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$M=\left\{x \in I_{2}: \quad x=\left(x_{1}, x_{2}, \ldots, x_{n}, \ldots\right)...
Jun 28, 2024
Solution by Steps
step 1
We are given the set MM defined as M={xI2:x=(x1,x2,,xn,),xn1n,n=1,2,}M=\left\{x \in I_{2}: \quad x=\left(x_{1}, x_{2}, \ldots, x_{n}, \ldots\right), \quad\left|x_{n}\right| \leq \frac{1}{\sqrt{n}}, \quad n=1,2, \ldots\right\}
step 2
To understand the set MM, we need to analyze the condition xn1n\left|x_{n}\right| \leq \frac{1}{\sqrt{n}}. This means that for each component xnx_n of the vector xx, the absolute value of xnx_n must be less than or equal to 1n\frac{1}{\sqrt{n}}
step 3
The set MM is a subset of I2I_2, where I2I_2 is likely a space of sequences or vectors. Each xMx \in M is a sequence (x1,x2,)(x_1, x_2, \ldots) such that the nn-th component xnx_n satisfies xn1n\left|x_{n}\right| \leq \frac{1}{\sqrt{n}}
step 4
Therefore, MM consists of all sequences in I2I_2 where each term xnx_n is bounded by 1n\frac{1}{\sqrt{n}}
Answer
MM is the set of all sequences in I2I_2 where each term xnx_n satisfies xn1n\left|x_{n}\right| \leq \frac{1}{\sqrt{n}}.
Key Concept
Set Definition
Explanation
The set MM is defined by a condition on the components of the sequences it contains, specifically that each component xnx_n must be less than or equal to 1n\frac{1}{\sqrt{n}} in absolute value.
Solution by Steps
step 1
We are given the operator A:C[0,π2]C[0,π2]A: C\left[0, \frac{\pi}{2}\right] \mapsto C\left[0, \frac{\pi}{2}\right] defined by the formula Ax(t)=0π2sin(t+s)x(s)dsA x(t)=\int_{0}^{\frac{\pi}{2}} \sin (t+s) x(s) d s
step 2
To find the norm of the operator AA, we need to determine A=supx1Ax\|A\| = \sup_{\|x\| \leq 1} \|Ax\|
step 3
Consider the function x(s)=1x(s) = 1 for s[0,π2]s \in \left[0, \frac{\pi}{2}\right]. Then, Ax(t)=0π2sin(t+s)dsAx(t) = \int_{0}^{\frac{\pi}{2}} \sin(t+s) ds
step 4
Evaluate the integral: Ax(t)=0π2sin(t+s)ds=[cos(t+s)]0π2=cos(t+π2)+cos(t)Ax(t) = \int_{0}^{\frac{\pi}{2}} \sin(t+s) ds = \left[-\cos(t+s)\right]_{0}^{\frac{\pi}{2}} = -\cos(t+\frac{\pi}{2}) + \cos(t)
step 5
Simplify the expression: Ax(t)=cos(t+π2)+cos(t)=(sin(t))+cos(t)=sin(t)+cos(t)Ax(t) = -\cos(t+\frac{\pi}{2}) + \cos(t) = -(-\sin(t)) + \cos(t) = \sin(t) + \cos(t)
step 6
The maximum value of sin(t)+cos(t)\sin(t) + \cos(t) on [0,π2]\left[0, \frac{\pi}{2}\right] is 2\sqrt{2}, which occurs when t=π4t = \frac{\pi}{4}
step 7
Therefore, Ax=2\|Ax\| = \sqrt{2} when x=1\|x\| = 1. Hence, the norm of the operator AA is A=2\|A\| = \sqrt{2}
Answer
The norm of the operator AA is 2\sqrt{2}.
Key Concept
Operator Norm
Explanation
The norm of an operator AA is the supremum of Ax\|Ax\| over all xx with x1\|x\| \leq 1. In this case, we evaluated the integral and found the maximum value of the resulting function to determine the norm.
Solution by Steps
step 1
We need to find the projection of the function x(t)=2t1x(t) = 2t - 1 onto the subspace V1V_1 of all polynomials of degree less than or equal to 1 in the space L2(0,1)L^2(0,1). The subspace V1V_1 is defined as V1={p(t)=a1t+a0a0,a1 are constants}V_1 = \{ p(t) = a_1 t + a_0 \mid a_0, a_1 \text{ are constants} \}
step 2
The projection of x(t)x(t) onto V1V_1 is given by the polynomial p(t)=a1t+a0p(t) = a_1 t + a_0 that minimizes the norm x(t)p(t)L2(0,1)\| x(t) - p(t) \|_{L^2(0,1)}
step 3
To find a0a_0 and a1a_1, we need to solve the following system of equations obtained by setting the inner products x(t)p(t),1L2(0,1)=0\langle x(t) - p(t), 1 \rangle_{L^2(0,1)} = 0 and x(t)p(t),tL2(0,1)=0\langle x(t) - p(t), t \rangle_{L^2(0,1)} = 0
step 4
Calculate x(t)p(t),1L2(0,1)=01(2t1a1ta0)dt=0\langle x(t) - p(t), 1 \rangle_{L^2(0,1)} = \int_0^1 (2t - 1 - a_1 t - a_0) \, dt = 0
step 5
Simplify the integral: 01(2t1a1ta0)dt=01(2ta1t1a0)dt=01((2a1)t1a0)dt\int_0^1 (2t - 1 - a_1 t - a_0) \, dt = \int_0^1 (2t - a_1 t - 1 - a_0) \, dt = \int_0^1 ((2 - a_1)t - 1 - a_0) \, dt
step 6
Evaluate the integral: 01((2a1)t1a0)dt=[(2a1)t22(1+a0)t]01=2a12(1+a0)=0\int_0^1 ((2 - a_1)t - 1 - a_0) \, dt = \left[ \frac{(2 - a_1)t^2}{2} - (1 + a_0)t \right]_0^1 = \frac{2 - a_1}{2} - (1 + a_0) = 0
step 7
Solve for a0a_0: 2a121a0=0    2a12=1+a0    2a1=2+2a0    a1=2a0    a1=2a0\frac{2 - a_1}{2} - 1 - a_0 = 0 \implies \frac{2 - a_1}{2} = 1 + a_0 \implies 2 - a_1 = 2 + 2a_0 \implies -a_1 = 2a_0 \implies a_1 = -2a_0
step 8
Calculate x(t)p(t),tL2(0,1)=01t(2t1a1ta0)dt=0\langle x(t) - p(t), t \rangle_{L^2(0,1)} = \int_0^1 t(2t - 1 - a_1 t - a_0) \, dt = 0
step 9
Simplify the integral: 01t(2t1a1ta0)dt=01(2t2ta1t2a0t)dt=01((2a1)t2ta0t)dt\int_0^1 t(2t - 1 - a_1 t - a_0) \, dt = \int_0^1 (2t^2 - t - a_1 t^2 - a_0 t) \, dt = \int_0^1 ((2 - a_1)t^2 - t - a_0 t) \, dt
step 10
Evaluate the integral: 01((2a1)t2ta0t)dt=[(2a1)t33t22a0t22]01=2a1312a02=0\int_0^1 ((2 - a_1)t^2 - t - a_0 t) \, dt = \left[ \frac{(2 - a_1)t^3}{3} - \frac{t^2}{2} - \frac{a_0 t^2}{2} \right]_0^1 = \frac{2 - a_1}{3} - \frac{1}{2} - \frac{a_0}{2} = 0
step 11
Solve for a0a_0: 2a1312a02=0    2a13=12+a02    2a1=32+3a02    42a1=3+3a0    12a1=3a0\frac{2 - a_1}{3} - \frac{1}{2} - \frac{a_0}{2} = 0 \implies \frac{2 - a_1}{3} = \frac{1}{2} + \frac{a_0}{2} \implies 2 - a_1 = \frac{3}{2} + \frac{3a_0}{2} \implies 4 - 2a_1 = 3 + 3a_0 \implies 1 - 2a_1 = 3a_0
step 12
Substitute a1=2a0a_1 = -2a_0 into the equation: 12(2a0)=3a0    1+4a0=3a0    1=a0    a0=11 - 2(-2a_0) = 3a_0 \implies 1 + 4a_0 = 3a_0 \implies 1 = -a_0 \implies a_0 = -1
step 13
Substitute a0=1a_0 = -1 into a1=2a0a_1 = -2a_0: a1=2(1)=2a_1 = -2(-1) = 2
step 14
The projection of x(t)=2t1x(t) = 2t - 1 onto V1V_1 is p(t)=a1t+a0=2t1p(t) = a_1 t + a_0 = 2t - 1
Answer
The projection of x(t)=2t1x(t) = 2t - 1 onto V1V_1 is p(t)=2t1p(t) = 2t - 1.
Key Concept
Projection of a function onto a subspace
Explanation
The projection of a function onto a subspace minimizes the distance between the function and the subspace, and is found by solving for the coefficients that satisfy the orthogonality conditions.
Solution by Steps
step 1
The problem involves understanding the space L2(0,1)L^{2}(0,1). This space consists of all square-integrable functions on the interval (0,1)(0,1)
step 2
A function ff belongs to L2(0,1)L^{2}(0,1) if \int_{0}^{1} |f(x)|^2 \, dx < \infty
step 3
The notation (Δf)20,1(\Delta f)^{2 {0, 1}} suggests a squared difference or a squared norm in the context of L2(0,1)L^{2}(0,1)
step 4
The expression {1,(Δf)2}\{1, (\Delta f)^2\} indicates a set containing the number 1 and the squared difference (Δf)2(\Delta f)^2
Answer
The space L2(0,1)L^{2}(0,1) consists of all functions whose square is integrable over the interval (0,1)(0,1).
Key Concept
L2(0,1)L^{2}(0,1) space
Explanation
L2(0,1)L^{2}(0,1) is a function space where the integral of the square of the function over the interval (0,1)(0,1) is finite.
Solution by Steps
step 1
We need to determine if the sequence xn=(1,12,122,,12n1,0,0,)x_n = \left(1, \frac{1}{2}, \frac{1}{2^2}, \cdots, \frac{1}{2^{n-1}}, 0, 0, \ldots\right) converges in the space I2I_2
step 2
The space I2I_2 consists of all sequences (an)(a_n) such that the series n=1an2\sum_{n=1}^{\infty} |a_n|^2 converges
step 3
For the given sequence xnx_n, we need to check if k=1(12k1)2\sum_{k=1}^{\infty} \left(\frac{1}{2^{k-1}}\right)^2 converges
step 4
Simplifying the series, we get k=1(12k1)2=k=114k1\sum_{k=1}^{\infty} \left(\frac{1}{2^{k-1}}\right)^2 = \sum_{k=1}^{\infty} \frac{1}{4^{k-1}}
step 5
This is a geometric series with the first term a=1a = 1 and common ratio r=14r = \frac{1}{4}
step 6
A geometric series k=0ark\sum_{k=0}^{\infty} ar^k converges if |r| < 1. Here, |r| = \frac{1}{4} < 1, so the series converges
step 7
Therefore, k=114k1\sum_{k=1}^{\infty} \frac{1}{4^{k-1}} converges, implying that the sequence xnx_n converges in the space I2I_2
Answer
The sequence xnx_n converges in the space I2I_2.
Key Concept
Convergence in I2I_2 space
Explanation
A sequence converges in the I2I_2 space if the series of the squares of its terms converges.
Solution by Steps
step 1
We need to determine the relative compactness of the set AA in the space l2l_{2}. The set AA is defined as A=\left\{x \in l_{2}: x=\left(x_{1}, x_{2}, \ldots, x_{n}, \ldots\right), \left|x_{n}\right|<n \text{ for } n=1,2, \ldots, 10, \left|x_{n}\right| \leq \frac{1}{n} \text{ for } n>10\right\}
step 2
To check for relative compactness in l2l_{2}, we need to verify if the set AA is totally bounded. A set is totally bounded if for every \epsilon > 0, there exists a finite number of balls of radius ϵ\epsilon that cover the set
step 3
Consider the elements xAx \in A. For n10n \leq 10, \left|x_{n}\right| < n. For n > 10, xn1n\left|x_{n}\right| \leq \frac{1}{n}
step 4
We need to show that the sequence {xn}\{x_n\} is bounded in l2l_{2}. For n10n \leq 10, \left|x_{n}\right| < n implies that \sum_{n=1}^{10} \left|x_{n}\right|^2 < \sum_{n=1}^{10} n^2
step 5
For n > 10, xn1n\left|x_{n}\right| \leq \frac{1}{n} implies that n=11xn2n=11(1n)2\sum_{n=11}^{\infty} \left|x_{n}\right|^2 \leq \sum_{n=11}^{\infty} \left(\frac{1}{n}\right)^2
step 6
The series n=11(1n)2\sum_{n=11}^{\infty} \left(\frac{1}{n}\right)^2 converges because it is a p-series with p=2 > 1
step 7
Therefore, n=1xn2\sum_{n=1}^{\infty} \left|x_{n}\right|^2 is bounded, which implies that the set AA is bounded in l2l_{2}
step 8
Since AA is bounded and the space l2l_{2} is a Hilbert space, the set AA is relatively compact if it is totally bounded
step 9
To show that AA is totally bounded, we need to cover AA with a finite number of balls of radius ϵ\epsilon. Given the boundedness of AA, we can find such a finite cover
step 10
Hence, the set AA is relatively compact in the space l2l_{2}
Answer
The set AA is relatively compact in the space l2l_{2}.
Key Concept
Relative Compactness
Explanation
Relative compactness in l2l_{2} involves showing that the set is totally bounded, which means it can be covered by a finite number of balls of any given radius.
Solution by Steps
step 1
We start with the given integral expression for the operator AA: Ax(1)=12t+sx(s)dsA x(1) = \int_{1}^{2} \sqrt{t+s} x(s) \, ds
step 2
To find the norm of the operator AA, we need to evaluate the integral and then determine the supremum of the resulting expression
step 3
First, we evaluate the integral 12t+sx(s)ds\int_{1}^{2} \sqrt{t+s} x(s) \, ds
step 4
Assuming x(s)x(s) is a function from reals to reals, we can write the norm of the operator AA as: A=12t+sx(s)ds\|A\| = \left\| \int_{1}^{2} \sqrt{t+s} x(s) \, ds \right\|
step 5
The norm of the operator AA is given by the absolute value of the integral: A=12t+sx(s)ds\|A\| = \left| \int_{1}^{2} \sqrt{t+s} x(s) \, ds \right|
step 6
To find the supremum, we consider the maximum value of the integral over all possible functions x(s)x(s) in the given space
step 7
Therefore, the norm of the operator AA is: A=supx(s)12t+sx(s)ds\|A\| = \sup_{x(s)} \left| \int_{1}^{2} \sqrt{t+s} x(s) \, ds \right|
Answer
A=supx(s)12t+sx(s)ds\|A\| = \sup_{x(s)} \left| \int_{1}^{2} \sqrt{t+s} x(s) \, ds \right|
Key Concept
Norm of an Operator
Explanation
The norm of an operator is determined by evaluating the integral and finding the supremum of the resulting expression over all possible functions in the given space.
Generated Graph
Solution by Steps
step 1
We start by integrating the given function (a1t+a0)2(a_1 t + a_0)^2 with respect to tt from t=0t=0 to t=1t=1
step 2
The integral is 01(a1t+a0)2dt\int_0^1 (a_1 t + a_0)^2 \, dt
step 3
Expanding the integrand, we get (a1t+a0)2=a12t2+2a1a0t+a02(a_1 t + a_0)^2 = a_1^2 t^2 + 2 a_1 a_0 t + a_0^2
step 4
Now, integrate each term separately: 01a12t2dt+012a1a0tdt+01a02dt. \int_0^1 a_1^2 t^2 \, dt + \int_0^1 2 a_1 a_0 t \, dt + \int_0^1 a_0^2 \, dt.
step 5
The integrals are: 01a12t2dt=a123,012a1a0tdt=a1a0,01a02dt=a02. \int_0^1 a_1^2 t^2 \, dt = \frac{a_1^2}{3}, \quad \int_0^1 2 a_1 a_0 t \, dt = a_1 a_0, \quad \int_0^1 a_0^2 \, dt = a_0^2.
step 6
Adding these results, we get: 01(a1t+a0)2dt=a123+a1a0+a02. \int_0^1 (a_1 t + a_0)^2 \, dt = \frac{a_1^2}{3} + a_1 a_0 + a_0^2.
Answer
01(a1t+a0)2dt=a123+a1a0+a02\int_0^1 (a_1 t + a_0)^2 \, dt = \frac{a_1^2}{3} + a_1 a_0 + a_0^2
Key Concept
Integration of a polynomial function
Explanation
The integral of a polynomial function can be found by integrating each term separately and then summing the results.
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