To solve this problem, we want to find the probability that \( i^{k_1} + i^{k_2} \neq 0 \) for natural numbers \( k_1 \) and \( k_2 \). This is equivalent to finding the probability that \( i^{k_1} \neq -i^{k_2} \).
1. Determine the possible values of \( i^k \):
The possible values of \( i^k \) for any natural number \( k \) are \( \{i, -1, -i, 1\} \). Specifically, \( i^k \) depends on \( k \pmod{4} \):
\( i^k = \begin{cases} 1 & \text{if } k \equiv 0 \pmod{4} \\ i & \text{if } k \equiv 1 \pmod{4} \\ -1 & \text{if } k \equiv 2 \pmod{4} \\ -i & \text{if } k \equiv 3 \pmod{4} \end{cases} \)
2. Find when \( i^{k_1} + i^{k_2} = 0 \):
We have \( i^{k_1} + i^{k_2} = 0 \) if and only if \( i^{k_1} = -i^{k_2} \). This means that \( i^{k_1} \) and \( i^{k_2} \) must be opposite values. The possible pairs of opposite values are \( (i, -i) \) and \( (1, -1) \).
3. Calculate the probability of \( i^{k_1} = -i^{k_2} \):
We want to find the probability that \( i^{k_1} \) and \( i^{k_2} \) are not opposites. Consider the possible values of \( k_1 \pmod{4} \). For each value of \( k_1 \pmod{4} \), we determine the value of \( k_2 \pmod{4} \) that makes \( i^{k_1} = -i^{k_2} \).
In each case, there is exactly one value of \( k_2 \pmod{4} \) that makes \( i^{k_1} = -i^{k_2} \). Since there are 4 possible values for \( k_2 \pmod{4} \), the probability that \( i^{k_1} = -i^{k_2} \) is \( \frac{1}{4} \).
4. Calculate the probability of \( i^{k_1} \neq -i^{k_2} \):
The probability that \( i^{k_1} \neq -i^{k_2} \) is \( 1 - \frac{1}{4} = \frac{3}{4} \).
Final Answer:
The probability that \( i^{k_1} + i^{k_2} \neq 0 \) is \( {\frac{3}{4}} \).
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 : \(A_2 \rightleftharpoons 2A\)
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,