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Why don't we observe the wave propertie...

Why don't we observe the wave properties of large objects such as a cricket ball?

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To understand why we don't observe the wave properties of large objects such as a cricket ball, we can follow these steps: ### Step 1: Understand de Broglie's Hypothesis According to de Broglie's hypothesis, every moving particle or body has an associated wavelength (λ), which can be calculated using the formula: \[ \lambda = \frac{H}{mv} \] where: - \( H \) is Planck's constant (\( 6.63 \times 10^{-34} \, \text{Js} \)), - \( m \) is the mass of the particle, - \( v \) is the velocity of the particle. ### Step 2: Determine the Mass and Velocity of a Cricket Ball Let's consider a typical cricket ball: - Mass (\( m \)) = 100 grams = \( 0.1 \, \text{kg} \) - Maximum velocity (\( v \)) = 50 meters per second. ### Step 3: Substitute Values into the de Broglie Equation Now, we can substitute the values of \( H \), \( m \), and \( v \) into the de Broglie equation: \[ \lambda = \frac{6.63 \times 10^{-34}}{0.1 \times 50} \] ### Step 4: Calculate the Wavelength Now, we perform the calculation: \[ \lambda = \frac{6.63 \times 10^{-34}}{5} \] \[ \lambda = 1.326 \times 10^{-34} \, \text{meters} \] ### Step 5: Analyze the Result The calculated wavelength (\( 1.32 \times 10^{-34} \, \text{meters} \)) is extremely small. Such a tiny wavelength is far beyond the detection capabilities of any current measuring instruments or detectors. ### Step 6: Conclusion Due to the extremely small wavelength associated with large objects like a cricket ball, we do not observe their wave properties. In contrast, microscopic particles like electrons, which have much smaller mass and can have relatively higher velocities, exhibit detectable wave properties. ---

To understand why we don't observe the wave properties of large objects such as a cricket ball, we can follow these steps: ### Step 1: Understand de Broglie's Hypothesis According to de Broglie's hypothesis, every moving particle or body has an associated wavelength (λ), which can be calculated using the formula: \[ \lambda = \frac{H}{mv} \] where: - \( H \) is Planck's constant (\( 6.63 \times 10^{-34} \, \text{Js} \)), - \( m \) is the mass of the particle, ...
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