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- Newsgroups: sci.physics
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- From: draper@sscvx1.ssc.gov
- Subject: Re: What are the conditions for Mass <-> Energy conversion
- Message-ID: <1992Dec29.154112.1@sscvx1.ssc.gov>
- Lines: 98
- Sender: usenet@sunova.ssc.gov (News Admin)
- Nntp-Posting-Host: sscvx1
- Organization: Superconducting Super Collider Laboratory
- References: <8091@tekig7.PEN.TEK.COM> <1992Dec26.134900.7041@hubcap.clemson.edu> <1992Dec28.024210.17537@monu6.cc.monash.edu.au>
- Date: Tue, 29 Dec 1992 21:41:12 GMT
-
- Sorry for the bandwidth, but I need to include alot of what I'm replying to
- for clarity...
- In article <1992Dec28.024210.17537@monu6.cc.monash.edu.au>, darice@yoyo.cc.monash.edu.au (Fred Rice) writes:
- > 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.
- >
- That's because equation 6 is wrong.
- What you probably meant to say is that conservation of energy demands
- E^2 = (E1 + E2)^2
- so that
- E^2 = p^2 = p1^2 + m1^2 + p2^2 + m2^2 + 2E1E2
- and since by conservation of momentum
- p = p1 + p2
- we then get
- p1^2 + p2^2 + 2p1p2cos(A) = p1^2 + m1^2 + p2^2 + m2^2 + 2E1E2.
- Solving for cos(A) gives
- cos(A) = [m1^2 + m2^2]/2p1p2 + E1E2/p1p2
- Now as long as m1 and m2 are nonzero, the first term on the right is
- positive-definite and the second term is greater than 1. Thus there is no real
- solution for A.
-
- But I generally only take off a couple of points for algebra errors.
-
- Paul Draper
- University of Texas at Arlington
- Mythink, not UTAthink, not SSCthink, not GOVthink
-