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Derivation of E=mc2

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Derivation of E=mc2 Yum-Yum Physics! * * * * * * * * * * * * * * * * * * * By the Work-Energy Theorem: In this case, we will consider PE = 0 so: From the definition ... – PowerPoint PPT presentation

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Title: Derivation of E=mc2


1
Derivation of Emc2
Yum-Yum Physics!
2
By the Work-Energy Theorem
In this case, we will consider PE 0 so
From the definition of work
Therefore
3
From Newtons original statement of Fma
This, along with the previous equation yields
4
We have dt and dx in the equation. Lets write it
all in terms of dt
When the variable changes from dx to dt, we must
also change the bounds of the integral
5
We can eliminate the dts so
Notice that the dt changed to d(mv) so the bounds
also changed
For velocities approaching c, the mass increases
The relativistic mass is
6
Since m0 is a constant, it can factored out of
the integral
Applying the Quotient Rule (keep in mind v is a
variable and c is a constant)
Yikes!
7
Combining these expressions for Energy yields
8
To get a common denominator, we will multiply the
numerator and denominator of by
9
Simplifying
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To evaluate the integral we make the substitution
Therefore
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Recall the relativistic mass
Substituting this yields
or
18
Make everything as simple as possible, but
not simpler!
19
Second Derivation
20
Consider a box with a light source of negligible
mass at the left end and a black absorber of
negligible mass at the other end. The total mass
of the box, source, and absorber is M. a Photon
is emitted from the left. It strikes the absorber
and is absorbed.
21
By conservation of momentum, when the photon
leaves the source, and travels right, the box
must move to the left to maintain a total
momentum of 0 in the system. We will use two
methods to calculate how far the box moves, and
equate the results.
22
The energy of a photon is given by
From de Broglies Equation
Thus
23
By the Law of Conservation of Momentum, the
momentum of the photon equals the momentum of the
box
From its definition, the velocity of the photon
is given by the displacement divided by the time
24
The velocity of the box is
The amount of time that the box moves is
The distance the box moves is
25
From the mass-energy equivalence, the photon
has mass since it has energy. Let this mass be m
(mltltM).
Since there is no external force on the system,
the center of mass must remain in the same
place. Therefore the moments of the box and
photon must have the same value
26
Equating the two expressions for d yields
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