\[ I = I_0 + \beta t = 20 + 3t \]
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
Two cells of emf 1V and 2V and internal resistance 2 \( \Omega \) and 1 \( \Omega \), respectively, are connected in series with an external resistance of 6 \( \Omega \). The total current in the circuit is \( I_1 \). Now the same two cells in parallel configuration are connected to the same external resistance. In this case, the total current drawn is \( I_2 \). The value of \( \left( \frac{I_1}{I_2} \right) \) is \( \frac{x}{3} \). The value of x is 1cm.
Current passing through a wire as function of time is given as $I(t)=0.02 \mathrm{t}+0.01 \mathrm{~A}$. The charge that will flow through the wire from $t=1 \mathrm{~s}$ to $\mathrm{t}=2 \mathrm{~s}$ is: