Construct Your Own Problem

Consider the decay of radioactive substances in the Earth's interior. The energy emitted is converted to thermal energy that reaches the earth's surface and is radiated away into cold dark space. Construct a problem in which you estimate the activity in a cubic meter of earth rock? And then calculate the power generated. Calculate how much power must cross each square meter of the Earth's surface if the power is dissipated at the same rate as it is generated. Among the things to consider are the activity per cubic meter, the energy per decay, and the size of the Earth.

Short Answer

Expert verified

a) The activity of the earth rock in cubic meter is\(R = \frac{E}{{{E_\alpha }}}\).

b) Calculated power generate is\(P\)is\(\left( {1.6 \times {{10}^{ - 13}}} \right)q\;W\).

c) The power crosses per unit cubic meter is \(\left( {1.48 \times {{10}^{ - 33}}} \right)q\frac{{\rm{W}}}{{{{\rm{m}}^3}}}\).

Step by step solution

01

Definition of thermal energy

The energy contained within a system that is accountable for its temperature is referred to as thermal energy. The transfer of thermal energy is referred to as heat.

02

Activity of the earth rock in cubic meter

Consider the given problem.

The energy, the heat radiated and the volume of earth is related by the formula given by:

\(\begin{align}{}E & = \frac{Q}{{{V_e}}}\\E & = \frac{{q\,{\rm{MeV}}}}{{\frac{4}{3}\pi {{\rm{R}}^3}}}\end{align}\)

Where\(Q\) is the heat radiated,\(E\) is energy and the\({V_e}\) is the volume of earth

Now substitute the value of\(R & = 6380\;{\rm{km}}\) as the radius of earth is\(6380\;{\rm{km}}\)in the above equation

\(\begin{align}{}E & = \frac{{q\,{\rm{MeV}}/{\rm{s}}}}{{\frac{4}{3}\pi {{(6380\,{\rm{Km}})}^3}}}\\ & = \frac{{q\,{\rm{MeV}}/{\rm{s}}}}{{\frac{4}{3} \times 3.14{{\left( {6380 \times {{10}^3}\;\,{\rm{m}}} \right)}^3}}}\\ & = \frac{{q\,{\rm{MeV}}/{\rm{s}}}}{{1.09 \times {{10}^{21}}\;\,{{\rm{m}}^3}}}\end{align}\)

Thus, the activity of earth's rock is given by:

\(R & = \frac{{\rm{E}}}{{{{\rm{E}}_\alpha }}}\)

Therefore, the value of \(R\) is \(\frac{{\rm{E}}}{{{{\rm{E}}_\alpha }}}\).

03

Calculate the power generated

b)

Find the power generated.

The power generating is the energy per unit time\(P = E\).

so after plug in the value we get,

\(\begin{array}{c}P = q\,{\rm{MeV}}/{\rm{s}}\\ = \left( {1.6 \times {{10}^{ - 13}}} \right)\,q\;{\rm{J}}/{\rm{s}}\\ = \left( {1.6 \times {{10}^{ - 13}}} \right)\,q\;{\rm{W}}\\P = \left( {1.6 \times {{10}^{ - 13}}} \right)\,q\;{\rm{W}}\end{array}\)

Therefore, the value of \(P\) is\(\left( {1.6 \times {{10}^{ - 13}}} \right)q\;{\rm{W}}\).

04

The power crosses per unit cubic meter

c)

Let us solve the given problem.

The power crosses per unit cubic meter is\(p = \frac{{\rm{P}}}{{{{\rm{V}}_e}}}\).

Plug in the value we get ,

\(\begin{array}{c}p = \frac{{\left( {1.6 \times {{10}^{ - 13}}} \right)q\;{\rm{W}}}}{{1.09 \times {{10}^{21}}\;{{\rm{m}}^3}}}\\ = \left( {1.48 \times {{10}^{ - 33}}} \right)q\,\frac{{\rm{W}}}{{{{\rm{m}}^3}}}p\\ = \left( {1.48 \times {{10}^{ - 33}}} \right)q\,\frac{{\rm{W}}}{{{{\rm{m}}^3}}}\end{array}\)

Therefore, the value of \(t\) is \(\left( {1.48 \times {{10}^{ - 33}}} \right)q\frac{{\rm{W}}}{{{{\rm{m}}^3}}}\).

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Most popular questions from this chapter

Suppose a particle of ionizing radiation deposits\(1.0\,{\rm{MeV}}\)in the gas of a Geiger tube, all of which goes to creating ion pairs. Each ion pair requires\(30.0\,{\rm{eV}}\)of energy. (a) The applied voltage sweeps the ions out of the gas in\(1.00\,{\rm{\mu s}}\). What is the current? (b) This current is smaller than the actual current since the applied voltage in the Geiger tube accelerates the separated ions, which then create other ion pairs in subsequent collisions. What is the current if this last effect multiplies the number of ion pairs by\({\rm{900}}\)?

  1. The \(^{{\rm{210}}}\) Po source used in a physics laboratory is labelled as having an activity of \(1.0\,{\rm{\mu Ci}}\) on the date it was prepared. A student measures the radioactivity of this source with a Geiger counter and observes 1500 counts per minute. She notices that the source was prepared 120 days before her lab. What fraction of the decays is she observing with her apparatus?
  2. Identify some of the reasons that only a fraction of the αs emitted are observed by the detector.

What is the ratio of the velocity of a \(5.00\,{\rm{MeV }}\beta \)ray to that of an\({\rm{\alpha }}\) particle with the same kinetic energy? This should confirm that \({\rm{\beta }}\) s travel much faster than \({\rm{\alpha }}\) s even when relativity is taken into consideration. (See also Exercise \({\rm{31}}{\rm{.11}}\).)

What is the difference betweenγrays and characteristic x rays? Is either necessarily more energetic than the other? Which can be the most energetic?

Radioactivity depends on the nucleus and not the atom or its chemical state. Why, then, is one kilogram of uranium more radioactive than one kilogram of uranium hexafluoride?

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