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Comment on “Length-dependent translation of messenger RNA by ribosomes”

Yunxin Zhang Shanghai Key Laboratory for Contemporary Applied Mathematics, Laboratory of Mathematics for Nonlinear Science, Centre for Computational Systems Biology, and School of Mathematical Sciences, Fudan University, Shanghai 200433, China. Email: xyz@fudan.edu.cn.
Abstract

In the recent paper of Valleriani et al [Phys. Rev. E 83, 042903 (2011)], a simple model for describing the translation of messenger RNA (mRNA) by ribosomes is presented, and an expression of the translational ratio rr, defined as the ratio of translation rate ωtl\omega_{\rm tl} of protein from mRNA to degradation rate ωp\omega_{p} of protein, is obtained. The key point to get this ratio rr is to get the translation rate ωtl\omega_{\rm tl}. In the study of Valleriani et al, ωtl\omega_{\rm tl} is assumed to be the mean value of measured translation rate, i.e. the mean value of ratio of the translation number of protein to the lifetime of mRNA. However, in experiments different methods might be used to get ωtl\omega_{\rm tl}. Therefore, for the sake of future application of their model to more experimental data analysis, in this comment three methods to get the translation rate ωtl\omega_{\rm tl}, and consequently the translational ratio rr, are provided. Based on one of the methods which might be employed in most of the experiments, we find that the translational ratio rr decays exponentially with the length of mRNA in prokaryotic cells, and decays reciprocally with the length of mRNA in eukaryotic cells. This result is slight different from that obtained in Valleriani’s study.

pacs:
87.10.Mn, 87.14.gn, 87.15.A.

In recent paper Valleriani2011 , Valleriani et al presented a simple model to describe the length-dependent translation properties of messager RNA (mRNA). In their model, the mRNA degradation process is assumed to be governed by rate ωr\omega_{r}, i.e. the probability density of lifetime tt of an intact mRNA is

ϕU=ωrexp(ωrt).\phi_{U}=\omega_{r}\exp(-\omega_{r}t). (1)

Meanwhile, the rate of ribosome entering the coding region of mRNA is assumed to be ωon\omega_{\rm on}, and the degradation rate of protein is denoted by ωp\omega_{p}.

To discuss the mRNA length-dependent properties of the translation to protein by ribosomes, in Valleriani2011 the expression of translational ratio, defined as

r=ωtl/ωp,r={\omega_{\rm tl}}/{\omega_{p}}, (2)

is obtained for translations in both prokaryotic and eukaryotic cells. Where ωtl\omega_{\rm tl} is the translation rate from mRNA to protein by ribosomes. Since the protein degradation rate ωp\omega_{p} is independent of mRNA, the essential point to analyze the mRNA length-dependent properties of the translational ratio rr, is to get the expression of translation rate ωtl\omega_{\rm tl}. Experimentally, there might be three methods to get ωtl\omega_{\rm tl}:

(I): ωtl\omega_{\rm tl} is obtained as the mean value of the measured translation rate f(t)f(t) from mRNA to protein, i.e.,

ωtl=f(t)=0f(t)ϕU(t)𝑑t,\omega_{\rm tl}=\langle f(t)\rangle=\int_{0}^{\infty}f(t)\phi_{U}(t)dt, (3)

where f(t)=N(t)/T(t)f(t)=N(t)/T(t), N(t)N(t) is the mean number of proteins that the mRNA will synthesize if degradation occurs at time tt, and T(t)T(t) is the lifetime of a mRNA before completely degraded (tt is the lifetime of an intact mRNA).

(II): ωtl\omega_{\rm tl} is obtained as the ratio of mean number N(t)\langle N(t)\rangle of proteins translated from one mRNA to the mean lifetime T(t)\langle T(t)\rangle of a mRNA, i.e.,

ωtl=N(t)/T(t).\omega_{\rm tl}=\left.{\langle N(t)\rangle}\right/{\langle T(t)\rangle}. (4)

(III): ωtl\omega_{\rm tl} is obtained as the reciprocal of the mean duration time of translating one protein from mRNA,

ωtl=11/f(t)=1T(t)/N(t).\omega_{\rm tl}=\frac{1}{\langle 1/f(t)\rangle}=\frac{1}{\langle T(t)/N(t)\rangle}. (5)

One can easily show that, for the mRNA translation problem discussed in Valleriani2011 , T(t)=tT(t)=t, N(t)=θ(ttLpro)ωon(ttLpro)N(t)=\theta(t-t_{L}^{\rm pro})\omega_{\rm on}(t-t_{L}^{\rm pro}) for translation in prokaryotic cells, and T(t)=t+tLeuT(t)=t+t_{L}^{\rm eu}, N(t)=ωontN(t)=\omega_{\rm on}t for translation in eukaryotic cells. Where θ(t)\theta(t) is Heaviside function, i.e. θ(t)=1\theta(t)=1 for t>0t>0 and θ(t)=0\theta(t)=0 for t<0t<0, tLpro=L/vprot_{L}^{\rm pro}=L/v^{\rm pro} and tLeu=L/veut_{L}^{\rm eu}=L/v^{\rm eu} are the time taken by ribosomes to reach the end of mRNA, LL is the length of mRNA, vprov^{\rm pro} and veuv^{\rm eu} are the average velocities of ribosome along mRNA in prokaryotic and eukaryotic cells respectively.

Intuitively, method (I) is reasonable, and actually this method is used in Valleriani2011 . On the other hand, method (III) is usually employed for some mathematical problems. For example, to get the mean translation rate ω\omega of a process which includes two sub-processes with rate ω1\omega_{1} and ω2\omega_{2}, one usually does the following calculations

ω=1T=1T1+T2=11/ω1+1/ω2=ω1ω2ω1+ω2.\omega=\frac{1}{\langle T\rangle}=\frac{1}{\langle T_{1}\rangle+\langle T_{2}\rangle}=\frac{1}{1/\omega_{1}+1/\omega_{2}}=\frac{\omega_{1}\omega_{2}}{\omega_{1}+\omega_{2}}. (6)

It should be pointed out that, if the method (III) is employed to get ωtl\omega_{\rm tl}, the experimental samples with no protein synthesized, i.e. samples for N(t)=0N(t)=0, should be discarded to avoid the infinite waiting time cases. Correspondingly, in the theoretical calculation in Eq. (5), the average T(t)/N(t)\langle T(t)/N(t)\rangle should be done for only large enough time ttlimt\geq t_{\rm lim} which satisfies N(t)1N(t)\geq 1, and the probability density ϕU\phi_{U} should be changed accordingly, ϕ^U(t)=ϕU(t)/tlimϕU(t)𝑑t=ωrexp[ωr(ttlim)]\hat{\phi}_{U}(t)=\phi_{U}(t)/\int_{t_{\rm lim}}^{\infty}\phi_{U}(t)dt=\omega_{r}\exp[-\omega_{r}(t-t_{\rm lim})] for ttlimt\geq t_{\rm lim}. In our numerical calculations, we use tlimpro=tLpro+1/ωont_{\rm lim}^{\rm pro}=t_{L}^{\rm pro}+1/\omega_{\rm on} for translation in prokaryotic cells, and tlimeu=1/ωont_{\rm lim}^{\rm eu}=1/\omega_{\rm on} for translation in eukaryotic cells.

Meanwhile, the simple method (II) is often used in the experimental data statistics. For this mRNA translation problem, one can easily get the following results by method (II). For mRNA translation in prokaryotic cells,

ωtlpro=\displaystyle\omega_{\rm tl}^{\rm pro}= θ(ttLpro)ωon(ttLpro)/t\displaystyle\left.{\left\langle\theta(t-t_{L}^{\rm pro})\omega_{\rm on}(t-t_{L}^{\rm pro})\right\rangle}\right/{\langle t\rangle} (7)
=\displaystyle= ωonexp(ωrtLpro).\displaystyle\omega_{\rm on}\exp(-\omega_{r}t_{L}^{\rm pro}).

So the translational ratio rpro=ωtlpro/ωpr^{\rm pro}=\omega_{\rm tl}^{\rm pro}/\omega_{p} decays exponentially with the length LproL^{\rm pro} of mRNA. Meanwhile, for the mRNA translation in eukaryotic cells,

ωtleu=ωont/t+tLeu=ωon/(1+ωrtLeu).\omega_{\rm tl}^{\rm eu}=\left.{\langle\omega_{\rm on}t\rangle}\right/{\langle t+t_{L}^{\rm eu}\rangle}=\left.{\omega_{\rm on}}\right/({1+\omega_{r}t_{L}^{\rm eu}}). (8)

So, roughly speaking, the translational ratio reu=ωtleu/ωpr^{\rm eu}=\omega_{\rm tl}^{\rm eu}/\omega_{p} decays reciprocally with the length of mRNA. Note: similar as the above discussion about the calculation of translation rate ωtl\omega_{\rm tl} in prokaryotic cells by method III, if the samples with N(t)=0N(t)=0 are discarded in experimental measurements, the methods I and II should also be changed correspondingly, with a modified probability density ϕ^U(t)\hat{\phi}_{U}(t) for ttlimt\geq t_{\rm lim} only.

For the sake of comparison, the theoretical results of translational ratio rr of E. coli and S. cerevisiae, obtained by the three methods, are plotted in Fig. 1, with model parameters listed in Tab. 1. Since method I is used by Valleriani et al. in Valleriani2011 , the curves in Fig. 1 (and the corresponding model parameters in Tab. 1) are copied from Valleriani2011 . One can see that, compared with the experimental data, these three methods all work reasonably well, but with slightly different model parameter (see Tab. 1). The most reasonable parameters should be the ones which are obtained by the same method as that used in the experimental measurements.

In conclusion, when one tries to apply the model presented in Valleriani2011 to real experimental data, the method used to get the translation rate ωtl\omega_{\rm tl} should be chosen properly to be consist with experiments.

Acknowledgments This work was supported by the Natural Science Foundation of Shanghai (Grant 11ZR1403700).

References

  • (1) A. Valleriani, G. Zhang, A. Nagar, Z. Ignatova, and R. Lipowsky Phys. Rev. E. 83, 042903 (2011).
Table 1: Model parameters ωon/ωp\omega_{\rm on}/\omega_{p} and ωr\omega_{r} obtained by fitting the theoretical results to experimental data of E. coli and S. cerevisiae respectively (see Ref. Valleriani2011 and references therein for the detailed description of the experimental data).
E. coli S. cerevisiae
ωon/ωp\omega_{\rm on}/\omega_{p} ωr\omega_{r}(min-1) ωon/ωp\omega_{\rm on}/\omega_{p} ωr\omega_{r}(min-1)
Valleriani et al. 708.2 0.2 7.69×103\times 10^{3} 0.2
method II 734 0.61 6.34×103\times 10^{3} 0.22
method III 841.1 0.15 6.62×103\times 10^{3} 0.02
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Figure 1: (Color online) Theoretical results of the translational ratio rpror^{\rm pro} for E. coli (a) and reur^{\rm eu} for S. cerevisiae (b). The dots and solid curves are copied from Ref. Valleriani2011 (see the related references therein). The model parameters ωon/ωp\omega_{\rm on}/\omega_{p} and ωr\omega_{r} used in the calculations are listed in Tab. 1.