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Let f: R rarr R be a continuous function...

Let `f: R rarr R` be a continuous function satisfying `f(x)+ f(x+ k) = n`, for all `x in R` where `k gt 0` and n is a positive integer. If `I_(1)= int_(0)^(4nk) f(x) dx and I_(2)= int_(-k)^(3k) f(x) dx`, then:

A

`I_(1) + 2I_(2)= 4nk`

B

`I_(1) + 2I_(2)= 2nk`

C

`I_(1) + n I_(2)= 4n^(2)k`

D

`I_(1) + nI_(2)= 6n^(2)k`

Text Solution

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The correct Answer is:
To solve the problem, we start with the given condition for the function \( f \): 1. **Given Condition**: \[ f(x) + f(x+k) = n \] for all \( x \in \mathbb{R} \), where \( k > 0 \) and \( n \) is a positive integer. 2. **Periodicity of the Function**: From the given condition, we can derive that: \[ f(x) + f(x+k) = n \quad \text{(1)} \] Replacing \( x \) with \( x+k \) in (1): \[ f(x+k) + f(x+2k) = n \quad \text{(2)} \] Replacing \( x \) with \( x+2k \) in (1): \[ f(x+2k) + f(x+3k) = n \quad \text{(3)} \] Continuing this process, we can observe that the function \( f \) is periodic with period \( 2k \). Therefore, we can express \( f(x) \) in terms of its values over one period. 3. **Integrals**: We define the integrals: \[ I_1 = \int_0^{4nk} f(x) \, dx \] \[ I_2 = \int_{-k}^{3k} f(x) \, dx \] 4. **Calculating \( I_1 \)**: Since \( f \) is periodic with period \( 2k \), we can break down \( I_1 \): \[ I_1 = \int_0^{4nk} f(x) \, dx = 2n \int_0^{2k} f(x) \, dx \] This is because \( 4nk \) can be divided into two full periods of \( 2k \). 5. **Calculating \( I_2 \)**: For \( I_2 \): \[ I_2 = \int_{-k}^{3k} f(x) \, dx \] We can split this integral into two parts: \[ I_2 = \int_{-k}^{0} f(x) \, dx + \int_{0}^{2k} f(x) \, dx + \int_{2k}^{3k} f(x) \, dx \] The integral from \( 2k \) to \( 3k \) can be transformed using the periodicity: \[ \int_{2k}^{3k} f(x) \, dx = \int_{0}^{k} f(x) \, dx \] Thus, we have: \[ I_2 = \int_{-k}^{0} f(x) \, dx + \int_{0}^{2k} f(x) \, dx + \int_{0}^{k} f(x) \, dx \] The integral from \( -k \) to \( 0 \) can also be transformed using periodicity: \[ \int_{-k}^{0} f(x) \, dx = \int_{k}^{0} f(x) \, dx = \int_{0}^{k} f(x) \, dx \] Therefore: \[ I_2 = 2 \int_{0}^{k} f(x) \, dx + \int_{0}^{2k} f(x) \, dx \] 6. **Final Calculation**: Now, we can express both integrals in terms of \( n \): - From the periodicity and the original condition, we find: \[ \int_{0}^{k} f(x) \, dx = \frac{nk}{2} \] - Thus: \[ I_1 = 2n \cdot 2 \cdot \frac{nk}{2} = 2n^2 k \] \[ I_2 = 2 \cdot \frac{nk}{2} + 2n \cdot k = 2nk \] 7. **Conclusion**: Therefore, we have: \[ I_1 = 2n^2 k \quad \text{and} \quad I_2 = 2nk \] The final result shows that \( I_1 \) and \( I_2 \) are related through their expressions, confirming the periodic nature of \( f \).
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