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Differential Equations question

2024 · 1 Feb · Shift 2 · Q44
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  5. /2024 · 1 Feb · Shift 2 · Q44

Differential Equations question

2024 · 1 Feb · Shift 2 · Q44

JEE MainMathematicsDifferential EquationsMCQ+4 / −1
Let α\alphaα be a non-zero real number. Suppose f:R→Rf: \mathbf{R} \rightarrow \mathbf{R}f:R→R is a differentiable function such that f(0)=2f(0)=2f(0)=2 and lim⁡x→−∞f(x)=1\lim\limits_{x \rightarrow-\infty} f(x)=1x→−∞lim​f(x)=1. If f′(x)=αf(x)+3f^{\prime}(x)=\alpha f(x)+3f′(x)=αf(x)+3, for all x∈Rx \in \mathbf{R}x∈R, then f(−log⁡e2)f\left(-\log _{\mathrm{e}} 2\right)f(−loge​2) is equal to :
  1. A
    7
  2. B
    9
  3. C
    3
  4. D
    5
View written solutionFree

Correct answer: B

  1. We need to solve the differential equation f′(x)=αf(x)+3,f'(x)=\alpha f(x)+3,f′(x)=αf(x)+3, with f(0)=2,lim⁡x→−∞f(x)=1,f(0)=2, \qquad \lim_{x\to -\infty} f(x)=1,f(0)=2,limx→−∞​f(x)=1, where α≠0\alpha\neq 0α=0 is real.

  2. Rewrite the differential equation in standard linear form: f′(x)−αf(x)=3.f'(x)-\alpha f(x)=3.f′(x)−αf(x)=3.

  3. First find the general solution.

    The homogeneous equation is fh′(x)−αfh(x)=0,f_h'(x)-\alpha f_h(x)=0,fh′​(x)−αfh​(x)=0, whose solution is fh(x)=Ceαx.f_h(x)=Ce^{\alpha x}.fh​(x)=Ceαx.

    For a particular solution, try a constant fp(x)=kf_p(x)=kfp​(x)=k. Then fp′(x)=0f_p'(x)=0fp′​(x)=0, so 0=αk+3  ⟹  k=−3α.0=\alpha k+3 \implies k=-\frac{3}{\alpha}.0=αk+3⟹k=−α3​.

    Hence the general solution is f(x)=Ceαx−3α.f(x)=Ce^{\alpha x}-\frac{3}{\alpha}.f(x)=Ceαx−α3​.

  4. Use the condition lim⁡x→−∞f(x)=1.\lim_{x\to -\infty} f(x)=1.limx→−∞​f(x)=1.

    Now, f(x)=Ceαx−3α.f(x)=Ce^{\alpha x}-\frac{3}{\alpha}.f(x)=Ceαx−α3​.

    For the limit as x→−∞x\to -\inftyx→−∞ to be finite, we must have α>0\alpha>0α>0; otherwise eαxe^{\alpha x}eαx would blow up as x→−∞x\to -\inftyx→−∞ unless C=0C=0C=0, which would conflict with the initial condition later.

    So for α>0\alpha>0α>0, eαx→0as x→−∞.e^{\alpha x}\to 0 \quad \text{as } x\to -\infty.eαx→0as x→−∞. Therefore, lim⁡x→−∞f(x)=−3α=1.\lim_{x\to -\infty} f(x)=-\frac{3}{\alpha}=1.limx→−∞​f(x)=−α3​=1.

    Hence, α=−3.\alpha=-3.α=−3.

  5. But this seems to contradict the requirement α>0\alpha>0α>0. So let us check more carefully by using the limit condition directly in the differential equation.

    If f(x)→1f(x)\to 1f(x)→1 as x→−∞x\to -\inftyx→−∞, then intuitively f′(x)→0f'(x)\to 0f′(x)→0 there, and from f′(x)=αf(x)+3,f'(x)=\alpha f(x)+3,f′(x)=αf(x)+3, we get 0=α(1)+3,0=\alpha(1)+3,0=α(1)+3, so α=−3.\alpha=-3.α=−3.

    Now solve with α=−3\alpha=-3α=−3: f′(x)=−3f(x)+3.f'(x)=-3f(x)+3.f′(x)=−3f(x)+3. Rewrite as f′(x)+3f(x)=3.f'(x)+3f(x)=3.f′(x)+3f(x)=3.

  6. Solve this equation.

    The homogeneous solution is fh(x)=Ce−3x.f_h(x)=Ce^{-3x}.fh​(x)=Ce−3x.

    A constant particular solution fp=kf_p=kfp​=k gives 0+3k=3  ⟹  k=1.0+3k=3 \implies k=1.0+3k=3⟹k=1.

    Thus, f(x)=Ce−3x+1.f(x)=Ce^{-3x}+1.f(x)=Ce−3x+1.

  7. Use f(0)=2f(0)=2f(0)=2: 2=C+1  ⟹  C=1.2=C+1 \implies C=1.2=C+1⟹C=1. Therefore, f(x)=e−3x+1.f(x)=e^{-3x}+1.f(x)=e−3x+1.

  8. Now compute f(−ln⁡2)f(-\ln 2)f(−ln2): f(−ln⁡2)=e−3(−ln⁡2)+1=e3ln⁡2+1=23+1=8+1=9.f(-\ln 2)=e^{-3(-\ln 2)}+1=e^{3\ln 2}+1=2^3+1=8+1=9.f(−ln2)=e−3(−ln2)+1=e3ln2+1=23+1=8+1=9.

  9. Check options:

    • A: 777
    • B: 999 ✅
    • C: 333
    • D: 555

So the correct answer is B.

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