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Nuclear fission is the process by which a heavy atomic nucleus, such as uranium-235 or plutonium-239, absorbs a neutron and becomes unstable. This instability causes the nucleus to split into two lighter nuclei, known as fission fragments, along with the release of additional neutrons and a substantial amount of energy.
The fission process begins when a nucleus captures a neutron, leading to a compound nucleus in an excited state. For instance, when uranium-235 ($^{235}U$) absorbs a neutron ($n$), it forms uranium-236 ($^{236}U$) in an excited state:
$$ ^{235}U + ^{1}n \rightarrow ^{236}U^* $$The energy released during nuclear fission primarily arises from the difference in binding energy between the reactants and the products. Binding energy per nucleon is higher in the fission fragments compared to the original heavy nucleus, resulting in the release of energy. This energy manifests as kinetic energy of the fission fragments, emitted neutrons, and electromagnetic radiation.
A critical aspect of nuclear fission is the possibility of a chain reaction. The neutrons released during fission can induce further fission events in adjacent nuclei. For a sustained chain reaction, at least one of the emitted neutrons must trigger another fission event. This concept is foundational in both nuclear reactors and atomic bombs.
The concept of critical mass is central to sustaining a chain reaction. Critical mass is the minimum amount of fissile material needed to maintain a self-sustaining chain reaction. Factors affecting critical mass include the type of fissile material, its purity, shape, and the presence of a neutron reflector. For example, the critical mass of $^{235}U$ is approximately 52 kilograms in a spherical shape without a reflector.
In nuclear reactors, neutron moderators and absorbers play vital roles in controlling the rate of the chain reaction. Moderators, such as water or graphite, slow down the fast neutrons produced during fission, increasing the likelihood of further fission events. Absorbers, or control rods made of materials like cadmium or boron, capture excess neutrons to regulate the reaction rate and prevent runaway scenarios.
The theoretical understanding of nuclear fission involves several models and equations. One fundamental equation related to fission energy release is derived from Einstein’s mass-energy equivalence:
$$ E = \Delta m \cdot c^2 $$The Capture Cross-Section ($\sigma$) is another important parameter, representing the probability of a neutron being absorbed by a nucleus, contributing to fission:
$$ \sigma = \frac{\text{Number of fissions}}{\text{Neutron flux} \times \text{Number of target nuclei}} $$Aspect | Nuclear Fission | Nuclear Fusion |
---|---|---|
Definition | Splitting of a heavy nucleus into lighter nuclei. | Joining of light nuclei to form a heavier nucleus. |
Energy Release | Releases significant energy per reaction. | Releases even more energy per reaction than fission. |
Fissile Materials | Uranium-235, Plutonium-239. | Hydrogen isotopes (Deuterium, Tritium). |
Chain Reaction | Supports a chain reaction with emitted neutrons. | Requires extreme conditions; chain reactions are not yet feasible. |
Byproducts | Produces radioactive waste. | Produces minimal radioactive waste. |
Applications | Nuclear power, nuclear weapons. | Currently limited to experimental reactors and stars. |
Safety Concerns | Potential for nuclear accidents and proliferation. | Challenges in achieving controlled reactions and managing high temperatures. |
1. **Mnemonic for Fission Steps:** "Neutron Captures, Nucleus Cracks, Neutrons Released" helps remember the sequence.
2. **Visualize the Process:** Drawing diagrams of the fission process can aid in understanding the splitting and neutron emission.
3. **Understand Key Equations:** Familiarize yourself with $E = \Delta m \cdot c^2$ and the capture cross-section formula to solve related problems efficiently.
4. **Practice Past Papers:** Engage with IB Physics SL past exam questions on nuclear fission to reinforce your knowledge and application skills.
1. The first controlled nuclear chain reaction was achieved in 1942 under the stands of the University of Chicago's Stagg Field, marking a pivotal moment in scientific history.
2. Nuclear fission was discovered accidentally in 1938 by Otto Hahn and Fritz Strassmann while they were experimenting with bombarding uranium with neutrons.
3. The energy released from fission can power cities for days with just a small amount of uranium, showcasing its immense potential for energy generation.
1. **Incorrect:** Assuming all neutrons released cause fission.
**Correct:** Only a fraction of emitted neutrons successfully induce further fission.
2. **Incorrect:** Confusing nuclear fission with radioactive decay.
**Correct:** Fission involves splitting a large nucleus, while radioactive decay is the spontaneous transformation of an unstable nucleus.
3. **Incorrect:** Overlooking the role of moderators in controlling the chain reaction.
**Correct:** Recognizing that moderators like water are essential to slow down neutrons and sustain the reaction.