Problem
An electron, with a mass of 9.11 Γ 10 β 31 β k g 9.11 \times 10^{-31} \, \mathrm{kg} 9.11 Γ 1 0 β 31 kg , moves with a speed of 0.75 c 0.75c 0.75 c . Find its relativistic momentum and compare this value with the momentum calculated from the classical expression.
Data
Rest mass of electron: m 0 = 9.11 Γ 10 β 31 β k g m_0 = 9.11 \times 10^{-31} \, \mathrm{kg} m 0 β = 9.11 Γ 1 0 β 31 kg
Speed of electron: v = 0.75 c v = 0.75c v = 0.75 c
Speed of light: c = 3 Γ 10 8 β m s β 1 c = 3 \times 10^8 \, \mathrm{ms}^{-1} c = 3 Γ 1 0 8 ms β 1
To Find:
Relativistic momentum (p rel p_{\text{rel}} p rel β )
Classical momentum (p class p_{\text{class}} p class β )
Prerequisite Concepts
Relativistic momentum:
p rel = m 0 v 1 β v 2 c 2 p_{\text{rel}} = \frac{m_0 v}{\sqrt{1 - \frac{v^2}{c^2}}} p rel β = 1 β c 2 v 2 β β m 0 β v β
where m 0 m_0 m 0 β is the rest mass, v v v is the speed of the electron, and c c c is the speed of light.
Classical momentum:
p class = m 0 v p_{\text{class}} = m_0 v p class β = m 0 β v
Solution
Step 1: Relativistic Momentum
Using the formula for relativistic momentum:
p rel = m 0 v 1 β v 2 c 2 p_{\text{rel}} = \frac{m_0 v}{\sqrt{1 - \frac{v^2}{c^2}}} p rel β = 1 β c 2 v 2 β β m 0 β v β
Substitute the given values:
p rel = ( 9.11 Γ 10 β 31 ) Γ ( 0.75 Γ 3 Γ 10 8 ) 1 β ( 0.75 c ) 2 c 2 p_{\text{rel}} = \frac{(9.11 \times 10^{-31}) \times (0.75 \times 3 \times 10^8)}{\sqrt{1 - \frac{(0.75c)^2}{c^2}}} p rel β = 1 β c 2 ( 0.75 c ) 2 β β ( 9.11 Γ 1 0 β 31 ) Γ ( 0.75 Γ 3 Γ 1 0 8 ) β
Simplify the denominator:
1 β ( 0.75 ) 2 c 2 c 2 = 1 β 0.5625 = 0.4375 = 0.6614 \sqrt{1 - \frac{(0.75)^2 c^2}{c^2}} = \sqrt{1 - 0.5625} = \sqrt{0.4375} = 0.6614 1 β c 2 ( 0.75 ) 2 c 2 β β = 1 β 0.5625 β = 0.4375 β = 0.6614
Now calculate:
p rel = ( 9.11 Γ 10 β 31 ) Γ ( 0.75 Γ 3 Γ 10 8 ) 0.6614 p_{\text{rel}} = \frac{(9.11 \times 10^{-31}) \times (0.75 \times 3 \times 10^8)}{0.6614} p rel β = 0.6614 ( 9.11 Γ 1 0 β 31 ) Γ ( 0.75 Γ 3 Γ 1 0 8 ) β
p rel = 2.05 Γ 10 β 22 0.6614 = 3.10 Γ 10 β 22 β k g β m s β 1 p_{\text{rel}} = \frac{2.05 \times 10^{-22}}{0.6614} = 3.10 \times 10^{-22} \, \mathrm{kg \, ms^{-1}} p rel β = 0.6614 2.05 Γ 1 0 β 22 β = 3.10 Γ 1 0 β 22 kg m s β 1
Step 2: Classical Momentum
Using the classical formula:
p class = m 0 v p_{\text{class}} = m_0 v p class β = m 0 β v
Substitute the values:
p class = ( 9.11 Γ 10 β 31 ) Γ ( 0.75 Γ 3 Γ 10 8 ) p_{\text{class}} = (9.11 \times 10^{-31}) \times (0.75 \times 3 \times 10^8) p class β = ( 9.11 Γ 1 0 β 31 ) Γ ( 0.75 Γ 3 Γ 1 0 8 )
p class = 2.05 Γ 10 β 22 β k g β m s β 1 p_{\text{class}} = 2.05 \times 10^{-22} \, \mathrm{kg \, ms^{-1}} p class β = 2.05 Γ 1 0 β 22 kg m s β 1
Answer
Relativistic Momentum:
p rel = 3.10 Γ 10 β 22 β k g β m s β 1 p_{\text{rel}} = 3.10 \times 10^{-22} \, \mathrm{kg \, ms^{-1}} p rel β = 3.10 Γ 1 0 β 22 kg m s β 1
Classical Momentum:
p class = 2.05 Γ 10 β 22 β k g β m s β 1 p_{\text{class}} = 2.05 \times 10^{-22} \, \mathrm{kg \, ms^{-1}} p class β = 2.05 Γ 1 0 β 22 kg m s β 1
Comparison:
The relativistic momentum is approximately 60 % 60\% 60% greater than the classical momentum, highlighting the importance of relativistic effects at high speeds.