

As the ordinary velocity is less than the speed light u<s, the driver maintained his car’s speed, and hence lawyer proved him innocent.

Therefore, the driver is innocent.

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Most popular questions from this chapter

(a) Construct a tensor Dμυ(analogous to Fμυ) out of Dand H. Use it to express Maxwell's equations inside matter in terms of the free current density Jfμ.

(b) Construct the dual tensor Hμυ(analogous to Gμυ)

(c) Minkowski proposed the relativistic constitutive relations for linear media:

Dμυηυ=c2εFμυηυ andHμυηυ=1μGμυηυ

Where εis the proper permittivity, μis the proper permeability, andηυ is the 4-velocity of the material. Show that Minkowski's formulas reproduce Eqs. 4.32 and 6.31, when the material is at rest.

(d) Work out the formulas relating D and H to E and B for a medium moving with (ordinary) velocity u.

In the past, most experiments in particle physics involved stationary targets: one particle (usually a proton or an electron) was accelerated to a high energy E, and collided with a target particle at rest (Fig. 12.29a). Far higher relative energies are obtainable (with the same accelerator) if you accelerate both particles to energy E, and fire them at each other (Fig. 12.29b). Classically, the energy E¯of one particle, relative to the other, is just 4E(why?) . . . not much of a gain (only a factor of 4). But relativistically the gain can be enormous. Assuming the two particles have the same mass, m, show that

E=2E2mc2=mc2 (12.58)

FIGURE 12.29

Suppose you use protons (mc2=1GeV)with E=30GeV. What Edo you get? What multiple of E does this amount to? (1GeV=109electronvolts)[Because of this relativistic enhancement, most modern elementary particle experiments involve colliding beams, instead of fixed targets.]

Synchronized clocks are stationed at regular intervals, a million apart, along a straight line. When the clock next to you reads 12 noon:

(a) What time do you see on the 90thclock down the line?

(b) What time do you observe on that clock?

(a) Draw a space-time diagram representing a game of catch (or a conversation) between two people at rest, apart. How is it possible for them to communicate, given that their separation is spacelike?

(b) There's an old limerick that runs as follows:

There once was a girl named Ms. Bright,

Who could travel much faster than light.

She departed one day,

The Einsteinian way,

And returned on the previous night.

What do you think? Even if she could travel faster than light, could she return before she set out? Could she arrive at some intermediate destination before she set out? Draw a space-time diagram representing this trip.

Show that the potential representation (Eq. 12.133) automatically satisfies [Suggestion: Use Prob. 12.54.]

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