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The de-Broglie wavelength L associated w...

The de-Broglie wavelength L associated with an elementary particle of linear momentum p is bets represented by the graph

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To solve the problem regarding the de Broglie wavelength \( L \) associated with an elementary particle of linear momentum \( p \), we can follow these steps: ### Step 1: Understand the de Broglie wavelength formula The de Broglie wavelength \( \lambda \) is given by the formula: \[ \lambda = \frac{h}{p} \] where \( h \) is the Planck constant and \( p \) is the linear momentum of the particle. ### Step 2: Identify the relationship between wavelength and momentum From the formula, we can see that the wavelength \( \lambda \) is inversely proportional to the momentum \( p \): \[ \lambda \propto \frac{1}{p} \] This means that as the momentum \( p \) increases, the wavelength \( \lambda \) decreases, and vice versa. ### Step 3: Rewrite the relationship using \( L \) In this problem, the wavelength is represented by \( L \): \[ L \propto \frac{1}{p} \] ### Step 4: Analyze the implications of the relationship - If \( p \) increases, \( L \) decreases. - If \( p \) decreases, \( L \) increases. ### Step 5: Determine the correct graph representation Given the relationship \( L \propto \frac{1}{p} \), the graph of \( L \) versus \( p \) should show a hyperbolic decline. This means that the graph will not be a straight line, nor will it be constant or exponential. ### Step 6: Evaluate the options provided 1. **Constant graph**: This is incorrect because \( L \) changes with \( p \). 2. **Straight line graph**: This is incorrect because \( L \) is inversely proportional to \( p \), not directly proportional. 3. **Exponential graph**: This is incorrect as well since the relationship is not exponential. 4. **Hyperbolic graph**: This is the correct representation as it shows the inverse relationship. ### Conclusion The best representation of the de Broglie wavelength \( L \) associated with an elementary particle of linear momentum \( p \) is a hyperbolic graph. ---
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