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8 - N u m e r i c a l   3

Problem

An electron, with a mass of 9.11Γ—10βˆ’31 kg9.11 \times 10^{-31} \, \mathrm{kg}, moves with a speed of 0.75c0.75c. Find its relativistic momentum and compare this value with the momentum calculated from the classical expression.


Data

  • Rest mass of electron: m0=9.11Γ—10βˆ’31 kgm_0 = 9.11 \times 10^{-31} \, \mathrm{kg}
  • Speed of electron: v=0.75cv = 0.75c
  • Speed of light: c=3Γ—108 msβˆ’1c = 3 \times 10^8 \, \mathrm{ms}^{-1}

To Find:

  1. Relativistic momentum (prelp_{\text{rel}})
  2. Classical momentum (pclassp_{\text{class}})

Prerequisite Concepts

  1. Relativistic momentum:
prel=m0v1βˆ’v2c2 p_{\text{rel}} = \frac{m_0 v}{\sqrt{1 - \frac{v^2}{c^2}}}

where m0m_0 is the rest mass, vv is the speed of the electron, and cc is the speed of light.

  1. Classical momentum:
pclass=m0v p_{\text{class}} = m_0 v

Solution

Step 1: Relativistic Momentum

Using the formula for relativistic momentum:

prel=m0v1βˆ’v2c2p_{\text{rel}} = \frac{m_0 v}{\sqrt{1 - \frac{v^2}{c^2}}}

Substitute the given values:

prel=(9.11Γ—10βˆ’31)Γ—(0.75Γ—3Γ—108)1βˆ’(0.75c)2c2p_{\text{rel}} = \frac{(9.11 \times 10^{-31}) \times (0.75 \times 3 \times 10^8)}{\sqrt{1 - \frac{(0.75c)^2}{c^2}}}

Simplify the denominator:

1βˆ’(0.75)2c2c2=1βˆ’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

Now calculate:

prel=(9.11Γ—10βˆ’31)Γ—(0.75Γ—3Γ—108)0.6614p_{\text{rel}} = \frac{(9.11 \times 10^{-31}) \times (0.75 \times 3 \times 10^8)}{0.6614} prel=2.05Γ—10βˆ’220.6614=3.10Γ—10βˆ’22 kg msβˆ’1p_{\text{rel}} = \frac{2.05 \times 10^{-22}}{0.6614} = 3.10 \times 10^{-22} \, \mathrm{kg \, ms^{-1}}

Step 2: Classical Momentum

Using the classical formula:

pclass=m0vp_{\text{class}} = m_0 v

Substitute the values:

pclass=(9.11Γ—10βˆ’31)Γ—(0.75Γ—3Γ—108)p_{\text{class}} = (9.11 \times 10^{-31}) \times (0.75 \times 3 \times 10^8) pclass=2.05Γ—10βˆ’22 kg msβˆ’1p_{\text{class}} = 2.05 \times 10^{-22} \, \mathrm{kg \, ms^{-1}}

Answer

  1. Relativistic Momentum:
prel=3.10Γ—10βˆ’22 kg msβˆ’1 p_{\text{rel}} = 3.10 \times 10^{-22} \, \mathrm{kg \, ms^{-1}}
  1. Classical Momentum:
pclass=2.05Γ—10βˆ’22 kg msβˆ’1 p_{\text{class}} = 2.05 \times 10^{-22} \, \mathrm{kg \, ms^{-1}}

Comparison:

The relativistic momentum is approximately 60%60\% greater than the classical momentum, highlighting the importance of relativistic effects at high speeds.