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The rest energy and total energy, respectively, of three particles, expressed in terms of a basic amount A are (1) A, 2A; (2) A, 3A; (3) 3A, 4A. Without written calculation, rank the particles according to their (a) mass, (b) kinetic energy, (c) Lorentz factor, and (d) speed, greatest first.

Short Answer

Expert verified

a) m3>m1=m2

b) k2>k1=k3

c) γ3>γ2>γ1

d)v3>v2>v1

Step by step solution

01

Mass

a)

An object at rest has some energy called rest mass energy and is expressed as

E=mc2

Lets use 1,2, and 3 subscripts for three particles respectively. The rest mass energy for three particles are given below

E1=AE2=AE3=3Awidth="66">E1=AE2=AE3=3A

As rest mass energy is only dependent on mass with c2 term being constant. Therefore, the particle with greatest rest energy will have greatest mass, here it is the third particle. As 1st and 2nd particle has same rest energy will have same mass.

m3>m1=m2

02

Kinetic energy

(b)

Kinetic energy can be expressed as total energy minus rest mass energy.

k=T-E

Here, in the problem the total energies and rest energies are given, therefore the kinetic energies of the three particles are

K1=2A-A=AK2=3A-A=2AK4=4A-3A=A

Therefore,

K2>K1=K3

03

Lorentz factor

The result of 2nd postulate of the special theory of relativity is that the clocks run slower for a moving object when measured from a rest frame. The factor by which the clock is running differently is called the Lorentz factor.

The expression for Lorentz factor is

Y=11-β2

Here βis the speed parameter v/c.

The expression for total energy of an object is

T=γmc2

The total energies of the three particles is

T1=2AT2=3AT3=4A

Rankings will be

T3>T2>T1γ3m3c2>γ2m2c2>γ1m1c2γ3m3>γ2m2>γ1m1

Let’s consider particle 1 and 2

γ2m2>γ1m1

As m1=m2, therefore, γ2>γ1.

And for particle 3, the mass and total energy, both are greatest, therefore will be greatest.

γ3>γ2>γ1

(d)

And, as Lorentz factor is related to speed with relation

γ=11-β2β=1-1γ2v=c1-1γ2

Therefore,

V3>V2>V1

Hence, greatest γwill have greatest speed.

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