An electron has a wavelength of 239 nm. Find its momentum. Planck’s constant is 6.63*10^-34?
λ is equal to h/p.
This equation contains three symbols:
A) The particle's wavelength is represented by λ; B) Planck's constant is represented by h; and C) the particle's momentum is represented by p.
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To find the momentum of an electron, we can use the de Broglie wavelength formula:
[ \text{wavelength} = \frac{h}{p} ]
Where:
- ( \text{wavelength} = 239 , \text{nm} = 239 \times 10^{-9} , \text{m} )
- ( h = 6.63 \times 10^{-34} , \text{m}^2 \cdot \text{kg/s} ) (Planck's constant)
- ( p ) is the momentum of the electron.
Rearranging the formula to solve for momentum:
[ p = \frac{h}{\text{wavelength}} ]
Substituting the given values:
[ p = \frac{6.63 \times 10^{-34} , \text{m}^2 \cdot \text{kg/s}}{239 \times 10^{-9} , \text{m}} ]
[ p = \frac{6.63 \times 10^{-34}}{239} \times 10^{-9} , \text{kg} \cdot \text{m/s} ]
[ p \approx 2.78 \times 10^{-27} , \text{kg} \cdot \text{m/s} ]
So, the momentum of the electron is approximately ( 2.78 \times 10^{-27} , \text{kg} \cdot \text{m/s} ).
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When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.
When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.
When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.
When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.
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