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The path of a charged particle in a unif...

The path of a charged particle in a uniform magnetic field depends on the angle `theta` between velocity vector and magnetic field, When `theta is 0^(@) or 180^(@), F_(m) = 0` hence path of a charged particle will be linear.
When `theta = 90^(@)`, the magnetic force is perpendicular to velocity at every instant. Hence path is a circle of radius `r = (mv)/(qB)`.
The time period for circular path will be `T = (2pim)/(qB)`
When `theta` is other than `0^(@), 180^(@) and 90^(@)`, velocity can be resolved into two components, one along `vec(B)` and perpendicular to B.
`v_(|/|)=cos theta`
`v_(^)= v sin theta`
The `v_(_|_)` component gives circular path and `v_(|/|)` givestraingt line path. The resultant path is a helical path. The radius of helical path
`r=(mv sin theta)/(qB)`
ich of helix is defined as `P=v_(|/|)T`
`P=(2 i mv cos theta)`
`p=(2 pi mv cos theta)/(qB)`
Two ions having masses in the ratio 1:1 and charges 1:2 are projected from same point into a uniform magnetic field with speed in the ratio 2:3 perpendicular to field. The ratio of radii of circle along which the two particles move is :

A

`4:3`

B

`2:3`

C

`3:2`

D

`3:4`

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The correct Answer is:
To solve the problem, we need to find the ratio of the radii of the circular paths of two ions moving in a uniform magnetic field. We will use the formula for the radius of the circular path of a charged particle in a magnetic field, which is given by: \[ r = \frac{mv}{qB} \] ### Step 1: Identify the given parameters - The masses of the two ions are in the ratio \( M_1 : M_2 = 1 : 1 \). - The charges of the two ions are in the ratio \( Q_1 : Q_2 = 1 : 2 \). - The speeds of the two ions are in the ratio \( V_1 : V_2 = 2 : 3 \). - The magnetic field \( B \) is uniform, so we can assume \( B_1 = B_2 \). ### Step 2: Write the formula for the radii of the two ions Using the formula for the radius of the path in a magnetic field, we can express the radii for both ions: - For Ion 1: \[ r_1 = \frac{M_1 V_1}{Q_1 B} \] - For Ion 2: \[ r_2 = \frac{M_2 V_2}{Q_2 B} \] ### Step 3: Find the ratio of the radii \( r_1 : r_2 \) To find the ratio \( \frac{r_1}{r_2} \), we substitute the expressions for \( r_1 \) and \( r_2 \): \[ \frac{r_1}{r_2} = \frac{\frac{M_1 V_1}{Q_1 B}}{\frac{M_2 V_2}{Q_2 B}} = \frac{M_1 V_1 Q_2}{M_2 V_2 Q_1} \] ### Step 4: Substitute the known ratios Now we substitute the known ratios into the equation: - \( M_1 : M_2 = 1 : 1 \) implies \( \frac{M_1}{M_2} = 1 \) - \( Q_1 : Q_2 = 1 : 2 \) implies \( \frac{Q_2}{Q_1} = 2 \) - \( V_1 : V_2 = 2 : 3 \) implies \( \frac{V_1}{V_2} = \frac{2}{3} \) Substituting these values into the ratio: \[ \frac{r_1}{r_2} = \frac{1 \cdot V_1 \cdot 2}{1 \cdot V_2 \cdot 1} = \frac{2 V_1}{V_2} \] ### Step 5: Substitute the ratio of speeds Now substituting \( \frac{V_1}{V_2} = \frac{2}{3} \): \[ \frac{r_1}{r_2} = 2 \cdot \frac{2}{3} = \frac{4}{3} \] ### Conclusion Thus, the ratio of the radii of the circular paths of the two ions is: \[ \frac{r_1}{r_2} = \frac{4}{3} \]

To solve the problem, we need to find the ratio of the radii of the circular paths of two ions moving in a uniform magnetic field. We will use the formula for the radius of the circular path of a charged particle in a magnetic field, which is given by: \[ r = \frac{mv}{qB} \] ### Step 1: Identify the given parameters - The masses of the two ions are in the ratio \( M_1 : M_2 = 1 : 1 \). - The charges of the two ions are in the ratio \( Q_1 : Q_2 = 1 : 2 \). - The speeds of the two ions are in the ratio \( V_1 : V_2 = 2 : 3 \). ...
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The path of a charged particle in a uniform magnetic field depends on the angle theta between velocity vector and magnetic field, When theta is 0^(@) or 180^(@), F_(m) = 0 hence path of a charged particle will be linear. When theta = 90^(@) , the magnetic force is perpendicular to velocity at every instant. Hence path is a circle of radius r = (mv)/(qB) . The time period for circular path will be T = (2pim)/(qB) When theta is other than 0^(@), 180^(@) and 90^(@) , velocity can be resolved into two components, one along vec(B) and perpendicular to B. v_(|/|)=cos theta v_(^)= v sin theta The v_(_|_) component gives circular path and v_(|/|) givestraingt line path. The resultant path is a helical path. The radius of helical path r=(mv sin theta)/(qB) ich of helix is defined as P=v_(|/|)T P=(2 i mv cos theta) p=(2 pi mv cos theta)/(qB) Which particle will have minimum frequency of revolution when projected with the same velocity perpendicular to a magnetic field.

The path of a charged particle in a uniform magnetic field depends on the angle theta between velocity vector and magnetic field, When theta is 0^(@) or 180^(@), F_(m) = 0 hence path of a charged particle will be linear. When theta = 90^(@) , the magnetic force is perpendicular to velocity at every instant. Hence path is a circle of radius r = (mv)/(qB) . The time period for circular path will be T = (2pim)/(qB) When theta is other than 0^(@), 180^(@) and 90^(@) , velocity can be resolved into two components, one along vec(B) and perpendicular to B. v_(|/|)=cos theta v_(^)= v sin theta The v_(_|_) component gives circular path and v_(|/|) givestraingt line path. The resultant path is a helical path. The radius of helical path r=(mv sin theta)/(qB) ich of helix is defined as P=v_(|/|)T P=(2 i mv cos theta) p=(2 pi mv cos theta)/(qB) A charged particle moves in a uniform magnetic field. The velocity of particle at some instant makes acute angle with magnetic field. The path of the particle will be

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