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A charged particle carrying charge 1 mu ...

A charged particle carrying charge `1 mu C` is moving with velocity `(2 hati + 3hati + 4hatk) ms^(-1)`. If an external magnetic field of `(5 hati + 3hatj - 6hatk) xx 10^(-3)T` exists in the region where the particle is moving then the force on the particle is `vecF xx 10^(-9)N`. The vector `vecF` is :

A

`-0.30 hati + 0.32 hatj - 0.9 hatk`

B

`-3.0 hati + 3.2hatj -0.9 hatk`

C

`-30hati + 32hatj - 9hatk`

D

`-300 hati + 320 hatj - 90hatk`

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To find the force on a charged particle moving in a magnetic field, we use the formula: \[ \vec{F} = q (\vec{v} \times \vec{B}) \] where: - \( \vec{F} \) is the force, - \( q \) is the charge, - \( \vec{v} \) is the velocity vector, and - \( \vec{B} \) is the magnetic field vector. Given: - Charge \( q = 1 \mu C = 1 \times 10^{-6} C \) - Velocity \( \vec{v} = (2 \hat{i} + 3 \hat{j} + 4 \hat{k}) \, m/s \) - Magnetic field \( \vec{B} = (5 \hat{i} + 3 \hat{j} - 6 \hat{k}) \times 10^{-3} \, T \) ### Step 1: Calculate the cross product \( \vec{v} \times \vec{B} \) We will set up the determinant for the cross product: \[ \vec{v} \times \vec{B} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 2 & 3 & 4 \\ 5 \times 10^{-3} & 3 \times 10^{-3} & -6 \times 10^{-3} \end{vmatrix} \] ### Step 2: Expand the determinant Calculating the determinant, we have: \[ \vec{v} \times \vec{B} = \hat{i} \begin{vmatrix} 3 & 4 \\ 3 \times 10^{-3} & -6 \times 10^{-3} \end{vmatrix} - \hat{j} \begin{vmatrix} 2 & 4 \\ 5 \times 10^{-3} & -6 \times 10^{-3} \end{vmatrix} + \hat{k} \begin{vmatrix} 2 & 3 \\ 5 \times 10^{-3} & 3 \times 10^{-3} \end{vmatrix} \] Calculating each of these 2x2 determinants: 1. For \( \hat{i} \): \[ 3 \times (-6 \times 10^{-3}) - 4 \times (3 \times 10^{-3}) = -18 \times 10^{-3} - 12 \times 10^{-3} = -30 \times 10^{-3} \] 2. For \( -\hat{j} \): \[ 2 \times (-6 \times 10^{-3}) - 4 \times (5 \times 10^{-3}) = -12 \times 10^{-3} - 20 \times 10^{-3} = -32 \times 10^{-3} \] Thus, it becomes \( +32 \times 10^{-3} \hat{j} \). 3. For \( \hat{k} \): \[ 2 \times (3 \times 10^{-3}) - 3 \times (5 \times 10^{-3}) = 6 \times 10^{-3} - 15 \times 10^{-3} = -9 \times 10^{-3} \] ### Step 3: Combine the results Putting it all together, we have: \[ \vec{v} \times \vec{B} = (-30 \times 10^{-3}) \hat{i} + (32 \times 10^{-3}) \hat{j} + (-9 \times 10^{-3}) \hat{k} \] ### Step 4: Multiply by charge \( q \) Now, we multiply by the charge \( q \): \[ \vec{F} = q (\vec{v} \times \vec{B}) = (1 \times 10^{-6}) \times (-30 \times 10^{-3} \hat{i} + 32 \times 10^{-3} \hat{j} - 9 \times 10^{-3} \hat{k}) \] Calculating this gives: \[ \vec{F} = (-30 \times 10^{-9} \hat{i} + 32 \times 10^{-9} \hat{j} - 9 \times 10^{-9} \hat{k}) \, N \] ### Final Result Thus, the force on the particle is: \[ \vec{F} = -30 \hat{i} + 32 \hat{j} - 9 \hat{k} \times 10^{-9} \, N \]

To find the force on a charged particle moving in a magnetic field, we use the formula: \[ \vec{F} = q (\vec{v} \times \vec{B}) \] where: - \( \vec{F} \) is the force, ...
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