Let f(x) be a continuously differentiable function on the interval (0, ∞) such that f(1) = 2 and \(\lim\limits_{t→x}\frac{t^{10}f(x)-x^{10}f(t)}{t^9-x^9}=1\)
for each x > 0. Then, for all x > 0, f(x) is equal to
To solve the problem, we need to analyze the given limit condition and find the function \( f(x) \) satisfying it.
1. Understanding the limit expression:
Given:
\[ \lim_{t \to x} \frac{t^{10} f(x) - x^{10} f(t)}{t^9 - x^9} = 1 \] for each \( x > 0 \).
2. Rewrite the limit to use the derivative concept:
Notice the numerator and denominator both tend to zero as \( t \to x \). This suggests using the definition of derivative or applying algebraic manipulation.
3. Rewrite numerator and denominator:
\[ \frac{t^{10} f(x) - x^{10} f(t)}{t^9 - x^9} = \frac{t^{10} f(x) - x^{10} f(x) + x^{10} f(x) - x^{10} f(t)}{t^9 - x^9} = \frac{f(x)(t^{10} - x^{10}) - x^{10} (f(t) - f(x))}{t^9 - x^9} \]
4. Separate the fraction:
\[ = f(x) \frac{t^{10} - x^{10}}{t^9 - x^9} - x^{10} \frac{f(t) - f(x)}{t^9 - x^9} \]
5. Analyze the first fraction as \( t \to x \):
Since \( t \to x \), using derivative formulas:
\[ \lim_{t \to x} \frac{t^{10} - x^{10}}{t^9 - x^9} \] Both numerator and denominator tend to zero, apply L'Hôpital's Rule:
Derivative of numerator w.r.t. \( t \): \( 10 t^9 \)
Derivative of denominator w.r.t. \( t \): \( 9 t^8 \)
Thus, the limit is:
\[ \frac{10 x^9}{9 x^8} = \frac{10}{9} x \]
6. Analyze the second fraction as \( t \to x \):
\[ \lim_{t \to x} \frac{f(t) - f(x)}{t^9 - x^9} = \lim_{t \to x} \frac{f(t) - f(x)}{t - x} \cdot \frac{t - x}{t^9 - x^9} = f'(x) \cdot \lim_{t \to x} \frac{1}{9 t^8} = \frac{f'(x)}{9 x^8} \]
7. Substitute limits back:
\[ 1 = f(x) \times \frac{10}{9} x - x^{10} \times \frac{f'(x)}{9 x^8} = \frac{10}{9} x f(x) - \frac{x^2}{9} f'(x) \]
8. Multiply both sides by 9:
\[ 9 = 10 x f(x) - x^{2} f'(x) \]
9. Rearranged differential equation:
\[ x^{2} f'(x) + 9 = 10 x f(x) \] or \[ x^{2} f'(x) - 10 x f(x) = -9 \]
10. Divide both sides by \( x^2 \):
\[ f'(x) - \frac{10}{x} f(x) = -\frac{9}{x^2} \] This is a linear differential equation of the form:
\[ f'(x) + P(x) f(x) = Q(x) \] with \( P(x) = -\frac{10}{x} \) and \( Q(x) = -\frac{9}{x^2} \).
11. Find the integrating factor (IF):
\[ IF = e^{\int P(x) dx} = e^{\int -\frac{10}{x} dx} = e^{-10 \ln x} = x^{-10} \]
12. Multiply entire equation by integrating factor:
\[ x^{-10} f'(x) - \frac{10}{x} x^{-10} f(x) = -\frac{9}{x^2} x^{-10} \] which simplifies to \[ \frac{d}{dx} \left( x^{-10} f(x) \right) = -9 x^{-12} \]
13. Integrate both sides:
\[ \int \frac{d}{dx} \left( x^{-10} f(x) \right) dx = \int -9 x^{-12} dx \] \[ x^{-10} f(x) = -9 \int x^{-12} dx + C \] \[ = -9 \times \left( \frac{x^{-11}}{-11} \right) + C = \frac{9}{11} x^{-11} + C \]
14. Solve for \( f(x) \):
\[ f(x) = x^{10} \left( \frac{9}{11} x^{-11} + C \right) = \frac{9}{11} x^{-1} + C x^{10} \]
15. Use the initial condition \( f(1) = 2 \):
\[ f(1) = \frac{9}{11} (1)^{-1} + C (1)^{10} = \frac{9}{11} + C = 2 \] \[ C = 2 - \frac{9}{11} = \frac{22}{11} - \frac{9}{11} = \frac{13}{11} \]
Final form of \( f(x) \):
\[ \boxed{ f(x) = \frac{9}{11x} + \frac{13}{11} x^{10} } \]
Figure 1 shows the configuration of main scale and Vernier scale before measurement. Fig. 2 shows the configuration corresponding to the measurement of diameter $ D $ of a tube. The measured value of $ D $ is:
The center of a disk of radius $ r $ and mass $ m $ is attached to a spring of spring constant $ k $, inside a ring of radius $ R>r $ as shown in the figure. The other end of the spring is attached on the periphery of the ring. Both the ring and the disk are in the same vertical plane. The disk can only roll along the inside periphery of the ring, without slipping. The spring can only be stretched or compressed along the periphery of the ring, following Hooke’s law. In equilibrium, the disk is at the bottom of the ring. Assuming small displacement of the disc, the time period of oscillation of center of mass of the disk is written as $ T = \frac{2\pi}{\omega} $. The correct expression for $ \omega $ is ( $ g $ is the acceleration due to gravity):