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Radio-Isotopes in Biochemistry
| Common name | Decay equation | Half-Life | Limit Energy in MeV |
|---|---|---|---|
| Tritium | 1H3 → 2He3 + β- + anti-neutrino | 12¼ y | 0.019 |
| C-14 | 6C14 → 7N14 + β- + anti-neutrino | 5,730 y | 0.16 |
| S-35 | 16S35 → 17Cl35 + β- + anti-neutrino | 88 d | 0.17 |
| I-131 | 33I131 → 34Xe131 + β- + anti-neutrino | 8.0 d | 0.61 |
| P-32 | 15P32 → 16S32 + β- + anti-neutrino | 14 d | 1.71 |
At one point add P-32 phosphate. Newly forming RNA and DNA will incorporate the P-32. After a minute, add a thousand-times as much P-31 phosphate. From then one newly forming RNA and DNA will not be radioactive.
If we isolate RNA from the culture a minute after adding the P-31, any RNA that was made during the time before adding P-31 will be radioactive (but none after the "quenching"). Suppose we have a good amount of radioactivity associated with the macromolecular fraction.
We allow our culture to grow two more minutes, and again isolate RNA. But this time there is no macromolecular P-32. Where did it go?
Next, let's take a look at the DNA made before, during, and after the P-32 "pulse."
Immediately, we use some of those new T4s to infect E.coli and they have a high efficiency of infection.
The next day we infect another batch of E.coli, but this time the efficiency has dropped more than a thousand fold. What happened in the refrigerator?
Would it have made any difference had we used tritiated thymidine rather that P-32?