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A hydrogen ion moving with a velocity of...

A hydrogen ion moving with a velocity of `10^(4)m//s` enters in magentic field `10^(-4)T` perpendicularly, then its radius of circular path is

A

10.01 m

B

1.01 m

C

101 m

D

0.101 m

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The correct Answer is:
To find the radius of the circular path of a hydrogen ion moving in a magnetic field, we can use the relationship between the magnetic force acting on the ion and the centripetal force required to keep it in circular motion. ### Step-by-Step Solution: 1. **Identify the Given Values:** - Velocity of the hydrogen ion, \( v = 10^4 \, \text{m/s} \) - Magnetic field strength, \( B = 10^{-4} \, \text{T} \) - Charge of a hydrogen ion, \( q = 1.6 \times 10^{-19} \, \text{C} \) - Mass of a hydrogen ion, \( m = 1.67 \times 10^{-27} \, \text{kg} \) 2. **Set Up the Equations:** The magnetic force \( F_m \) acting on the ion is given by: \[ F_m = q v B \] The centripetal force \( F_c \) required to keep the ion in circular motion is given by: \[ F_c = \frac{m v^2}{r} \] Where \( r \) is the radius of the circular path. 3. **Equate the Forces:** Since the magnetic force provides the centripetal force, we can set these two equations equal to each other: \[ q v B = \frac{m v^2}{r} \] 4. **Rearrange to Solve for \( r \):** Rearranging the equation to find the radius \( r \): \[ r = \frac{m v}{q B} \] 5. **Substitute the Known Values:** Now, substitute the values into the equation: \[ r = \frac{(1.67 \times 10^{-27} \, \text{kg}) (10^4 \, \text{m/s})}{(1.6 \times 10^{-19} \, \text{C}) (10^{-4} \, \text{T})} \] 6. **Calculate the Numerator:** \[ \text{Numerator} = 1.67 \times 10^{-27} \times 10^4 = 1.67 \times 10^{-23} \] 7. **Calculate the Denominator:** \[ \text{Denominator} = 1.6 \times 10^{-19} \times 10^{-4} = 1.6 \times 10^{-23} \] 8. **Final Calculation:** Now, divide the numerator by the denominator: \[ r = \frac{1.67 \times 10^{-23}}{1.6 \times 10^{-23}} \approx 1.04 \, \text{m} \] ### Conclusion: The radius of the circular path of the hydrogen ion in the magnetic field is approximately \( r \approx 1.04 \, \text{m} \).
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