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
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,




What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)