12.2 CHAPTER 12. WAVE NATURE OF MATTER
λ =
h
mv=
6 , 63 × 10 −^34 J· s
(0,150 kg)(40 m· s−^1 )
= 1, 11 × 10 −^34 mThis wavelength is considerably smaller thanthe diameter of a
proton which is approximately 10 −^15 m. Hence the wave-like
properties of this cricketball are too small to beobserved.Example 2: The de Broglie wavelength of an electron
QUESTIONCalculate the de Brogliewavelength of an electron moving at 40 m·s−^1.SOLUTIONStep 1 : Determine what is required and how to approach the problem
We are required to calculate the de Broglie wavelength of an
electron given its speed. We can do this by using:λ =
h
mvStep 2 : Determine what is given
We are given:- The velocity of the electron v = 40 m· s−^1
and we know: - The mass of the electron me= 9, 11 × 10 −^31 kg
- Planck’s constant h = 6, 63 × 10 −^34 J· s
Step 3 : Calculate the de Broglie wavelengthλ =h
mv=
6 , 63 × 10 −^34 J· s
(9, 11 × 10 −^31 kg)(40 m· s−^1 )
= 1, 82 × 10 −^5 m
= 0,0182 mm