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- Newsgroups: sci.physics
- Path: sparky!uunet!munnari.oz.au!bruce.cs.monash.edu.au!monu6!yoyo.cc.monash.edu.au!darice
- From: darice@yoyo.cc.monash.edu.au (Fred Rice)
- Subject: Re: What are the conditions for Mass <-> Energy conversion
- Message-ID: <1992Dec28.024210.17537@monu6.cc.monash.edu.au>
- Sender: news@monu6.cc.monash.edu.au (Usenet system)
- Organization: Monash University, Melb., Australia.
- References: <8091@tekig7.PEN.TEK.COM> <1992Dec26.134900.7041@hubcap.clemson.edu>
- Date: Mon, 28 Dec 1992 02:42:10 GMT
- Lines: 124
-
- In <1992Dec26.134900.7041@hubcap.clemson.edu> jtbell@hubcap.clemson.edu (Jon Bell) writes:
- >In article <8091@tekig7.PEN.TEK.COM> bhides@tekig1.PEN.TEK.COM (Sandhiprakas J Bhide) writes:
- >>
- >>Now, if it is indeed true, why is that sunrays or for that matter
- >>any other energy such as heat does not by itself convert into mass?
- >>That is while I am shaving in front of the mirror, why is that the
- >>light emnating from the lamp does not get converted into mass?
- >>
- >Various "conservation laws" have to be satisfied. For example, a single
- >photon (quantum of light energy) traveling through "empty" space
- >cannot spontaneously convert into a material particle (or convert part
- >of its energy into one) because it would violate conservation of
- >momentum. However, if a high-energy (e.g. gamma-ray) photon passes near
- >an atomic nucleus, it can produce an electron-positron pair, because
- >the nucleus can recoil slightly to conserve momentum.
-
- In more detail, according to special relativity, the following relation
- holds:
-
- E^2 = (p^2)(c^2) + (m^2)(c^4) [1]
-
- where E=energy, p=momentum, m=mass,
- and c=speed of light, which is a constant.
-
- We require conservation of energy and momentum, i.e. of E and p.
-
- Since a photon has no mass, it's energy squared according to [1] is
-
- E(photon)^2 = (p^2)(c^2) [2]
-
- whereas the energy of a single particle is the full equation given in [1].
- Since we require energy to be conserved (and thus energy squared to be
- conserved), equating [2] and [1], for the initial photon before
- conversion to mass and the particle after the photon is converted to
- mass, we get
-
- (p^2)(c^2) = (p^2)(c^2) + (m^2)(c^4) [3].
-
- The momentum (p) on the left hand side (for the photon) and on the right
- hand side (for the particle) are identical because we require
- conservation of momentum.
-
- Equation [3] simplifies to
-
- 0 = (m^2)(c^4) [5].
-
- Since c is a nonzero constant, in equation [5] we require m=0, i.e. a
- single photon cannot spontaneously convert into a single particle with mass.
-
- How about a photon converting into two particles?
-
- Let's say our two particles, 1 and 2, have masses m1 and m2 and momenta
- p1 and p2 respectively, and let's leave p to be the momentum of the
- photon.
-
- Then equation [3] becomes:
-
- (p^2)(c^2) = (p1^2)(c^2) + (p2^2)(c^2) + (m1^2)(c^4) + (m2^2)(c^4)
- = (p1^2 + p2^2)(c^2) + (m1^2 + m2^2)(c^4) [6]
-
- However, due to conservation of momentum, we require _p_ = _p1_ + _p2_,
- where _a_ means that _a_ is a vector,
- and therefore _p_^2 = (_p1_ + _p2_)^2 = p1^2 + p2^2 + 2p1p2cos(A), where A
- is the angle between _p1_ and _p2_. Thus [6] becomes
-
- (p1^2 + p2^2 + 2p1p2cos(A))(c^2) = (p1^2 + p2^2)(c^2) + (m1^2 + m2^2)(c^4)
-
- => 2p1p2cos(A) = (m1^2 + m2^2)(c^2) [7]
-
- Equation [7] is the equation that needs to be fulfilled in
- order to have a photon spontaneously convert into two particles (such as
- an electron-positron pair).
-
- This seems to me to be possible.
-
- For example, let's say an electron-positron pair is created, each having
- a mass of m0. (By the way, in this case m0 = 0.511 MeV/c^2.)
- For simplification, let's also assume that the angle A -> 0, and thus
- cos(A) -> 1. And, for further simplification, let's assume that the
- magnitude of the momenta of particles 1 and 2 are equal, i.e., that
- p1 = p2. Then [7] becomes
-
- 2(p1^2) = 2(m0^2)(c^2) [8]
-
- According to Relativity, the relation of the momentum, p, to the
- velocity, v, of a particle of mass m0, is
-
- p = m0 * v [9]
- -----------------
- [1-(v/c)^2]^(1/2)
-
- Substituting this into [8], we get
-
- 2(m0^2)(v^2)
- ------------ = 2(m0^2)(c^2)
- [1-(v/c)^2]
-
- => (v^2)/(c^2) = 1 - (v^2)/(c^2) [assuming m0 does not equal 0]
-
- => 2(v^2) = c^2
-
- => v^2 = 1/2(c^2)
-
- which is a possible result (i.e. v < c).
-
- So, it seems to me that a photon *can* spontaneously convert into two
- particles with mass, as long as it has enough energy.
-
- So, could Jon Bell or someone else remark on this?
- My math, assuming it is mistake-free, contradicts what Jon Bell was claiming.
-
- >In this example, an electron-positron pair has to be produced (not just an
- >electron or just a positron) so that electric charge is conserved.
-
- >Actually, in the case of light rays coming from your shaving lamp, the
- >photons have so little energy (a few eV apiece) that they cannot possibly
- >produce even the least massive particles (electrons/positrons, 511,000 eV
- >apiece).
-
- >Jon Bell / Dept. of Physics & C.S. / Presbyterian College / Clinton SC USA
- >would violate
-
- Fred Rice
- darice@yoyo.cc.monash.edu.au
-