Radioactive Decay Constant: The radioactive decay of a material follows the formula: N(t) = N0 \(\times\) \(\text{e}^{(-\lambda t)}\), where N(t) is the activity at time t, N0 is the initial activity,\(\lambda\) is the decay constant, and t is time.
If R1 is the activity at time t1 and R2 is the activity at time t2, we have:
R1 = N0 \(\times\) \(\text{e}^{(-\lambda t_1)}\)
R2 = N0 \(\times\) \(\text{e}^{(-\lambda t_2)}\)
Dividing these equations: \(\frac{\text{R}_1}{\text{R}_2}\) = \(\frac{\text{e}^{(-\lambda t_1)}}{\text{e}^{(-\lambda t_2)}}\)= \(\text{e}^{(-\lambda(t_1-t_2))}\)
So, the correct option is R1 = R2 \(\text{e}^{-\lambda(t_1-t_2)}\)
The current passing through the battery in the given circuit, is:
A bob of heavy mass \(m\) is suspended by a light string of length \(l\). The bob is given a horizontal velocity \(v_0\) as shown in figure. If the string gets slack at some point P making an angle \( \theta \) from the horizontal, the ratio of the speed \(v\) of the bob at point P to its initial speed \(v_0\) is :
A full wave rectifier circuit with diodes (\(D_1\)) and (\(D_2\)) is shown in the figure. If input supply voltage \(V_{in} = 220 \sin(100 \pi t)\) volt, then at \(t = 15\) msec:
In the year 1911, Rutherford discovered the atomic nucleus along with his associates. It is already known that every atom is manufactured of positive charge and mass in the form of a nucleus that is concentrated at the center of the atom. More than 99.9% of the mass of an atom is located in the nucleus. Additionally, the size of the atom is of the order of 10-10 m and that of the nucleus is of the order of 10-15 m.
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