Consider the sequence \( \{a_n\}_{n=0}^{\infty} \) defined by the recurrence relation:
\( a_{n+2} - 3a_{n+1} + 2a_n = 1, \quad a_0 = a_1 = 0 \)
The homogeneous part of the recurrence is:
\( a_{n+2} - 3a_{n+1} + 2a_n = 0 \)
Its characteristic equation is:
\( r^2 - 3r + 2 = 0 \)
Factoring, we get:
\( (r - 1)(r - 2) = 0 \)
Hence, the roots are \( r = 1 \) and \( r = 2 \), and the general solution of the homogeneous equation is:
\( a_n^{(h)} = A + B \cdot 2^n \)
Since the non-homogeneous term is a constant (1), we try a particular solution of the form:
\( a_n^{(p)} = C \cdot n \)
Substituting into the recurrence, we have:
\( C(n+2) - 3C(n+1) + 2Cn = Cn + 2C - 3Cn - 3C + 2Cn = -C \)
Setting \( -C = 1 \) gives \( C = -1 \). Thus, the particular solution is:
\( a_n^{(p)} = -n \)
The general solution is the sum of the homogeneous and particular solutions:
\( a_n = A + B \cdot 2^n - n \)
Using the initial conditions:
Subtracting the first equation from the second yields:
\( (A+2B) - (A+B) = B = 1 \)
Therefore, \( A = -1 \), and the closed-form expression for the sequence is:
\( a_n = 2^n - n - 1 \)
We wish to compute:
\( E = a_{25}a_{23} - 2a_{25}a_{22} - 2a_{23}a_{24} + 4a_{22}a_{24} \)
Notice that this expression factors as:
\( E = \bigl(a_{25} - 2a_{24}\bigr)\bigl(a_{23} - 2a_{22}\bigr) \)
Let’s simplify the term \( a_n - 2a_{n-1} \) using the closed form:
\( a_n - 2a_{n-1} = \Bigl(2^n - n - 1\Bigr) - 2\Bigl(2^{n-1} - (n-1) - 1\Bigr) \)
Expanding, we get:
\( = 2^n - n - 1 - 2^n + 2(n-1) + 2 = n - 1 \)
Therefore:
Thus, the expression simplifies to:
\( E = 24 \times 22 = 528 \)
The value of the expression is 528.
Match List - I with List - II:
List - I:
(A) Electric field inside (distance \( r > 0 \) from center) of a uniformly charged spherical shell with surface charge density \( \sigma \), and radius \( R \).
(B) Electric field at distance \( r > 0 \) from a uniformly charged infinite plane sheet with surface charge density \( \sigma \).
(C) Electric field outside (distance \( r > 0 \) from center) of a uniformly charged spherical shell with surface charge density \( \sigma \), and radius \( R \).
(D) Electric field between two oppositely charged infinite plane parallel sheets with uniform surface charge density \( \sigma \).
List - II:
(I) \( \frac{\sigma}{\epsilon_0} \)
(II) \( \frac{\sigma}{2\epsilon_0} \)
(III) 0
(IV) \( \frac{\sigma}{\epsilon_0 r^2} \) Choose the correct answer from the options given below:
Consider the following statements:
A. Surface tension arises due to extra energy of the molecules at the interior as compared to the molecules at the surface of a liquid.
B. As the temperature of liquid rises, the coefficient of viscosity increases.
C. As the temperature of gas increases, the coefficient of viscosity increases.
D. The onset of turbulence is determined by Reynolds number.
E. In a steady flow, two streamlines never intersect.
Choose the correct answer from the options given below:
Ordinary Differential Equations is an equation that indicates the relation of having one independent variable x, and one dependent variable y, along with some of its other derivatives.
\(F(\frac{dy}{dt},y,t) = 0\)
A partial differential equation is a type, in which the equation carries many unknown variables with their partial derivatives.
It is the linear polynomial equation in which derivatives of different variables exist. Linear Partial Differential Equation derivatives are partial and function is dependent on the variable.
When the degree of f(x,y) and g(x,y) is the same, it is known to be a homogeneous differential equation.
\(\frac{dy}{dx} = \frac{a_1x + b_1y + c_1}{a_2x + b_2y + c_2}\)
Read More: Differential Equations