A A 2 K
Author: c | 2025-04-23
= 0 k 2 k 2 k 3 k k 2 2 k 2 7 k 2 k = 1 ⇒ 10 k 2 9 k = 1 ⇒ 10 k 2 9 k − 1 = 0 ⇒ (10 k − 1) (k 1) = 0 ⇒ k = − 1, 1 10 It is known that probability of any observation must always
Factor k^2-k-2
K − 1 ) + a 2 · φ CO ( k − 1 ) + a 3 · φ CO 2 ( k − 1 ) + a 4 · φ CH 4 ( k − 1 ) + a 5 · T max ( k − 1 ) , (8) u 2 ≡ V O 2 ( k ) = a 0 + a 1 · V air ( k − 1 ) V O 2 ( k − 1 ) + a 2 · φ CO ( k − 1 ) + a 3 · φ CO 2 ( k − 1 ) + a 4 · φ CH 4 ( k − 1 ) + a 5 · T max ( k − 1 ) . (9) The third model type aims to achieve the necessary temperature for syngas production. The models regarding the ratio of gasification agents and the maximum temperature T m a x in the channel are in the linear and quadratic form. The structure of the model is as the following [25]: u 1 ≡ V air ( k ) = a 0 + a 1 · V air ( k − 1 ) V O 2 ( k − 1 ) + a 2 · T max ( k − 1 ) + a 3 T max 2 ( k − 1 ) , (10) u 2 ≡ V O 2 ( k ) = a 0 + a 1 · T p 1 ) T p 2 / ( 1 − T p 2 ) give 95% confidence limits for the odds ratio in the absence of covariates. 3.2. The Common Odds RatioConsider K independent studies (or strata from the same study), where from the kth study, we have observations for two independent binomial random variables X 1 k and X 2 k with respective success probabilities p 1 k and p 2 k , and respective sample sizes n 1 k and n 2 k , k = 1, 2, ...., K. Thus, the odds ratio from the kth study is δ k = p 1 k / ( 1 − p 1 k ) p 2 k / ( 1 − p 2 k ) , k = 1, 2, ...., K. Assuming that the odds ratio is the same across the K studies, we have δ 1 = δ 2 = . . . . = δ K = δ (say). 3.2.1. An Approximate GPQ for the Common Odds RatioAn approximate GPQ for each δ k , to be denoted by T δ k , can be constructed from the kth study, proceeding as mentioned in Section 3.1. We now combine these GPQs in order to obtain an approximate GPQ for the common odds ratio δ. For this, we propose a weighted average of the study-specific GPQs on the log scale. The weights that we shall use are motivated as follows. For i = 1, 2, if p ^ i k denote sample proportions from the kth study, and if δ ^ k = p ^ 1 k / ( 1 − p ^ 1 k ) p ^ 2 k / ( 1 − p ^ 2 k ) , k = 1, 2, ...., K, then using the delta method, an approximate variance of log ( δ ^ k ) , say 1 / w k , is given by: 1 / w k = 1 n 1 k p 1 k + 0.5 + 1 n 1 k ( 1 − p 1 k ) + 0.5 + 1 n 2 k p 2 k + 0.5 + 1 n 2 k ( 1 − p 2 k ) + 0.5 , where we have also used a continuity correction. Noting that log ( δ ) = ∑ k = 1 K w k log ( δ k ) / ∑ k = 1 K w k , an approximate GPQ T δ for the common odds ratio can be obtained from log ( T δ ) = ∑ k = 1 K T w k log ( T δ k ) / ∑Factor k^2-k-2 - Mathway
. . , K [ 31 ] (reduced result).1: A ← ( K [ 31 ] & 0 b 1 ) ≪ 6 2: B ← ( K [ 31 ] & 0 b 10 ) ≪ 5 3: C ← ( K [ 31 ] & 0 b 1111111 ) 4: K [ 16 ] ← K [ 16 ] ⨁ ( ( A ⨁ B ⨁ C ) ≪ 1 ) 5: K [ 8 ] ← K [ 8 ] ⨁ K [ 24 ] ⨁ ( ( K [ 23 ] ≪ 7 ) ∣ ( K [ 24 ] ≫ 1 ) ) ⨁ ( ( K [ 23 ] ≪ 6 ) ∣ ( ( K [ 24 ] ≫ 2 ) ) ⨁ ( ( K [ 23 ] ≪ 1 ) ∣ ( K [ 24 ] ≫ 7 ) ) 6: K [ 0 ] ← K [ 0 ] ⨁ K [ 16 ] ⨁ ( K [ 16 ] ≫ 2 ) ⨁ ( K [ 16 ] ≫ 7 ) 7:forl = 1 to 7 do8: K [ i + 8 ] ← K [ i + 8 ] ⨁ K [ i + 24 ] ⨁ ( ( K [ i + 23 ] ≪ 7 ) ∣ ( K [ i + 24 ] ≫ 1 ) ) ⨁ ( ( K [ i + 23 ] ≪ 6 ) ∣ ( K [ i + 24 ] ≫ 2 ) ) ⨁ ( ( K [ i + 23 ] ≪ 1 ) ∣ ( K [ i + 24 ] ≫ 7 ) ) 9: K [ i ] ← K [ i ] ⨁ K [ i + 16 ] ⨁ ( ( K [ i + 15 ] ≪ 7 ) ∣ ( K [ i + 16 ] ≫ 1 ) ) ⨁ ( ( K [ i + 15 ] ≪ 6 ) ∣ ( K [ i + 16 ] ≫ 2 ) ) ⨁ ( ( K [. = 0 k 2 k 2 k 3 k k 2 2 k 2 7 k 2 k = 1 ⇒ 10 k 2 9 k = 1 ⇒ 10 k 2 9 k − 1 = 0 ⇒ (10 k − 1) (k 1) = 0 ⇒ k = − 1, 1 10 It is known that probability of any observation must alwaysSolve for k k^ k^2=0
− 1 ) + a 2 · φ CO ( k − 1 ) + a 3 · φ CO 2 ( k − 1 ) + a 4 · φ CH 4 ( k − 1 ) + a 5 · T ( k − 1 ) , (6) u 2 ≡ V o 2 ( k ) = a 0 + a 1 · V O 2 ( k − 1 ) + a 2 · φ CO ( k − 1 ) + a 3 · φ CO 2 ( k − 1 ) + a 4 · φ CH 4 ( k − 1 ) + a 5 · T ( k − 1 ) , (7) where k represents the control step of the sampling period τ 0 ; V a i r and V O 2 represent the flow rates of injected air and oxygen to the mixture (m 3 /h); φ i is the concentration of CO, CO 2 , and CH 4 in the syngas (%); and T represents the coal temperature in the gasification channel ( ∘ C).The second type of model refers to the ratio of the flow rates of gasification agents and the highest temperature in the gasification channel T m a x . The structure of this model is the following [25]: u 1 ≡ V air ( k ) = a 0 + a 1 · V air ( k − 1 ) V O 2 ( Open.Elliptic Paraboloid & Hyperbolic ParaboloidHyperbolic And Elliptic Paraboloid 3D GraphAnd here’s the cool part! We can even combine our quadric surfaces to yield such surfaces as elliptic paraboloids or hyperbolic paraboloids.Traces Of Quadric SurfacesSo, how do we determine the resulting surface?We look for traces.ExampleFor instance, let’s name the shapes by identifying the traces:\begin{equation}x-5 y^{2}+2 z^{2}=0\end{equation}First, we notice that one of the variables is not squared. This instantly tells us that we are dealing with a paraboloid. Now, all we have to do is determine what kind of paraboloid (i.e., elliptic, or hyperbolic)How?Finding traces means we let each variable become a constant (number), and identify it’s resulting curve.If \(x=k\) where \(k\) is any constant, then \(k-5 y^{2}+2 z^{2}=0\) which is a hyperbola.If \(y=k\) where \(k\) is any constant, then \(x-5 k^{2}+2 z^{2}=0\) which is a parabola.If \(z=k\) where \(k\) is any constant, then \(x-5 y^{2}+2 k^{2}=0\) which is a parabola.This means that \(x-5 y^{2}+2 z^{2}=0\) in the Cartesian coordinate system is a hyperbolic paraboloid that will open along the x-axis because it is the non-squared term.ExampleLet’s tackle this problem.Name the shapes by identifying the traces\begin{equation}x^{2}-5 y^{2}+2 z^{2}=8\end{equation}First, we notice that all of the variables are squared, but one of the variables is negative. This instantly tells us that we are dealing with a hyperboloid of one-sheet. Let’s confirm our suspicions by finding the traces.If \(x=k\) where \(k\) is any constant, then \(k^{2}-5 y^{2}+2 z^{2}=8\) which is a hyperbola.If \(y=k\) where \(k\) is any constant, then \(x^{2}-5 k^{2}+2 z^{2}=8\) which is asum [k^2/2^k, [k,1,n]] - Wolfram
+ K i K f ) ] G 3 = L m m ema + m el L m + J m L m η ema k ema 2 R G 2 = η ema k ema 2 R ( J m R m + J m K i K f + B fm L m ) + B fr L m + ( m ema + m el ) ( R m + K i K f ) G 1 = η ema k ema 2 R ( C T C E + B fm R m + K i K f B fm ) + B fr ( R m + K i K f ) + S t L m G 0 = S t ( R m + K i K f ) By dividing both the numerator and the denominator on the right side of Equation (11) by the coefficient of u, we obtain: F ema = u − ( F 3 s 3 + F 2 s 2 + F 1 s ) x a ( s 2 m el + S t ) R k ema η ema K i K v C T [ ( s 2 m el + S t ) R k ema η ema K i K v C T ] ( G 3 s 3 + G 2 s 2 + G 1 s + G 0 ) (12) It can be seen from Figure 13 that to suppress the disturbance force, the feedforward correction element should be used to counteract the part following u in the numerator of Equation (12): G T = F 3 s 3 + F 2 s 2 + F 1 s ( s 2 m el + S t ) R k ema η ema K i K v C T (13) The simulation model of the DEMA force servo system introduced with a PID controller and a feedforward correction element is shown in Figure 14 [48,49,50].As shown in Figure 14, we added several modules in the model to simulate the sampling and data processing of the processor, making the simulation model more realistic. In order to make the simulation model easier to understand and operate, we use PMSM and planetary-roller screw pairs as super components, and integrate feedforward and its sampling and data processing into the super components.The disturbance ofSolve for K (x-k)^2=K^22xx^2 - Mathway
D 12 d C 2 D 12 cD 11 + D 12 d D 21 32 H Fixed-Order Controller Design Choose matrices a, b, c, d to minimize the H norm of the transfer function The dimension of a is k by k (order, between 0 and n=dim(A)) The dimension of b is k by p (number of system inputs) The dimension of c is m (number of system outputs) by k The dimension of d is m by p Total number of variables is (k+m)(k+p) The case k=0 is static output feedback A + B 2 d C 2 B 2 c b C 2 a B 1 + B 2 d D 21 b D 21 C 1 + D 12 d C 2 D 12 cD 11 + D 12 d D 21 33 H Fixed-Order Controller Design Choose matrices a, b, c, d to minimize the H norm of the transfer function The dimension of a is k by k (order, between 0 and n=dim(A)) The dimension of b is k by p (number of system inputs) The dimension of c is m (number of system outputs) by k The dimension of d is m by p Total number of variables is (k+m)(k+p) The case k=0 is static output feedback When B1,C1 are empty, all I/O channels are in performance measure A + B 2 d C 2 B 2 c b C 2 a B 1 + B 2 d D 21 b D 21 C 1 + D 12 d C 2 D 12 cD 11 + D 12 d D 21 34 HIFOO: H Fixed-Order Optimization Aims to find a, b, c, d for which H norm is locally optimal Begins by minimizing the spectral abscissa max(real(eig(A-block))). = 0 k 2 k 2 k 3 k k 2 2 k 2 7 k 2 k = 1 ⇒ 10 k 2 9 k = 1 ⇒ 10 k 2 9 k − 1 = 0 ⇒ (10 k − 1) (k 1) = 0 ⇒ k = − 1, 1 10 It is known that probability of any observation must alwaysSolve K^2 (3)^2-K (3)-2
F 1 + ⋯ + y k f k = 0 } and\n\nfurthermore it has codimension k .\n\nClaim: { C i } ni = 1 is a basis of prim ( ) . It is enough to prove that λ C i is different from zero in H k,k prim ( Y, Q ) or equivalently that the cohomology classes { λ C i } ni = 1 do not come from the ambient space. By contradiction, let us assume that there exists a j and C ⊂ P 2 k + 1 Σ ,X such that λ C ∈ H k,k ( P 2 k + 1 Σ ,X , Q ) with i ∗ ( λ C ) = λ C j or in terms of homology there exists a ( k + 2 ) -dimensional algebraic subvariety V ⊂ P 2 k + 1 Σ ,X such that V ∩ Y = C j so they are equal as a homology class of P 2 k + 1 Σ ,X ,i.e., [ V ∩ Y ] = [ C j ] . It is easy to check that π ( V ) ∩ X = C j as a subvariety of P k + 2 Σ where π ∶ ( x, y ) ↦ x . Hence [ π ( V ) ∩ X ] = [ C j ] which is equivalent to say that λ C j comes from P k + 2 Σ which contradicts the choice of [ C j ] .\n\nRemark 5.2 . Into the proof of the previous theorem, the key fact was that on X the Hodge conjecture holds and we translate it to Y by contradiction. So, using an analogous argument we have:\n\nargument we have:\n\nProposition 5.3. Let Y =Comments
K − 1 ) + a 2 · φ CO ( k − 1 ) + a 3 · φ CO 2 ( k − 1 ) + a 4 · φ CH 4 ( k − 1 ) + a 5 · T max ( k − 1 ) , (8) u 2 ≡ V O 2 ( k ) = a 0 + a 1 · V air ( k − 1 ) V O 2 ( k − 1 ) + a 2 · φ CO ( k − 1 ) + a 3 · φ CO 2 ( k − 1 ) + a 4 · φ CH 4 ( k − 1 ) + a 5 · T max ( k − 1 ) . (9) The third model type aims to achieve the necessary temperature for syngas production. The models regarding the ratio of gasification agents and the maximum temperature T m a x in the channel are in the linear and quadratic form. The structure of the model is as the following [25]: u 1 ≡ V air ( k ) = a 0 + a 1 · V air ( k − 1 ) V O 2 ( k − 1 ) + a 2 · T max ( k − 1 ) + a 3 T max 2 ( k − 1 ) , (10) u 2 ≡ V O 2 ( k ) = a 0 + a 1 ·
2025-03-26T p 1 ) T p 2 / ( 1 − T p 2 ) give 95% confidence limits for the odds ratio in the absence of covariates. 3.2. The Common Odds RatioConsider K independent studies (or strata from the same study), where from the kth study, we have observations for two independent binomial random variables X 1 k and X 2 k with respective success probabilities p 1 k and p 2 k , and respective sample sizes n 1 k and n 2 k , k = 1, 2, ...., K. Thus, the odds ratio from the kth study is δ k = p 1 k / ( 1 − p 1 k ) p 2 k / ( 1 − p 2 k ) , k = 1, 2, ...., K. Assuming that the odds ratio is the same across the K studies, we have δ 1 = δ 2 = . . . . = δ K = δ (say). 3.2.1. An Approximate GPQ for the Common Odds RatioAn approximate GPQ for each δ k , to be denoted by T δ k , can be constructed from the kth study, proceeding as mentioned in Section 3.1. We now combine these GPQs in order to obtain an approximate GPQ for the common odds ratio δ. For this, we propose a weighted average of the study-specific GPQs on the log scale. The weights that we shall use are motivated as follows. For i = 1, 2, if p ^ i k denote sample proportions from the kth study, and if δ ^ k = p ^ 1 k / ( 1 − p ^ 1 k ) p ^ 2 k / ( 1 − p ^ 2 k ) , k = 1, 2, ...., K, then using the delta method, an approximate variance of log ( δ ^ k ) , say 1 / w k , is given by: 1 / w k = 1 n 1 k p 1 k + 0.5 + 1 n 1 k ( 1 − p 1 k ) + 0.5 + 1 n 2 k p 2 k + 0.5 + 1 n 2 k ( 1 − p 2 k ) + 0.5 , where we have also used a continuity correction. Noting that log ( δ ) = ∑ k = 1 K w k log ( δ k ) / ∑ k = 1 K w k , an approximate GPQ T δ for the common odds ratio can be obtained from log ( T δ ) = ∑ k = 1 K T w k log ( T δ k ) / ∑
2025-04-09. . , K [ 31 ] (reduced result).1: A ← ( K [ 31 ] & 0 b 1 ) ≪ 6 2: B ← ( K [ 31 ] & 0 b 10 ) ≪ 5 3: C ← ( K [ 31 ] & 0 b 1111111 ) 4: K [ 16 ] ← K [ 16 ] ⨁ ( ( A ⨁ B ⨁ C ) ≪ 1 ) 5: K [ 8 ] ← K [ 8 ] ⨁ K [ 24 ] ⨁ ( ( K [ 23 ] ≪ 7 ) ∣ ( K [ 24 ] ≫ 1 ) ) ⨁ ( ( K [ 23 ] ≪ 6 ) ∣ ( ( K [ 24 ] ≫ 2 ) ) ⨁ ( ( K [ 23 ] ≪ 1 ) ∣ ( K [ 24 ] ≫ 7 ) ) 6: K [ 0 ] ← K [ 0 ] ⨁ K [ 16 ] ⨁ ( K [ 16 ] ≫ 2 ) ⨁ ( K [ 16 ] ≫ 7 ) 7:forl = 1 to 7 do8: K [ i + 8 ] ← K [ i + 8 ] ⨁ K [ i + 24 ] ⨁ ( ( K [ i + 23 ] ≪ 7 ) ∣ ( K [ i + 24 ] ≫ 1 ) ) ⨁ ( ( K [ i + 23 ] ≪ 6 ) ∣ ( K [ i + 24 ] ≫ 2 ) ) ⨁ ( ( K [ i + 23 ] ≪ 1 ) ∣ ( K [ i + 24 ] ≫ 7 ) ) 9: K [ i ] ← K [ i ] ⨁ K [ i + 16 ] ⨁ ( ( K [ i + 15 ] ≪ 7 ) ∣ ( K [ i + 16 ] ≫ 1 ) ) ⨁ ( ( K [ i + 15 ] ≪ 6 ) ∣ ( K [ i + 16 ] ≫ 2 ) ) ⨁ ( ( K [
2025-03-31− 1 ) + a 2 · φ CO ( k − 1 ) + a 3 · φ CO 2 ( k − 1 ) + a 4 · φ CH 4 ( k − 1 ) + a 5 · T ( k − 1 ) , (6) u 2 ≡ V o 2 ( k ) = a 0 + a 1 · V O 2 ( k − 1 ) + a 2 · φ CO ( k − 1 ) + a 3 · φ CO 2 ( k − 1 ) + a 4 · φ CH 4 ( k − 1 ) + a 5 · T ( k − 1 ) , (7) where k represents the control step of the sampling period τ 0 ; V a i r and V O 2 represent the flow rates of injected air and oxygen to the mixture (m 3 /h); φ i is the concentration of CO, CO 2 , and CH 4 in the syngas (%); and T represents the coal temperature in the gasification channel ( ∘ C).The second type of model refers to the ratio of the flow rates of gasification agents and the highest temperature in the gasification channel T m a x . The structure of this model is the following [25]: u 1 ≡ V air ( k ) = a 0 + a 1 · V air ( k − 1 ) V O 2 (
2025-04-10