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A uniform magnetic field B = 1.2 mT is d...

A uniform magnetic field `B = 1.2` mT is directed vertically upward throughout the volume of a laboratory chamber . A proton (`m_(p) = 1.67 xx 10^(-27)` kg) enters the laboratory horizontally from south to north. Calculate the magnitude of centripetal acceleration of the proton if its speed is `3 xx 10^(7)` m/s

A

`3.45 xx 10^(12) m//s^(2)`

B

`1.67 xx 10^(12) m//s^(2)`

C

`5.25 xx 10^(12) m//s^(2)`

D

`2.75 xx 10^(12) m//s^(2)`

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To solve the problem of calculating the magnitude of centripetal acceleration of a proton moving in a magnetic field, we will follow these steps: ### Step 1: Understand the Given Information We have the following information: - Magnetic field strength, \( B = 1.2 \, \text{mT} = 1.2 \times 10^{-3} \, \text{T} \) - Mass of the proton, \( m_p = 1.67 \times 10^{-27} \, \text{kg} \) - Speed of the proton, \( v = 3 \times 10^7 \, \text{m/s} \) ### Step 2: Calculate the Charge of the Proton The charge of a proton is a known constant: - Charge of the proton, \( q = 1.6 \times 10^{-19} \, \text{C} \) ### Step 3: Determine the Centripetal Force When a charged particle moves in a magnetic field, it experiences a magnetic force given by: \[ F = qvB \] This force acts as the centripetal force required to keep the proton moving in a circular path. Therefore, we can equate the magnetic force to the centripetal force: \[ F = \frac{mv^2}{r} \] Where \( r \) is the radius of the circular path. ### Step 4: Relate the Forces Setting the magnetic force equal to the centripetal force, we have: \[ qvB = \frac{mv^2}{r} \] ### Step 5: Solve for Centripetal Acceleration Centripetal acceleration \( a_c \) can be expressed as: \[ a_c = \frac{v^2}{r} \] From the previous equation, we can express \( r \) in terms of \( q, v, B, \) and \( m \): \[ r = \frac{mv}{qB} \] Substituting \( r \) into the centripetal acceleration formula gives: \[ a_c = \frac{v^2}{\frac{mv}{qB}} = \frac{qvB}{m} \] ### Step 6: Substitute the Values Now we can substitute the known values into the equation: \[ a_c = \frac{(1.6 \times 10^{-19} \, \text{C})(3 \times 10^7 \, \text{m/s})(1.2 \times 10^{-3} \, \text{T})}{1.67 \times 10^{-27} \, \text{kg}} \] ### Step 7: Calculate the Result Calculating the numerator: \[ 1.6 \times 10^{-19} \times 3 \times 10^7 \times 1.2 \times 10^{-3} = 5.76 \times 10^{-15} \] Now, dividing by the mass of the proton: \[ a_c = \frac{5.76 \times 10^{-15}}{1.67 \times 10^{-27}} \approx 3.44 \times 10^{12} \, \text{m/s}^2 \] ### Final Answer The magnitude of the centripetal acceleration of the proton is: \[ \boxed{3.44 \times 10^{12} \, \text{m/s}^2} \]

To solve the problem of calculating the magnitude of centripetal acceleration of a proton moving in a magnetic field, we will follow these steps: ### Step 1: Understand the Given Information We have the following information: - Magnetic field strength, \( B = 1.2 \, \text{mT} = 1.2 \times 10^{-3} \, \text{T} \) - Mass of the proton, \( m_p = 1.67 \times 10^{-27} \, \text{kg} \) - Speed of the proton, \( v = 3 \times 10^7 \, \text{m/s} \) ...
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