Physics - Ch 66 Ch 4 Quantum Mechanics: Schrodinger Eqn (23 of 92) Prob. of Finding Particle 3
TLDRThe video script discusses the calculation of the probability of finding a particle in a specific location within a potential well. It explains the process of defining the region of interest and using the probability density function to find the likelihood at the first energy level. The script details the mathematical steps, including the use of trigonometric identities and integration, to arrive at the probability for a small region between L/4 and L/4 + ΞX. The result provides an understanding of the particle's presence in that area and hints at a method for approximating the result more efficiently.
Takeaways
- π The topic is finding the probability of a particle being in a specific location, using the electron line model.
- π The region of interest is between x = L/4 and x = L/4 + ΞX, with ΞX being a very small distance (0.01L).
- 𧬠The probability is calculated using the probability density function, which is the square of the wave function at each point.
- π The wave function for the first energy level (N=1) is considered, which is real and does not require complex conjugate multiplication.
- π The calculation involves integrating the sine squared of an angle, using the trigonometric identity (1 - cos(2ΞΈ))/2.
- π’ The integral is computed over the specified limits (0.25L to 0.26L), with the proper differential (2Ο/L * dx).
- π The result simplifies to a difference in sines of the upper and lower limits, divided by L and 2Ο.
- π― As ΞX approaches zero, the probability of finding the particle at the exact location L/4 approaches 0.1.
- π The method can be used to find the probability of finding the particle at any point along the path, offering a 1% chance at any given point.
- π The approach demonstrates how to calculate probabilities for particles in quantum mechanics, particularly in a one-dimensional infinite potential well.
Q & A
What is the main objective of the discussion in the transcript?
-The main objective is to find the probability of finding a particle in a particular location, specifically between x equals L/4 and a small distance farther (Delta X).
How is Delta X defined in the context of the transcript?
-Delta X is defined as a very small distance, specifically 0.01L, representing the range in which the probability of finding the particle is being calculated.
What is the significance of the first energy level (N equals 1) in this discussion?
-At the first energy level (N equals 1), the probability density function is used to find the particle at any point between 0 and L, which is crucial for calculating the probability in the specified region.
How is the probability calculated for the particle being between L/4 and L/4 + Delta X?
-The probability is calculated by integrating the square of the wave function (since it's real and doesn't require complex conjugation) over the interval from L/4 to L/4 + Delta X.
What trigonometric identity is used in the calculation?
-The trigonometric identity used is 1/2 * (1 - cos(2 * angle)), where the angle is 2 * n * PI * x / L.
How does the integral change when Delta X becomes very small?
-As Delta X approaches zero, the second part of the interval becomes infinitely small, and the probability of finding the particle at exactly that location (L/4) approaches 0.1.
What is the final probability calculated for the particle being in the region from x equals L/4 to x equals L/4 plus Delta X?
-The final probability calculated is approximately 0.0103L, or a 1% chance of finding the particle in that small region.
Why is the wave function used in the calculation without its complex conjugate?
-The wave function is used without its complex conjugate because it does not have an imaginary part at the first energy level (N equals 1).
What does the probability density function represent in this context?
-The probability density function represents the probability of finding the particle at any point between 0 and L at the first energy level.
How does the probability change as we make Delta X smaller?
-As Delta X becomes smaller, the probability of finding the particle at a specific location (L/4) increases, approaching 0.1 or 10% as Delta X goes to zero.
Outlines
π Calculating Particle Probability in a Defined Region
This paragraph explains the process of determining the probability of finding a particle within a specific region. It introduces the concept of defining a region between two points, x equals L/4 and x equals L/4 + ΞX, where ΞX is a very small distance (0.01L). The discussion revolves around the probability density function and the calculation of probability by integrating the wave function's square over the defined region. The integral is broken down into two parts, and the trigonometric identity for sine squared is applied. The calculation involves finding the difference in sine values at the upper and lower limits of the integral, which simplifies to a result that represents the probability of finding the particle in the given region.
π Probability as ΞX Approaches Zero and the 1% Chance
The second paragraph delves into the implications of making ΞX, the interval for finding the particle, increasingly smaller. It explains that as ΞX approaches zero, the probability of finding the particle at an exact location (L/4) converges to a specific value, which is 0.1 in this case. The paragraph emphasizes the concept that the probability of finding the particle anywhere along the path within the small region is about 1%, and this probability can be calculated for any specific point along the particle's path. The explanation concludes with a discussion on the mathematical approach to finding the particle's probability at any given point in the region.
Mindmap
Keywords
π‘probability
π‘particle
π‘wave function
π‘energy level
π‘potential well
π‘trigonometric identity
π‘integration
π‘differential
π‘limits of integration
π‘quantum tunneling
π‘radians
Highlights
The main objective is to find the probability of a particle being in a specific location.
The region of interest is defined between x equals L/4 and a small distance farther (Delta X = 0.01L).
The probability is calculated for the first energy level (N=1) of the particle in a one-dimensional box.
The probability density function is used, which is the product of the wave function since it's real-valued.
The integral involves the sine squared of an angle, which can be simplified using a trigonometric identity.
The limits of integration are 0.25L and 0.26L, representing the region of interest.
The integral is separated into two parts for easier calculation.
The proper differential is used in the integral, which involves multiplying by 2Ο/L.
The integral of the cosine function results in the sine function, which simplifies the expression.
The probability is found by evaluating the sine functions at the upper and lower limits of integration.
The final probability expression is simplified by canceling out L and combining terms.
The probability of finding the particle in the small region is approximately 0.0103L.
As Delta X approaches zero, the probability of finding the particle at an exact location becomes a definite value.
The process can be used to find the probability of finding the particle at any point along the path.
The method provides a way to calculate the probability distribution of a particle in a quantum system.
The approach demonstrates the application of wave functions and quantum mechanics principles in determining particle location probabilities.
The explanation includes a step-by-step breakdown of the mathematical process, making it accessible for understanding.
Transcripts
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