The fission cross section in a nuclear reactor is a measure of the probability that a neutron will induce fission in a particular nucleus. It is a crucial parameter for determining the neutron flux and reaction rates within the reactor core. Different isotopes have different fission cross sections depending on their ability to undergo fission when struck by a neutron.
Different elements absorb neutrons to different extents. The measure of this is called the neutron absorption cross section, you can visualise this as the size of a scoop collecting water from a stream, or something similar. Cadmium just happens to have a very large cross section for slow neutrons which are the main cause of the fission chain reaction in a reactor. Boron has similar properties. The precise reason for this involves study of nuclear physics, which you will have to read up in a scientific book on the subject, to get some understanding.
Hafnium is used in nuclear reactors as a control rod material to regulate the nuclear fission process. It has a high neutron-capture cross-section, meaning it is effective in absorbing neutrons and controlling the rate of the nuclear reaction. The addition of hafnium control rods helps maintain the reactor at a safe and stable operating condition.
Control rods are made of materials that readily absorb neutrons, such as boron or cadmium. These materials have a high neutron absorption cross section, which means they are very likely to absorb a neutron when it comes in contact with them. The design and placement of control rods in a nuclear reactor are carefully engineered to ensure that they absorb just enough neutrons to control the rate of the nuclear reaction without completely stopping it.
Not at all, the temperature of U-235 or Pu-239 which are used for nuclear energy production by fission, has no effect on the fission reaction, which is driven only by the capture cross-section for neutron capture. Slow neutrons are captured more strongly than fast ones, so it is an advantage for the moderator not to be at a high temperature.
1. Energy (heat) 2. Fast neutrons 3. Fission products (atoms of other elements of lower atomic weight, often very radioactive). All three are produced simultaneously, for every fission that occurs.
Different elements absorb neutrons to different extents. The measure of this is called the neutron absorption cross section, you can visualise this as the size of a scoop collecting water from a stream, or something similar. Cadmium just happens to have a very large cross section for slow neutrons which are the main cause of the fission chain reaction in a reactor. Boron has similar properties. The precise reason for this involves study of nuclear physics, which you will have to read up in a scientific book on the subject, to get some understanding.
In nuclear physics, a cross section is essentially the probability that a nucleus will interact with something. An isotope with a high fission cross section, like U-235, is very likely to absorb a thermal (slow) neutron and undergo fission. The cross section has units of area, usually cm2, which is where the name comes from. When the cross section is multiplied by the neutron flux, the product is the fission rate, or number of fissions per second.
Cadmium is used in nuclear reactors as a control rod material. Control rods are inserted into the reactor core to absorb neutrons and regulate the nuclear fission process. Cadmium has a high neutron absorption cross-section, making it effective for controlling the rate of nuclear reactions.
They are used in nuclear reactor to control the rate of fission of uranium and plutonium. Because these elements have different capture cross sections for neutrons of varying energies, the compositions of the control rods must be designed for the neutron spectrum of the reactor it is supposed to control.
Hafnium is used in nuclear reactors as a control rod material to regulate the nuclear fission process. It has a high neutron-capture cross-section, meaning it is effective in absorbing neutrons and controlling the rate of the nuclear reaction. The addition of hafnium control rods helps maintain the reactor at a safe and stable operating condition.
They are used in nuclear reactor to control the rate of fission of uranium and plutonium. Because these elements have different capture cross sections for neutrons of varying energies, the compositions of the control rods must be designed for the neutron spectrum of the reactor it is supposed to control.
The source of energy in a nuclear reactor is the release of binding energy, i.e. the binding energy that hold protons and neutrons together in the nucleus of the atom. Heavy nuclides, such as uranium, are split into lighter nuclides, such as cesium and barium (and many others, in a semi-random cross section). The binding energy required to hold the original uranium together is less than the daughter products and is released to the system in the form of heat and other radiation.
Control rods are made of materials that readily absorb neutrons, such as boron or cadmium. These materials have a high neutron absorption cross section, which means they are very likely to absorb a neutron when it comes in contact with them. The design and placement of control rods in a nuclear reactor are carefully engineered to ensure that they absorb just enough neutrons to control the rate of the nuclear reaction without completely stopping it.
A nuclear cross section is a "technical" way of saying how large a "target" a given atomic nucleus presents to an incoming neutron. And we need to know that about different elements, and about the different isotopes of those elements. There are some other applications, but this is the "biggie" for the use of the term nuclear cross section. And we need to start with the idea that fission begins with a neutron entering an atomic nucleus to cause fission. If your model of nuclear fission is a cue ball breaking a rack of billliard balls, we need to refine it. Get you from the "B" grade to an "A" grade in physics. A neutron doesn't "smash" an atomic nucleus. It is captured by it (neutron capture) and an instability results. A neutron released in the fission process comes away from the fission event like a bullet out of a gun. Because it is moving so "fast" it has a low probability of being captured. It needs to undergo some scattering (little "collisions" with other atomic nuclei) to slow it down (thermalize it). The thermal neutron has a higher probability of being captured by a given nucleus and causing another fission, if it is captured by a fissionable atom. We've seen how the energy of the neutron affects its probability of being captured, but it turns out that different elements present a different sized "target" for the neutron. The size depends on the energy of that neutron, but also on the element being targeted, and which isotope of that element is under consideration. To repeat, each element has a different nuclear cross section (target size) for a neutron (of a given energy), and each isotope of a given element has a different nuclear cross section (for that same given neutron energy). Three things are at work. The energy of the neutron aside, the element and the different isotopes of each element have different probabilities of capturing a neutron of a given energy. The nuclear cross section is a measure of the "receptivity" of a given nucleus to an incoming neutron. It's that probability of capture. That's it in a nutshell. Links can be found below.
Boron has a high nuclear cross section. That means that it easily stop neutrons. Neutrons are necessary for nuclear fission to occur. Boron is used in the control rods, for startup and shutdown control, as well as for low to medium power modulation. It is also used as an emergency criticality control, injected into the core, in the event of failure of the control rods to work. It is also injected into the coolant after a refueling operation to trim reactivity and prevent the new fuel rods from being too reactive.
Control rods have a large neutron absorption cross section. That means that they slow down, absorb, and effectively stop neutrons. In order to sustain a fission reaction, you need a certain number of neutrons of a certain energy interacting with fissile material at a certain rate so that everything is in equilibrium. When you insert the control rods, you bring the core geometry to a sub-critical state, what we call KEffective < 1, and the fission reaction stops.
Helium is used as a coolant in nuclear gas reactors because it is chemically inert, meaning it does not react with other materials in the reactor. It has high thermal conductivity, which helps in transferring heat away from the reactor core efficiently. Helium also has low neutron capture cross-section, making it less likely to absorb neutrons and become radioactive.