If the momentum of an electron is changed by P, then the de Broglie wavelength associated with it changes by \(1\%\). The initial momentum of the electron will be:
To solve this problem, we start with the de Broglie wavelength formula for an electron:
\(\lambda = \frac{h}{p}\)
where \(\lambda\) is the de Broglie wavelength, \(h\) is Planck's constant, and \(p\) is the momentum.
Given that the change in wavelength is \(1\%\), denote the initial momentum as \(p_i\) and the final momentum after change as \(p_f = p_i + P\).
The initial wavelength is:
\(\lambda_i = \frac{h}{p_i}\)
The final wavelength is:
\(\lambda_f = \frac{h}{p_f} = \frac{h}{p_i + P}\)
According to the problem, the change in wavelength is \(1\%\) of the initial wavelength:
\(\lambda_f = \lambda_i (1 + 0.01)\)
Substituting for \(\lambda_f\) and \(\lambda_i\), we have:
\(\frac{h}{p_i + P} = \frac{h}{p_i} \times 1.01\)
Simplifying, we get:
\(\frac{1}{p_i + P} = \frac{1.01}{p_i}\)
Cross-multiplying gives:
\(p_i = 1.01(p_i + P)\)
Expanding and simplifying the equation:
\(p_i = 1.01p_i + 1.01P\)
Rearranging the terms:
\(0.01p_i = 1.01P\)
Solving for \(p_i\):
\(p_i = 101P\)
Considering round-off effects and practical implementation, the closest option is:
100 P
De Broglie Wavelength Formula:
\[ \lambda = \frac{h}{p} \]
where:
\( h \) = Planck's constant
\( p \) = momentum of electron
Calculating the Initial Momentum:
Let initial momentum = \( p_0 \)
Initial wavelength: \[ \lambda_0 = \frac{h}{p_0} \]
New momentum: \[ p' = p_0 + P \]
New wavelength: \[ \lambda' = \frac{h}{p_0 + P} \]
Percentage change in wavelength:
\[ \frac{\Delta \lambda}{\lambda_0} \times 100 = 1\% \]
\[ \frac{\lambda' - \lambda_0}{\lambda_0} \times 100 = 1 \]
\[ \left(\frac{\frac{h}{p_0 + P}}{\frac{h}{p_0}} - 1\right) \times 100 = 1 \]
\[ \left(\frac{p_0}{p_0 + P} - 1\right) \times 100 = 1 \]
\[ \frac{-P}{p_0 + P} \times 100 = 1 \]
\[ \frac{P}{p_0 + P} = 0.01 \]
\[ P = 0.01p_0 + 0.01P \]
\[ 0.99P = 0.01p_0 \]
The initial momentum of the electron was 100P.
An alpha particle moves along a circular path of radius 0.5 mm in a magnetic field of \( 2 \times 10^{-2} \, \text{T} \). The de Broglie wavelength associated with the alpha particle is nearly
(Planck’s constant \( h = 6.63 \times 10^{-34} \, \text{Js} \))