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Chapter 30, Problem 41P

(a)

To determine

The temperature required for the carbon cycle.

(a)

Expert Solution
Check Mark

Answer to Problem 41P

The temperature required for the carbon cycle is 5×107K_.

Explanation of Solution

Write the expression for the kinetic energy to overcome the columbic repulsion barrier in the proton-proton cycle reaction

    K=ke(e)(2e)r        (I)

Here, K is the kinetic energy, ke is the columbic constant, e is the electronic charge, r is the separation between the charges.

Write the expression for the columbic barrier to Bethe’s fifth and eight reaction.

    KB=ke(e)(7e)r        (I)

Here, KB is the columbic energy barrier.

Write the expression for the temperature required for the carbon cycle reaction using equation (I) and (II).

    TC=72(Tpp)        (III)

Here, TC is the temperature of carbon cycle, Tpp is the temperature of proton-proton cycle.

Conclusion:

Substitute 1.5×107K for Tpp in equation (III) to find TC.

    TC=72(1.5×107K)=5.25×107K5×107K

Therefore, the temperature required for the carbon cycle is 5×107K_.

(b)

To determine

The energy released in each reaction in the carbon cycle and the overall energy released.

(b)

Expert Solution
Check Mark

Answer to Problem 41P

The energy released Q1=1.94MeV_, Q2=1.20MeV_, Q3=1.02MeV_, Q4=7.55MeV_, Q5=7.30MeV_, Q6=1.73MeV_, Q7=1.02MeV_, Q8=4.97MeV_ and the overall energy Q=26.7MeV_.

Explanation of Solution

Let the general reaction in the carbon cycle is as follows.

    a+XY+b        (IV)

Here, a is the bombarding particle, X is the target nucleus, b is the outgoing particle, Y is the product nucleus.

Write the expression for the energy released in the reaction given in equation (I).

    Q=[M(a)+M(X)M(Y)M(b)](931.5MeV/u)        (V)

Here, M(a) is the bombarding particle, M(X) is the mass of target nucleus, M(Y) is the mass of the product nucleus, M(b) is the mass of the outgoing particle.

Write the expression for the total energy released in the carbon-cycle reaction.

    Q=Q1+Q2+Q3+Q4+Q5+Q6+Q7+Q8=i=18Qi        (VI)

Here, Q is the total energy released in the carbon cycle reaction, Qi is the energy released in each reaction.

Conclusion:

Substitute 12.000000u for M(12C), 1.007825u for M(1H), 13.005739u for M(13N), 0u for M(γ) in equation (V) to solve for Q1.

    Q1=[12.000000u+1.007825u13.005739u](931.5MeV/u)=1.94MeV

Substitute 13.005739u for M(13N), 13.003355u for M(13C), 0.000549u for M(e) in equation (V) to find Q2.

    Q2=[13.005739u13.003355u2(0.000549u)](931.5MeV/u)=1.20MeV

Substitute 0.000549u for M(e+), 0.000549u for M(e), 0u for M(γ) in equation (V) to find Q3.

    Q3=2(0.000549u)(931.5MeV/u)=1.02MeV

Substitute 13.003355u for M(13C), 1.007825u for M(1H), 14.003074u for M(14N), 0u for M(γ) in equation (V) to find Q4.

    Q4=[13.003355u+1.007825u14.003074u](931.5MeV/u)=7.55MeV

Substitute 15.003065u for M(15O), 14.003074u for M(14N), 1.007825u for M(1H), 0u for M(γ) in equation (V) to find Q5.

    Q5=[14.003074u+1.007825u15.003065u](931.5MeV/u)=7.30MeV

Substitute 15.003065u for M(15O), 0.000549u for M(e+), 15.000109u for M(15N) in equation (V) to find Q6.

    Q6=[15.003065u15.000109u2(0.000549u)](931.5MeV/u)=1.73MeV

Substitute 0.000549u for M(e+), 0.000549u for M(e), 0u for M(γ) in equation (V) to find Q7.

    Q7=2(0.000549u)(931.5MeV/u)=1.02MeV

Substitute 15.000109u for M(15N), 1.007825u for M(1H), 12.000000u for M(12C), 4.002603u for M(4He) in equation (V) to find Q8.

    Q8=[15.000109u+1.007825u12.000000u4.002603u](931.5MeV/u)=4.97MeV

Substitute 1.94MeV for Q1, 1.20MeV for Q2, 1.02MeV for Q3, 7.55MeV for Q4, 7.30MeV for Q5, 1.73MeV for Q6, 1.20MeV for Q7, 4.97MeV for Q8 in equation (VI) to find Q.

    Q=1.94MeV+1.20MeV+1.20MeV+7.55MeV+7.30MeV+1.73MeV+1.20MeV+4.97MeV=26.7MeV

Therefore, the energy released Q1=1.94MeV_, Q2=1.20MeV_, Q3=1.02MeV_, Q4=7.55MeV_, Q5=7.30MeV_, Q6=1.73MeV_, Q7=1.02MeV_, Q8=4.97MeV_ and the overall energy Q=26.7MeV_.

(c)

To determine

Whether the energy carried off by the neutrinos is deposited in the star.

(c)

Expert Solution
Check Mark

Answer to Problem 41P

Not all the energy appeared as the internal energy in the star. When the neutrino is created, it is likely to fly apart without interacting with any other particles.

Explanation of Solution

The amount of energy released in the reaction is not appeared as the internal energy in the star. When a neutrino is created, it is more likely to fly directly out of the star without any interaction with other particles.

Conclusion:

Therefore, all the energy is not appeared as the internal energy in the star. When the neutrino is created, it is likely to fly apart without interacting with any other particles.

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Chapter 30 Solutions

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