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A particle with charge 2.0 C movess thro...

A particle with charge 2.0 C movess through a uniform magnetic field. At one instant the velocity of the particle is `(2.0hati+4.0hatj+6.0hatk)` m`//`s and the magnetic force on the particle is `(4.0hati-20hatj+12hatk)` N.
The x and y components of the magnetic fields are equal. What is `vecB` ?

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To find the magnetic field vector \(\vec{B}\) given the information in the problem, we will follow these steps: ### Step 1: Define the magnetic field vector Since the x and y components of the magnetic field are equal, we can express the magnetic field vector as: \[ \vec{B} = x \hat{i} + x \hat{j} + z \hat{k} \] ### Step 2: Write the force equation The magnetic force \(\vec{F}\) on a charged particle moving in a magnetic field is given by the equation: \[ \vec{F} = q (\vec{v} \times \vec{B}) \] where \(q\) is the charge of the particle, \(\vec{v}\) is its velocity, and \(\vec{B}\) is the magnetic field. ### Step 3: Substitute known values Given: - Charge \(q = 2.0 \, \text{C}\) - Velocity \(\vec{v} = (2.0 \hat{i} + 4.0 \hat{j} + 6.0 \hat{k}) \, \text{m/s}\) - Force \(\vec{F} = (4.0 \hat{i} - 20.0 \hat{j} + 12.0 \hat{k}) \, \text{N}\) We can substitute these values into the force equation: \[ (4.0 \hat{i} - 20.0 \hat{j} + 12.0 \hat{k}) = 2.0 \, (\vec{v} \times \vec{B}) \] ### Step 4: Calculate the cross product \(\vec{v} \times \vec{B}\) Using the determinant method for the cross product: \[ \vec{v} \times \vec{B} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 2 & 4 & 6 \\ x & x & z \end{vmatrix} \] Calculating the determinant, we have: \[ \vec{v} \times \vec{B} = \hat{i} (4z - 6x) - \hat{j} (2z - 6x) + \hat{k} (2x - 4x) \] \[ = (4z - 6x) \hat{i} - (2z - 6x) \hat{j} - 2x \hat{k} \] ### Step 5: Substitute back into the force equation Now substituting \(\vec{v} \times \vec{B}\) back into the force equation: \[ (4.0 \hat{i} - 20.0 \hat{j} + 12.0 \hat{k}) = 2.0 \, ((4z - 6x) \hat{i} - (2z - 6x) \hat{j} - 2x \hat{k}) \] This simplifies to: \[ (4.0 \hat{i} - 20.0 \hat{j} + 12.0 \hat{k}) = (8z - 12x) \hat{i} - (4z - 12x) \hat{j} - 4x \hat{k} \] ### Step 6: Equate coefficients Now we equate the coefficients of \(\hat{i}\), \(\hat{j}\), and \(\hat{k}\): 1. For \(\hat{i}\): \[ 8z - 12x = 4 \quad \text{(1)} \] 2. For \(\hat{j}\): \[ -4z + 12x = -20 \quad \text{(2)} \] 3. For \(\hat{k}\): \[ -4x = 12 \quad \text{(3)} \] ### Step 7: Solve the equations From equation (3): \[ x = -3 \] Substituting \(x = -3\) into equation (1): \[ 8z - 12(-3) = 4 \implies 8z + 36 = 4 \implies 8z = 4 - 36 \implies 8z = -32 \implies z = -4 \] ### Step 8: Write the magnetic field vector Now substituting \(x\) and \(z\) back into the magnetic field vector: \[ \vec{B} = -3 \hat{i} - 3 \hat{j} - 4 \hat{k} \] ### Final Answer Thus, the magnetic field vector is: \[ \vec{B} = -3.0 \hat{i} - 3.0 \hat{j} - 4.0 \hat{k} \, \text{T} \]
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