To find the amount of electric charge that crosses through the wire in 20 seconds, we start with the relation given for current:
\(I = I_0 + \beta t\)
where \( I_0 = 20 \, \text{A} \) and \( \beta = 3 \, \text{A/s} \).
The electric charge \( Q \) that passes through the wire can be calculated using the formula:
\(Q = \int I \, dt\)
Substitute the expression for \( I \) into the integral:
\(Q = \int (I_0 + \beta t) \, dt\)
Evaluate the integral over the time interval from \( t = 0 \) to \( t = 20 \, \text{s} \):
\(Q = \int_0^{20} (20 + 3t) \, dt = [20t + \frac{3}{2}t^2]_0^{20}\)
Calculate the definite integral:
\(= \left( 20 \times 20 + \frac{3}{2} \times 20^2 \right) - \left( 20 \times 0 + \frac{3}{2} \times 0^2 \right)\)
\(= 400 + \frac{3}{2} \times 400\)
\(= 400 + 600\)
\(= 1000 \, \text{C}\)
Hence, the correct amount of electric charge that crosses through the wire in 20 seconds is 1000 C.
\[ I = I_0 + \beta t = 20 + 3t \]
The current \(I = \frac{dq}{dt}\), so we can write:
\[ dq = (20 + 3t) dt \]
\[ q = \int_{0}^{20} (20 + 3t) dt \]
Split the integral:
\[ q = \int_{0}^{20} 20 dt + \int_{0}^{20} 3t dt \]
\[ q = \left[20t\right]_{0}^{20} + \left[\frac{3t^2}{2}\right]_{0}^{20} \]
\[ = (20 \times 20) + \frac{3 \times 20^2}{2} \]
\[ = 400 + \frac{3 \times 400}{2} \]
\[ = 400 + 600 = 1000 \, C \]
So, the correct answer is: 1000 C
An infinitely long straight wire carrying current $I$ is bent in a planar shape as shown in the diagram. The radius of the circular part is $r$. The magnetic field at the centre $O$ of the circular loop is :

