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A charge of 4.0 muC is moving with a vel...

A charge of `4.0 muC` is moving with a velocity of `4.0 times 10^6ms^(–1)` along the positive y-axis under a magnetic field `vec B` of strength `(2 hat k)` T. The force acting on the charge is `x hat i N`. The value of x is __.

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To solve the problem, we will use the formula for the magnetic force acting on a charge moving in a magnetic field, which is given by: \[ \vec{F} = q(\vec{v} \times \vec{B}) \] where: - \(\vec{F}\) is the magnetic force, - \(q\) is the charge, - \(\vec{v}\) is the velocity vector, - \(\vec{B}\) is the magnetic field vector. ### Step 1: Convert the charge to coulombs The charge is given as \(4.0 \, \mu C\). We need to convert this to coulombs: \[ q = 4.0 \, \mu C = 4.0 \times 10^{-6} \, C \] **Hint:** Remember that \(1 \, \mu C = 10^{-6} \, C\). ### Step 2: Write the velocity vector The velocity is given as \(4.0 \times 10^6 \, m/s\) along the positive y-axis. Thus, we can express the velocity vector as: \[ \vec{v} = 4.0 \times 10^6 \, \hat{j} \, m/s \] **Hint:** The unit vector \(\hat{j}\) indicates the direction along the y-axis. ### Step 3: Write the magnetic field vector The magnetic field is given as \(2 \hat{k} \, T\). Therefore, we can express the magnetic field vector as: \[ \vec{B} = 2 \hat{k} \, T \] **Hint:** The unit vector \(\hat{k}\) indicates the direction along the z-axis. ### Step 4: Calculate the cross product \(\vec{v} \times \vec{B}\) Now we need to calculate the cross product of \(\vec{v}\) and \(\vec{B}\): \[ \vec{F} = q(\vec{v} \times \vec{B}) = 4.0 \times 10^{-6} \, C \cdot (\hat{j} \times \hat{k}) \] Using the right-hand rule, we find: \[ \hat{j} \times \hat{k} = \hat{i} \] Thus, we have: \[ \vec{v} \times \vec{B} = (4.0 \times 10^6) \cdot 2 \hat{i} = 8.0 \times 10^6 \hat{i} \] **Hint:** The right-hand rule helps determine the direction of the cross product. ### Step 5: Calculate the force \(\vec{F}\) Now substituting back into the force equation: \[ \vec{F} = q(\vec{v} \times \vec{B}) = 4.0 \times 10^{-6} \cdot (8.0 \times 10^6 \hat{i}) \] Calculating this gives: \[ \vec{F} = 32 \hat{i} \, N \] ### Conclusion The value of \(x\) in the force \(\vec{F} = x \hat{i} \, N\) is: \[ \boxed{32} \]
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