Research Article Oscillation for Second-Order Nonlinear Delay Dynamic Equations on Time Scales
|
|
- Τιμοθέα Κομνηνός
- 6 χρόνια πριν
- Προβολές:
Transcript
1 Hindawi Publishing Corporation Advances in Difference Equations Volume 2009, Article ID , 13 pages doi: /2009/ Research Article Oscillation for Second-Order Nonlinear Delay Dynamic Equations on Time Scales Zhenlai Han, 1, 2 Tongxing Li, 2 Shurong Sun, 2 and Chenghui Zhang 1 1 School of Control Science and Engineering, Shandong University, Jinan, Shandong , China 2 School of science, University of Jinan, Jinan, Shandon , China Correspondence should be addressed to Zhenlai Han, hanzhenlai@163.com Received 6 December 2008; Revised 27 February 2009; Accepted 25 May 2009 Recommended by Alberto Cabada By means of Riccati transformation technique, we establish some new oscillation criteria for the second-order nonlinear delay dynamic equations r t x Δ t γ Δ p t f x τ t 0onatime scale T; here γ > 0 is a quotient of odd positive integers with r and p real-valued positive rdcontinuous functions defined on T. Our results not only extend some results established by Hassan in 2008 but also unify the oscillation of the second-order nonlinear delay differential equation and the second-order nonlinear delay difference equation. Copyright q 2009 Zhenlai Han et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. 1. Introduction The theory of time scales, which has recently received a lot of attention, was introduced by Hilger in his Ph.D. Thesis in 1988 in order to unify continuous and discrete analysis see Hilger 1. Several authors have expounded on various aspects of this new theory; see the survey paper by Agarwal et al. 2 and references cited therein. A book on the subject of time scales, by Bohner and Peterson 3, summarizes and organizes much of the time scale calculus. We refer also to the last book by Bohner and Peterson 4 for advances in dynamic equations on time scales. For the notation used hereinafter we refer to the next section that provides some basic facts on time scales extracted from Bohner and Peterson 3. A time scale T is an arbitrary closed subset of the reals, and the cases when this time scale is equal to the reals or to the integers represent the classical theories of differential and of difference equations. Many other interesting time scales exist, and they give rise to plenty of applications, among them the study of population dynamic models which are discrete in season and may follow a difference scheme with variable step-size or often modeled
2 2 Advances in Difference Equations by continuous dynamic systems, die out, say in winter, while their eggs are incubating or dormant, and then in season again, hatching gives rise to a nonoverlapping population see Bohner and Peterson 3. Not only does the new theory of the so-called dynamic equations unify the theories of differential equations and difference equations but also it extends these classical cases to cases in between, for example, to the so-called q-difference equations when T q N 0 {q t : t N 0,q > 1} which has important applications in quantum theory and can be applied on different types of time scales like T hn, T N 2,andT T n the space of the harmonic numbers. In recent years, there has been much research activity concerning the oscillation and nonoscillation of solutions of various equations on time scales, and we refer the reader to Bohner and Saker 5, Erbe 6, and Hassan 7. However, there are few results dealing with the oscillation of the solutions of delay dynamic equations on time scales Following this trend, in this paper, we are concerned with oscillation for the secondorder nonlinear delay dynamic equations ( ( γ ) Δ r t x t ) Δ p t f x τ t 0, t T. 1.1 We assume that γ>0 is a quotient of odd positive integers, r and p are positive, realvalued rd-continuous functions defined on T, τ : T R is strictly increasing, and T : τ T T is a time scale, τ t t and τ t as t, f C R, R which satisfies for some positive constant L, f x /x γ L, for all nonzero x. For oscillation of the second-order delay dynamic equations, Agarwal et al. 8 considered the second-order delay dynamic equations on time scales x ΔΔ t p t x τ t 0, t T, 1.2 and established some sufficient conditions for oscillation of 1.2. Zhang and Shanliang 15 studied the second-order nonlinear delay dynamic equations on time scales x ΔΔ t p t f x t τ 0, t T, 1.3 and the second-order nonlinear dynamic equations on time scales x ΔΔ t p t f x σ t 0, t T, 1.4 where τ R and t τ T, f : R R is continuous and nondecreasing f u >k>0, and uf u > 0foru / 0, and they established the equivalence of the oscillation of 1.3 and 1.4, from which obtained some oscillation criteria and comparison theorems for 1.3. However, the results established in 15 are valid only when the graininess function μ t is bounded which is a restrictive condition. Also the restriction f u >k>0isrequired. Sahiner 13 considered the second-order nonlinear delay dynamic equations on time scales x ΔΔ t p t f x τ t 0, t T, 1.5
3 Advances in Difference Equations 3 where f : R R is continuous, uf u > 0foru / 0and f u L u, τ : T T, τ t t and lim t τ t, and he proved that if there exists a Δ-differentiable function δ t such that [ lim sup p s δ σ s τ s t t 0 σ s σ s ( δ Δ s ) 2 ] Δs, 4Lk 2 δ σ s τ s 1.6 then every solution of 1.5 oscillates. Now, we observe that the condition 1.6 depends on an additional constant k 0, 1 which implies that the results are not sharp seeerbeetal. 10. Han et al. 12 investigated the second-order Emden-Fowler delay dynamic equations on time scales x ΔΔ t p t x γ τ t 0, t T, 1.7 established some sufficient conditions for oscillation of 1.7, and extended the results given in 8. Erbe et al. 10 considered the general nonlinear delay dynamic equations on time scales ( p t x Δ t ) Δ q t f x τ t 0, t T, 1.8 where p and q are positive, real-valued rd-continuous functions defined on T, τ : T T is rd-continuous, τ t t and τ t as t,andf C R, R such that satisfies for some positive constant L, f x L x, xf x > 0 for all nonzero x, and they extended the generalized Riccati transformation techniques in the time scales setting to obtain some new oscillation criteria which improve the results given by Zhang and Shanliang 15 and Sahiner 13. Clearly, 1.2, 1.3, 1.5, and 1.8 are the special cases of 1.1. In this paper, we consider the second-order nonlinear delay dynamic equation on time scales 1.1. As we are interested in oscillatory behavior, we assume throughout this paper that the given time scale T is unbounded above. We assume t 0 T, and it is convenient to assume t 0 > 0. We define the time scale interval of the form t 0, T by t 0, T t 0, T. We shall also consider the two cases t 0 t 0 ( ) 1 1/γ Δt, 1.9 r t ( ) 1 1/γ Δt< r t The paper is organized as follows. In Section 2, we intend to use the Riccati transformation technique, a simple consequence of Keller s chain rule, and an inequality to obtain some sufficient conditions for oscillation of all solutions of 1.1. InSection 3, wegive an example in order to illustrate the main results.
4 4 Advances in Difference Equations 2. Main Results In this section, we give some new oscillation criteria for 1.1. In order to prove our main results, we will use the formula ( x t γ ) 1 Δ γ hx σ t 1 h x t γ 1 x Δ t dh, where x t is delta differentiable and eventually positive or eventually negative, which is a simple consequence of Keller s chain rule see Bohner and Peterson 3, Theorem 1.90.Also, we need the following auxiliary result. For convenience, we note that d t max{0,d t }, d t max{0, d t }, R t : r 1/γ t α t : Δs r 1/γ s, R t R t μ t, β t : α t, 0 <γ 1; β t : αγ t, γ > Lemma 2.1. Assume that 1.9 holds and assume further that x t is an eventually positive solution of 1.1. Then there exists a t 0, T such that x Δ t > 0, x t >R t x Δ t, ( ( ) γ ) Δ r t x Δ x t t < 0, x σ t >α t, t, T. 2.3 The proof is similar to that of Hassan 7, Lemma 2.1, and so is omitted. Lemma 2.2 Chain Rule. Assume that τ : T R is strictly increasing and T : τ T T is a time scale, τ σ t σ τ t. Letx : T R. Ifτ Δ t, and let x Δ τ t exist for t T κ,then x τ t Δ exist, and x τ t Δ x Δ τ t τ Δ t. 2.4 Proof. Let 0 <ε<1 be given and define ε ε 1 τ Δ t x Δ τ t 1. Note that 0 <ε < 1. According to the assumptions, there exist neighborhoods N 1 of t and N 2 of τ t such that τ σ t τ s σ t s τ Δ t ε σ t s, s N 1, x σ τ t x r σ τ t r x Δ τ t ε σ τ t r, r N
5 Advances in Difference Equations 5 Put N N 1 τ 1 N 2 and let s N. Then s N 1 and τ s N 2 and x τ σ t x τ s σ t s x Δ τ t τ Δ t x τ σ t x τ s σ τ t τ s x Δ τ t [ ] σ τ t τ s σ t s τ Δ t x Δ τ t x σ τ t x τ s σ τ t τ s x Δ τ t [ ] τ σ t τ s σ t s τ Δ t x Δ τ t ε σ τ t τ s ε σ t s x Δ τ t ε { } σ τ t τ s σ t s τ Δ t σ t s τ Δ t σ t s x Δ τ t ε { } τ σ t τ s σ t s τ Δ t σ t s τ Δ t σ t s x Δ τ t ε { } ε σ t s σ t s τ Δ t σ t s x Δ τ t { ε σ t s ε { ε σ t s 1 } τ Δ t x Δ τ t } τ Δ t x Δ τ t 2.6 ε σ t s. The proof is completed. Theorem 2.3. Assume that 1.9 holds and τ C 1 rd t 0, T, T,τ σ t σ τ t. Furthermore, assume that there exists a positive function δ C 1 rd t 0, T, R and for all sufficiently large, one has lim sup Lp s α γ τ s δ σ s t ) γ 1 r τ s (( δ Δ s ) ( ) γ 1 ( γ 1 δσ s β τ s τ Δ s ) Δs. γ 2.7 Then 1.1 is oscillatory on t 0, T. Proof. Suppose that 1.1 has a nonoscillatory solution x t on t 0, T. We may assume without loss of generality that x t > 0andx τ t > 0 for all t, T, t 0, T. We shall consider only this case, since the proof when x t is eventually negative is similar. In view of Lemma 2.1,weget 2.3. Define the function ω t by ω t δ t r t ( x Δ t ) γ x τ t γ, t, T. 2.8
6 6 Advances in Difference Equations Then ω t > 0. In view of 1.1 and 2.8 we get ( ω Δ t Lp t δ σ t x τ t γ x τ σ t γ δδ t δ t ω t δσ t r t x Δ t ) γ( x τ t γ ) Δ x τ t γ x τ σ t γ. 2.9 When 0 <γ 1, using 2.1 and 2.4, we have ( x τ t γ ) 1 Δ [ γ h x τ t σ 1 h x τ t ] γ 1 x τ t Δ dh 0 γ 1 0 h x τ σ t 1 h x τ σ t γ 1 x τ t Δ dh 2.10 γ x τ σ t γ 1 x Δ τ t τ Δ t. So, by 2.9 ( ω Δ t Lp t δ σ t x τ t γ x τ σ t γ δδ t δ t ω t γδσ t r t x Δ t ) γ x Δ τ t τ Δ t x τ t γ, 2.11 x τ σ t hence, we get ω Δ t Lp t δ σ t x τ t γ x τ σ t γ δδ t δ t ω t γδσ t r t ( x Δ t ) γ 1 τ Δ t x τ t γ 1 x τ t x τ σ t x Δ τ t, x Δ t 2.12 and using Lemma 2.1, by r t x Δ t γ Δ < 0, we find x Δ τ t /x Δ t r t /r τ t 1/γ,by x t /x σ t >α t, we get x τ t /x τ σ t >α τ t, and so we obtain ω Δ t Lp t δ σ t α γ τ t δδ t δ t ω t γδ σ t x τ t τ Δ t x τ σ t r 1/γ ω t γ 1/γ γ 1/γ τ t δ t Lp t δ σ t α γ τ t δδ t δ t ω t 2.13 γδ σ τ Δ t t α τ t r 1/γ τ t δ t γ 1/γ ω t γ 1/γ.
7 Advances in Difference Equations 7 When γ>1, using 2.1 and 2.4, we have ( x τ t γ ) 1 Δ [ γ h x τ t σ 1 h x τ t ] γ 1 x τ t Δ dh 0 γ 1 0 h x τ t 1 h x τ t γ 1 x τ t Δ dh 2.14 γ x τ t γ 1 x Δ τ t τ Δ t. So, we get ω Δ t Lp t δ σ t x τ t γ x τ σ t γ δδ t δ t ω t γδ σ t r t ( x Δ t ) γ 1 x τ t γ 1 x γ τ t x γ τ σ t Lp t δ σ t α γ τ t δδ t δ t ω t x Δ τ t τ Δ t x Δ t 2.15 γδ σ t α γ τ Δ t τ t r 1/γ τ t δ t γ 1/γ ω t γ 1/γ. So by the definition of β t,weobtain,forγ>0, ω Δ t Lp t δ σ t α γ τ t ( δ Δ t ) δ t ω t γδ σ τ Δ t t β τ t r λ 1 τ t δ λ t ωλ t, 2.16 where λ : γ 1/γ. Define A 0andB 0by A λ : γδσ t β τ t τ Δ t δ t λ r λ 1 τ t ωλ t, B λ 1 : r λ 1/λ τ t ( δ Δ t ) λ ( γδ σ t β τ t τ Δ t ) 1/λ Then, using the inequality λab λ 1 A λ λ 1 B λ, λ yields ( δ Δ t ) δ t ω t γδ σ τ Δ t r τ t (( δ Δ t ) t β τ t r λ 1 τ t δ λ t ωλ t ( ) γ 1 ( γ 1 δσ t β τ t τ Δ t ). γ ) γ
8 8 Advances in Difference Equations From 2.16, wefind ω Δ t Lp t δ σ t α γ r τ t (( δ Δ t ) τ t ( ) γ 1 ( γ 1 δσ t β τ t τ Δ t ) γ ) γ 1 Integrating the inequality 2.20 from to t, weobtain Lp s α γ τ s δ σ r τ s (( δ Δ s ) ) γ 1 s ( ) γ 1 ( γ 1 δσ s β τ s τ Δ s ) Δs ω t γ 1 ω t ω, 2.21 which contradicts 2.7. The proof is completed. Remark 2.4. From Theorem 2.3, we can obtain different conditions for oscillation of all solutions of 1.1 with different choices of δ t. Theorem 2.5. Assume that 1.9 holds and τ C 1 rd t 0, T, T,τ σ t σ τ t. Furthermore, assume that there exist functions H, h C rd D, R, whered { t, s : t s t 0 } such that H t, t 0, t t 0, H t, s > 0, t > s t 0, 2.22 and H has a nonpositive continuous Δ-partial derivation H Δ s t, s with respect to the second variable and satisfies H Δ s σ t,s H σ t,σ s δδ s δ s h t, s δ s H σ t,σ s γ/ γ 1, 2.23 and for all sufficiently large, lim sup t 1 H σ t, K t, s Δs, 2.24 where δ t is a positive Δ-differentiable function and K t, s LH σ t,σ s α γ τ s δ σ s p s r τ s h t, s γ 1 ( γ 1 ) γ 1 ( δσ s β τ s τ Δ s ) γ Then 1.1 is oscillatory on t 0, T. Proof. Suppose that 1.1 has a nonoscillatory solution x t on t 0, T. We may assume without loss of generality that x t > 0andx τ t > 0 for all t, T, t 0, T.
9 Advances in Difference Equations 9 We proceed as in the proof of Theorem 2.3, and we get Then from 2.16 with δ Δ t replaced by δ Δ t, we have Lp t δ σ t α γ τ t ω Δ t δδ t δ t ω t τ Δ t γδσ t β τ t r λ 1 τ t δ λ t ωλ t Multiplying both sides of 2.26, witht replaced by s, byh σ t,σ s, integrating with respect to s from to σ t,weget H σ t,σ s Lp s δ σ s α γ τ s Δs H σ t,σ s ω Δ s Δs H σ t,σ s δδ s δ s ω s Δs 2.27 H σ t,σ s γδ σ τ Δ s s β τ s r λ 1 τ s δ λ s ωλ s Δs. Integrating by parts and using 2.22 and 2.23, weobtain H σ t,σ s Lp s δ σ s α γ τ s Δs H σ t, ω H Δ s σ t,s ω s Δs H σ t,σ s γδ σ τ Δ s s β τ s r λ 1 τ s δ λ s ωλ s Δs H σ t,σ s δδ s δ s ω s Δs H σ t, ω [ h t, s δ s H σ t,σ s 1/λ ω s ] H σ t,σ s γδ σ τ Δ s s β τ s r λ 1 τ s δ λ s ωλ s Δs 2.28 H σ t, ω [ h t, s δ s H σ t,σ s 1/λ ω s ] H σ t,σ s γδ σ τ Δ s s β τ s r λ 1 τ s δ λ s ωλ s Δs.
10 10 Advances in Difference Equations Again, let λ : γ 1/γ, define A 0andB 0by A λ : H σ t,σ s γδ σ τ Δ s s β τ s r λ 1 τ s δ s λ ωλ s, B λ 1 : h t, s r λ 1/λ τ s λ ( γδ σ s β τ s τ Δ s ) 1/λ, 2.29 and using the inequality λab λ 1 A λ λ 1 B λ, λ 1, 2.30 we find h t, s δ s H σ t,σ s 1/λ ω s H σ t,σ s γδ σ τ Δ s s β τ s r λ 1 τ s δ λ s ωλ s 2.31 r τ s h t, s γ 1 ( ) γ 1 ( γ 1 δσ s β τ s τ Δ s ). γ Therefore, from the definition of K t, s, weobtain K t, s Δs H σ t, ω, 2.32 and this implies that 1 σ t K t, s Δs ω, 2.33 H σ t, which contradicts This completes the proof. Now, we give some sufficient conditions when 1.10 holds, which guarantee that every solution of 1.1 oscillates or converges to zero on t 0, T. Theorem 2.6. Assume 1.10 holds and τ C 1 rd t 0, T, T,τ σ t σ τ t. Furthermore, assume that there exists a positive function δ C 1 rd t 0, T, R, for all sufficiently large,such that 2.7 or 2.22, 2.23, and 2.24 hold. If there exists a positive function η C 1 rd t 0, T, R, η Δ t 0, such that t 0 [ 1 t ] 1/γ η σ s p s Δs Δt, 2.34 η t r t t 0 then every solution of 1.1 is either oscillatory or converges to zero on t 0, T.
11 Advances in Difference Equations 11 Proof. We proceed as in Theorem 2.3 or Theorem 2.5, and we assume that 1.1 has a nonoscillatory solution such that x t > 0, and x τ t > 0, for all t, T. From the proof of Lemma 2.1, we see that there exist two possible cases for the sign of x Δ t. The proof when x Δ t is an eventually positive is similar to that of the proof of Theorem 2.3 or Theorem 2.5, and hence it is omitted. Next, suppose that x Δ t < 0fort, T. Then x t is decreasing and lim t x t b 0. We assert that b 0. If not, then x τ t x t x σ t b>0fort, T. Since f x τ t L x τ t γ, there exists a number t 2, T such that f x τ t Lb γ for t t 2. Defining the function u t η t r t x Δ t γ, we obtain from 1.1 ( γ ( ( ) γ ) Δ u Δ t η Δ t r t x t ) Δ η σ t r t x Δ t η σ t p t f x τ t Lη σ t p t x τ t γ Lb γ η σ t p t, t t 2, T Hence, for t t 2, T, we have u t u t 2 Lb γ t 2 η σ s p s Δs Lb γ t 2 η σ s p s Δs, 2.36 because of u t 2 η t 2 r t 2 x Δ t 2 γ < 0. So, we have x t x t 2 t 2 x Δ s Δs L 1/γ b [ 1 s ] 1/γ η σ τ p τ Δτ Δs η s r s t 2 t 2 By condition 2.34, wegetx t as t, and this is a contradiction to the fact that x t > 0fort.Thusb 0 and then x t 0ast. The proof is completed. 3. Application and Example Hassan 7 considered the second-order half-linear dynamic equations on time scales ( ( γ ) Δ r t x t ) Δ p t x γ t 0, t T, 3.1 where γ>0 is a quotient of odd positive integers, and r and p are positive, real-valued rdcontinuous functions defined on T, and he established some new oscillation criteria of 3.1. For example
12 12 Advances in Difference Equations Theorem 3.1 Hassan 7, Theorem 2.1. Assume that 1.9 holds. Furthermore, assume that there exists a positive function δ C 1 rd t 0,, R such that lim sup p s α γ s δ σ s t t 0 ) γ 1 r s (( δ Δ s ) ( ) γ 1 ( γ 1 δσ s β s ) Δs. γ 3.2 Then 3.1 is oscillatory on t 0, T. We note that 1.1 becomes 3.1 when f x x γ,τ t t, andtheorem 2.3 becomes Theorem 3.1, andsotheorem 2.3 in this paper essentially includes results of Hassan 7, Theorem 2.1. Similarly, Theorem 2.5 includes results of Hassan 7, Theorem 2.2, andtheorem 2.6 includes results of Hassan 7, Theorem 2.4. One can easily see that nonlinear delay dynamic equations 1.8 considered by Erbe et al. 10 are the special cases of 1.1, and the results obtained in 10 cannot be applied in 1.1, and so our results are new. Example 3.2. Consider the second-order delay dynamic equations (( ) γ ) Δ x Δ σ τ t γ t tτ γ t x γ τ t 0, t t 0, T, 3.3 where γ > 0 is a quotient of odd positive integers, τ t t, and τ T T is a time scale, lim t τ t,τ Δ t > 0,τ σ t σ τ t. Let r t 1, p t σ τ t γ /tτ γ t, f x x γ,l 1, t t 0, T. Then condition 1.9 holds, R t t, and we can find 0 <k<1 such that α t R t /R t μ t t /σ t kt/σ t,α τ t kτ t /σ τ t for t t k > t 0. Take δ t 1. By Theorem 2.3,weobtain lim sup Lp s α γ τ s δ σ s t ) γ 1 r τ s (( δ Δ s ) ( ) γ 1 ( γ 1 δσ s β τ s τ Δ s ) Δs γ lim sup p s α γ τ s Δs t k γ σ τ s lim sup t t k sτ γ s k γ Δs lim sup. t t k s γ τ γ s σ τ s γ Δs 3.4 We conclude that 3.3 is oscillatory. Acknowledgments The authors sincerely thank the reviewers for their valuable suggestions and useful comments that have lead to the present improved version of the original manuscript.
13 Advances in Difference Equations 13 This research is supported by the Natural Science Foundation of China , China Postdoctoral Science Foundation Funded Project , Shandong Postdoctoral Funded Project and supported by Shandong Research Funds Y2008A28, and also supported by the University of Jinan Research Funds for Doctors B0621, XBS0843. References 1 S. Hilger, Analysis on measure chains a unified approach to continuous and discrete calculus, Results in Mathematics, vol. 18, no. 1-2, pp , R. P. Agarwal, M. Bohner, D. O Regan, and A. Peterson, Dynamic equations on time scales: a survey, Journal of Computational and Applied Mathematics, vol. 141, no. 1-2, pp. 1 26, M. Bohner and A. Peterson, Dynamic Equations on Time Scales: An Introduction with Applications, Birkhäuser, Boston, Mass, USA, M. Bohner and A. Peterson, Eds., Advances in Dynamic Equations on Time Scales, Birkhäuser, Boston, Mass, USA, M. Bohner and S. H. Saker, Oscillation of second order nonlinear dynamic equations on time scales, The Rocky Mountain Journal of Mathematics, vol. 34, no. 4, pp , L. Erbe, Oscillation results for second-order linear equations on a time scale, Journal of Difference Equations and Applications, vol. 8, no. 11, pp , T. S. Hassan, Oscillation criteria for half-linear dynamic equations on time scales, Journal of Mathematical Analysis and Applications, vol. 345, no. 1, pp , R. P. Agarwal, M. Bohner, and S. H. Saker, Oscillation of second order delay dynamic equations, The Canadian Applied Mathematics Quarterly, vol. 13, no. 1, pp. 1 17, M. Bohner, B. Karpuz, and Ö. Öcalan, Iterated oscillation criteria for delay dynamic equations of first order, Advances in Difference Equations, vol. 2008, Article ID , 12 pages, L. Erbe, A. Peterson, and S. H. Saker, Oscillation criteria for second-order nonlinear delay dynamic equations, Journal of Mathematical Analysis and Applications, vol. 333, no. 1, pp , Z. Han, B. Shi, and S. Sun, Oscillation criteria for second-order delay dynamic equations on time scales, Advances in Difference Equations, vol. 2007, Article ID 70730, 16 pages, Z. Han, S. Sun, and B. Shi, Oscillation criteria for a class of second-order Emden-Fowler delay dynamic equations on time scales, Journal of Mathematical Analysis and Applications, vol. 334, no. 2, pp , Y. Sahiner, Oscillation of second-order delay differential equations on time scales, Nonlinear Analysis: Theory, Methods & Applications, vol. 63, no. 5 7, pp. e1073 e1080, Y. Sahiner, Oscillation of second-order neutral delay and mixed-type dynamic equations on time scales, Advances in Difference Equations, vol. 2006, Article ID 65626, 9 pages, B. G. Zhang and Z. Shanliang, Oscillation of second-order nonlinear delay dynamic equations on time scales, Computers & Mathematics with Applications, vol. 49, no. 4, pp , 2005.
Congruence Classes of Invertible Matrices of Order 3 over F 2
International Journal of Algebra, Vol. 8, 24, no. 5, 239-246 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/.2988/ija.24.422 Congruence Classes of Invertible Matrices of Order 3 over F 2 Ligong An and
Διαβάστε περισσότερα2 Composition. Invertible Mappings
Arkansas Tech University MATH 4033: Elementary Modern Algebra Dr. Marcel B. Finan Composition. Invertible Mappings In this section we discuss two procedures for creating new mappings from old ones, namely,
Διαβάστε περισσότεραEvery set of first-order formulas is equivalent to an independent set
Every set of first-order formulas is equivalent to an independent set May 6, 2008 Abstract A set of first-order formulas, whatever the cardinality of the set of symbols, is equivalent to an independent
Διαβάστε περισσότεραSCITECH Volume 13, Issue 2 RESEARCH ORGANISATION Published online: March 29, 2018
Journal of rogressive Research in Mathematics(JRM) ISSN: 2395-028 SCITECH Volume 3, Issue 2 RESEARCH ORGANISATION ublished online: March 29, 208 Journal of rogressive Research in Mathematics www.scitecresearch.com/journals
Διαβάστε περισσότεραST5224: Advanced Statistical Theory II
ST5224: Advanced Statistical Theory II 2014/2015: Semester II Tutorial 7 1. Let X be a sample from a population P and consider testing hypotheses H 0 : P = P 0 versus H 1 : P = P 1, where P j is a known
Διαβάστε περισσότεραOrdinal Arithmetic: Addition, Multiplication, Exponentiation and Limit
Ordinal Arithmetic: Addition, Multiplication, Exponentiation and Limit Ting Zhang Stanford May 11, 2001 Stanford, 5/11/2001 1 Outline Ordinal Classification Ordinal Addition Ordinal Multiplication Ordinal
Διαβάστε περισσότεραHomework 3 Solutions
Homework 3 Solutions Igor Yanovsky (Math 151A TA) Problem 1: Compute the absolute error and relative error in approximations of p by p. (Use calculator!) a) p π, p 22/7; b) p π, p 3.141. Solution: For
Διαβάστε περισσότεραCoefficient Inequalities for a New Subclass of K-uniformly Convex Functions
International Journal of Computational Science and Mathematics. ISSN 0974-89 Volume, Number (00), pp. 67--75 International Research Publication House http://www.irphouse.com Coefficient Inequalities for
Διαβάστε περισσότεραSOME PROPERTIES OF FUZZY REAL NUMBERS
Sahand Communications in Mathematical Analysis (SCMA) Vol. 3 No. 1 (2016), 21-27 http://scma.maragheh.ac.ir SOME PROPERTIES OF FUZZY REAL NUMBERS BAYAZ DARABY 1 AND JAVAD JAFARI 2 Abstract. In the mathematical
Διαβάστε περισσότεραExample Sheet 3 Solutions
Example Sheet 3 Solutions. i Regular Sturm-Liouville. ii Singular Sturm-Liouville mixed boundary conditions. iii Not Sturm-Liouville ODE is not in Sturm-Liouville form. iv Regular Sturm-Liouville note
Διαβάστε περισσότεραUniform Convergence of Fourier Series Michael Taylor
Uniform Convergence of Fourier Series Michael Taylor Given f L 1 T 1 ), we consider the partial sums of the Fourier series of f: N 1) S N fθ) = ˆfk)e ikθ. k= N A calculation gives the Dirichlet formula
Διαβάστε περισσότεραProblem Set 3: Solutions
CMPSCI 69GG Applied Information Theory Fall 006 Problem Set 3: Solutions. [Cover and Thomas 7.] a Define the following notation, C I p xx; Y max X; Y C I p xx; Ỹ max I X; Ỹ We would like to show that C
Διαβάστε περισσότεραC.S. 430 Assignment 6, Sample Solutions
C.S. 430 Assignment 6, Sample Solutions Paul Liu November 15, 2007 Note that these are sample solutions only; in many cases there were many acceptable answers. 1 Reynolds Problem 10.1 1.1 Normal-order
Διαβάστε περισσότερα4.6 Autoregressive Moving Average Model ARMA(1,1)
84 CHAPTER 4. STATIONARY TS MODELS 4.6 Autoregressive Moving Average Model ARMA(,) This section is an introduction to a wide class of models ARMA(p,q) which we will consider in more detail later in this
Διαβάστε περισσότεραCHAPTER 25 SOLVING EQUATIONS BY ITERATIVE METHODS
CHAPTER 5 SOLVING EQUATIONS BY ITERATIVE METHODS EXERCISE 104 Page 8 1. Find the positive root of the equation x + 3x 5 = 0, correct to 3 significant figures, using the method of bisection. Let f(x) =
Διαβάστε περισσότεραSection 8.3 Trigonometric Equations
99 Section 8. Trigonometric Equations Objective 1: Solve Equations Involving One Trigonometric Function. In this section and the next, we will exple how to solving equations involving trigonometric functions.
Διαβάστε περισσότεραMINIMAL CLOSED SETS AND MAXIMAL CLOSED SETS
MINIMAL CLOSED SETS AND MAXIMAL CLOSED SETS FUMIE NAKAOKA AND NOBUYUKI ODA Received 20 December 2005; Revised 28 May 2006; Accepted 6 August 2006 Some properties of minimal closed sets and maximal closed
Διαβάστε περισσότεραPhys460.nb Solution for the t-dependent Schrodinger s equation How did we find the solution? (not required)
Phys460.nb 81 ψ n (t) is still the (same) eigenstate of H But for tdependent H. The answer is NO. 5.5.5. Solution for the tdependent Schrodinger s equation If we assume that at time t 0, the electron starts
Διαβάστε περισσότεραEE512: Error Control Coding
EE512: Error Control Coding Solution for Assignment on Finite Fields February 16, 2007 1. (a) Addition and Multiplication tables for GF (5) and GF (7) are shown in Tables 1 and 2. + 0 1 2 3 4 0 0 1 2 3
Διαβάστε περισσότεραStatistical Inference I Locally most powerful tests
Statistical Inference I Locally most powerful tests Shirsendu Mukherjee Department of Statistics, Asutosh College, Kolkata, India. shirsendu st@yahoo.co.in So far we have treated the testing of one-sided
Διαβάστε περισσότεραOther Test Constructions: Likelihood Ratio & Bayes Tests
Other Test Constructions: Likelihood Ratio & Bayes Tests Side-Note: So far we have seen a few approaches for creating tests such as Neyman-Pearson Lemma ( most powerful tests of H 0 : θ = θ 0 vs H 1 :
Διαβάστε περισσότεραA Note on Intuitionistic Fuzzy. Equivalence Relation
International Mathematical Forum, 5, 2010, no. 67, 3301-3307 A Note on Intuitionistic Fuzzy Equivalence Relation D. K. Basnet Dept. of Mathematics, Assam University Silchar-788011, Assam, India dkbasnet@rediffmail.com
Διαβάστε περισσότεραResearch Article Existence of Positive Solutions for m-point Boundary Value Problems on Time Scales
Hindawi Publishing Corporation Discrete Dynamics in Nature and Society Volume 29, Article ID 189768, 12 pages doi:1.1155/29/189768 Research Article Existence of Positive Solutions for m-point Boundary
Διαβάστε περισσότεραChapter 6: Systems of Linear Differential. be continuous functions on the interval
Chapter 6: Systems of Linear Differential Equations Let a (t), a 2 (t),..., a nn (t), b (t), b 2 (t),..., b n (t) be continuous functions on the interval I. The system of n first-order differential equations
Διαβάστε περισσότεραFinite Field Problems: Solutions
Finite Field Problems: Solutions 1. Let f = x 2 +1 Z 11 [x] and let F = Z 11 [x]/(f), a field. Let Solution: F =11 2 = 121, so F = 121 1 = 120. The possible orders are the divisors of 120. Solution: The
Διαβάστε περισσότεραderivation of the Laplacian from rectangular to spherical coordinates
derivation of the Laplacian from rectangular to spherical coordinates swapnizzle 03-03- :5:43 We begin by recognizing the familiar conversion from rectangular to spherical coordinates (note that φ is used
Διαβάστε περισσότεραΑπόκριση σε Μοναδιαία Ωστική Δύναμη (Unit Impulse) Απόκριση σε Δυνάμεις Αυθαίρετα Μεταβαλλόμενες με το Χρόνο. Απόστολος Σ.
Απόκριση σε Δυνάμεις Αυθαίρετα Μεταβαλλόμενες με το Χρόνο The time integral of a force is referred to as impulse, is determined by and is obtained from: Newton s 2 nd Law of motion states that the action
Διαβάστε περισσότεραNew Oscillation Criteria for Second-Order Neutral Delay Dynamic Equations
International Journal of Mathematical Analysis Vol. 11, 2017, no. 19, 945-954 HIKARI Ltd, www.m-hikari.com https://doi.org/10.12988/ijma.2017.79127 New Oscillation Criteria for Second-Order Neutral Delay
Διαβάστε περισσότεραHOMEWORK 4 = G. In order to plot the stress versus the stretch we define a normalized stretch:
HOMEWORK 4 Problem a For the fast loading case, we want to derive the relationship between P zz and λ z. We know that the nominal stress is expressed as: P zz = ψ λ z where λ z = λ λ z. Therefore, applying
Διαβάστε περισσότεραInverse trigonometric functions & General Solution of Trigonometric Equations. ------------------ ----------------------------- -----------------
Inverse trigonometric functions & General Solution of Trigonometric Equations. 1. Sin ( ) = a) b) c) d) Ans b. Solution : Method 1. Ans a: 17 > 1 a) is rejected. w.k.t Sin ( sin ) = d is rejected. If sin
Διαβάστε περισσότεραMatrices and Determinants
Matrices and Determinants SUBJECTIVE PROBLEMS: Q 1. For what value of k do the following system of equations possess a non-trivial (i.e., not all zero) solution over the set of rationals Q? x + ky + 3z
Διαβάστε περισσότεραSCHOOL OF MATHEMATICAL SCIENCES G11LMA Linear Mathematics Examination Solutions
SCHOOL OF MATHEMATICAL SCIENCES GLMA Linear Mathematics 00- Examination Solutions. (a) i. ( + 5i)( i) = (6 + 5) + (5 )i = + i. Real part is, imaginary part is. (b) ii. + 5i i ( + 5i)( + i) = ( i)( + i)
Διαβάστε περισσότεραMath221: HW# 1 solutions
Math: HW# solutions Andy Royston October, 5 7.5.7, 3 rd Ed. We have a n = b n = a = fxdx = xdx =, x cos nxdx = x sin nx n sin nxdx n = cos nx n = n n, x sin nxdx = x cos nx n + cos nxdx n cos n = + sin
Διαβάστε περισσότεραConcrete Mathematics Exercises from 30 September 2016
Concrete Mathematics Exercises from 30 September 2016 Silvio Capobianco Exercise 1.7 Let H(n) = J(n + 1) J(n). Equation (1.8) tells us that H(2n) = 2, and H(2n+1) = J(2n+2) J(2n+1) = (2J(n+1) 1) (2J(n)+1)
Διαβάστε περισσότερα3.4 SUM AND DIFFERENCE FORMULAS. NOTE: cos(α+β) cos α + cos β cos(α-β) cos α -cos β
3.4 SUM AND DIFFERENCE FORMULAS Page Theorem cos(αβ cos α cos β -sin α cos(α-β cos α cos β sin α NOTE: cos(αβ cos α cos β cos(α-β cos α -cos β Proof of cos(α-β cos α cos β sin α Let s use a unit circle
Διαβάστε περισσότεραThe Simply Typed Lambda Calculus
Type Inference Instead of writing type annotations, can we use an algorithm to infer what the type annotations should be? That depends on the type system. For simple type systems the answer is yes, and
Διαβάστε περισσότεραSecond Order RLC Filters
ECEN 60 Circuits/Electronics Spring 007-0-07 P. Mathys Second Order RLC Filters RLC Lowpass Filter A passive RLC lowpass filter (LPF) circuit is shown in the following schematic. R L C v O (t) Using phasor
Διαβάστε περισσότεραSecond Order Partial Differential Equations
Chapter 7 Second Order Partial Differential Equations 7.1 Introduction A second order linear PDE in two independent variables (x, y Ω can be written as A(x, y u x + B(x, y u xy + C(x, y u u u + D(x, y
Διαβάστε περισσότερα6.3 Forecasting ARMA processes
122 CHAPTER 6. ARMA MODELS 6.3 Forecasting ARMA processes The purpose of forecasting is to predict future values of a TS based on the data collected to the present. In this section we will discuss a linear
Διαβάστε περισσότεραFourier Series. MATH 211, Calculus II. J. Robert Buchanan. Spring Department of Mathematics
Fourier Series MATH 211, Calculus II J. Robert Buchanan Department of Mathematics Spring 2018 Introduction Not all functions can be represented by Taylor series. f (k) (c) A Taylor series f (x) = (x c)
Διαβάστε περισσότεραAreas and Lengths in Polar Coordinates
Kiryl Tsishchanka Areas and Lengths in Polar Coordinates In this section we develop the formula for the area of a region whose boundary is given by a polar equation. We need to use the formula for the
Διαβάστε περισσότεραMain source: "Discrete-time systems and computer control" by Α. ΣΚΟΔΡΑΣ ΨΗΦΙΑΚΟΣ ΕΛΕΓΧΟΣ ΔΙΑΛΕΞΗ 4 ΔΙΑΦΑΝΕΙΑ 1
Main source: "Discrete-time systems and computer control" by Α. ΣΚΟΔΡΑΣ ΨΗΦΙΑΚΟΣ ΕΛΕΓΧΟΣ ΔΙΑΛΕΞΗ 4 ΔΙΑΦΑΝΕΙΑ 1 A Brief History of Sampling Research 1915 - Edmund Taylor Whittaker (1873-1956) devised a
Διαβάστε περισσότεραApproximation of distance between locations on earth given by latitude and longitude
Approximation of distance between locations on earth given by latitude and longitude Jan Behrens 2012-12-31 In this paper we shall provide a method to approximate distances between two points on earth
Διαβάστε περισσότεραMath 446 Homework 3 Solutions. (1). (i): Reverse triangle inequality for metrics: Let (X, d) be a metric space and let x, y, z X.
Math 446 Homework 3 Solutions. (1). (i): Reverse triangle inequalit for metrics: Let (X, d) be a metric space and let x,, z X. Prove that d(x, z) d(, z) d(x, ). (ii): Reverse triangle inequalit for norms:
Διαβάστε περισσότεραTridiagonal matrices. Gérard MEURANT. October, 2008
Tridiagonal matrices Gérard MEURANT October, 2008 1 Similarity 2 Cholesy factorizations 3 Eigenvalues 4 Inverse Similarity Let α 1 ω 1 β 1 α 2 ω 2 T =......... β 2 α 1 ω 1 β 1 α and β i ω i, i = 1,...,
Διαβάστε περισσότεραforms This gives Remark 1. How to remember the above formulas: Substituting these into the equation we obtain with
Week 03: C lassification of S econd- Order L inear Equations In last week s lectures we have illustrated how to obtain the general solutions of first order PDEs using the method of characteristics. We
Διαβάστε περισσότεραAreas and Lengths in Polar Coordinates
Kiryl Tsishchanka Areas and Lengths in Polar Coordinates In this section we develop the formula for the area of a region whose boundary is given by a polar equation. We need to use the formula for the
Διαβάστε περισσότερα2. Let H 1 and H 2 be Hilbert spaces and let T : H 1 H 2 be a bounded linear operator. Prove that [T (H 1 )] = N (T ). (6p)
Uppsala Universitet Matematiska Institutionen Andreas Strömbergsson Prov i matematik Funktionalanalys Kurs: F3B, F4Sy, NVP 2005-03-08 Skrivtid: 9 14 Tillåtna hjälpmedel: Manuella skrivdon, Kreyszigs bok
Διαβάστε περισσότεραLecture 2. Soundness and completeness of propositional logic
Lecture 2 Soundness and completeness of propositional logic February 9, 2004 1 Overview Review of natural deduction. Soundness and completeness. Semantics of propositional formulas. Soundness proof. Completeness
Διαβάστε περισσότεραHomomorphism in Intuitionistic Fuzzy Automata
International Journal of Fuzzy Mathematics Systems. ISSN 2248-9940 Volume 3, Number 1 (2013), pp. 39-45 Research India Publications http://www.ripublication.com/ijfms.htm Homomorphism in Intuitionistic
Διαβάστε περισσότεραChapter 6: Systems of Linear Differential. be continuous functions on the interval
Chapter 6: Systems of Linear Differential Equations Let a (t), a 2 (t),..., a nn (t), b (t), b 2 (t),..., b n (t) be continuous functions on the interval I. The system of n first-order differential equations
Διαβάστε περισσότεραSection 7.6 Double and Half Angle Formulas
09 Section 7. Double and Half Angle Fmulas To derive the double-angles fmulas, we will use the sum of two angles fmulas that we developed in the last section. We will let α θ and β θ: cos(θ) cos(θ + θ)
Διαβάστε περισσότεραORDINAL ARITHMETIC JULIAN J. SCHLÖDER
ORDINAL ARITHMETIC JULIAN J. SCHLÖDER Abstract. We define ordinal arithmetic and show laws of Left- Monotonicity, Associativity, Distributivity, some minor related properties and the Cantor Normal Form.
Διαβάστε περισσότεραJesse Maassen and Mark Lundstrom Purdue University November 25, 2013
Notes on Average Scattering imes and Hall Factors Jesse Maassen and Mar Lundstrom Purdue University November 5, 13 I. Introduction 1 II. Solution of the BE 1 III. Exercises: Woring out average scattering
Διαβάστε περισσότεραNowhere-zero flows Let be a digraph, Abelian group. A Γ-circulation in is a mapping : such that, where, and : tail in X, head in
Nowhere-zero flows Let be a digraph, Abelian group. A Γ-circulation in is a mapping : such that, where, and : tail in X, head in : tail in X, head in A nowhere-zero Γ-flow is a Γ-circulation such that
Διαβάστε περισσότεραANSWERSHEET (TOPIC = DIFFERENTIAL CALCULUS) COLLECTION #2. h 0 h h 0 h h 0 ( ) g k = g 0 + g 1 + g g 2009 =?
Teko Classes IITJEE/AIEEE Maths by SUHAAG SIR, Bhopal, Ph (0755) 3 00 000 www.tekoclasses.com ANSWERSHEET (TOPIC DIFFERENTIAL CALCULUS) COLLECTION # Question Type A.Single Correct Type Q. (A) Sol least
Διαβάστε περισσότεραEcon 2110: Fall 2008 Suggested Solutions to Problem Set 8 questions or comments to Dan Fetter 1
Eon : Fall 8 Suggested Solutions to Problem Set 8 Email questions or omments to Dan Fetter Problem. Let X be a salar with density f(x, θ) (θx + θ) [ x ] with θ. (a) Find the most powerful level α test
Διαβάστε περισσότερα( y) Partial Differential Equations
Partial Dierential Equations Linear P.D.Es. contains no owers roducts o the deendent variables / an o its derivatives can occasionall be solved. Consider eamle ( ) a (sometimes written as a ) we can integrate
Διαβάστε περισσότεραPractice Exam 2. Conceptual Questions. 1. State a Basic identity and then verify it. (a) Identity: Solution: One identity is csc(θ) = 1
Conceptual Questions. State a Basic identity and then verify it. a) Identity: Solution: One identity is cscθ) = sinθ) Practice Exam b) Verification: Solution: Given the point of intersection x, y) of the
Διαβάστε περισσότεραNotes on the Open Economy
Notes on the Open Econom Ben J. Heijdra Universit of Groningen April 24 Introduction In this note we stud the two-countr model of Table.4 in more detail. restated here for convenience. The model is Table.4.
Διαβάστε περισσότεραGenerating Set of the Complete Semigroups of Binary Relations
Applied Mathematics 06 7 98-07 Published Online January 06 in SciRes http://wwwscirporg/journal/am http://dxdoiorg/036/am067009 Generating Set of the Complete Semigroups of Binary Relations Yasha iasamidze
Διαβάστε περισσότερα6.1. Dirac Equation. Hamiltonian. Dirac Eq.
6.1. Dirac Equation Ref: M.Kaku, Quantum Field Theory, Oxford Univ Press (1993) η μν = η μν = diag(1, -1, -1, -1) p 0 = p 0 p = p i = -p i p μ p μ = p 0 p 0 + p i p i = E c 2 - p 2 = (m c) 2 H = c p 2
Διαβάστε περισσότεραAppendix to On the stability of a compressible axisymmetric rotating flow in a pipe. By Z. Rusak & J. H. Lee
Appendi to On the stability of a compressible aisymmetric rotating flow in a pipe By Z. Rusak & J. H. Lee Journal of Fluid Mechanics, vol. 5 4, pp. 5 4 This material has not been copy-edited or typeset
Διαβάστε περισσότεραLecture 2: Dirac notation and a review of linear algebra Read Sakurai chapter 1, Baym chatper 3
Lecture 2: Dirac notation and a review of linear algebra Read Sakurai chapter 1, Baym chatper 3 1 State vector space and the dual space Space of wavefunctions The space of wavefunctions is the set of all
Διαβάστε περισσότεραCRASH COURSE IN PRECALCULUS
CRASH COURSE IN PRECALCULUS Shiah-Sen Wang The graphs are prepared by Chien-Lun Lai Based on : Precalculus: Mathematics for Calculus by J. Stuwart, L. Redin & S. Watson, 6th edition, 01, Brooks/Cole Chapter
Διαβάστε περισσότεραSrednicki Chapter 55
Srednicki Chapter 55 QFT Problems & Solutions A. George August 3, 03 Srednicki 55.. Use equations 55.3-55.0 and A i, A j ] = Π i, Π j ] = 0 (at equal times) to verify equations 55.-55.3. This is our third
Διαβάστε περισσότεραD Alembert s Solution to the Wave Equation
D Alembert s Solution to the Wave Equation MATH 467 Partial Differential Equations J. Robert Buchanan Department of Mathematics Fall 2018 Objectives In this lesson we will learn: a change of variable technique
Διαβάστε περισσότεραCommutative Monoids in Intuitionistic Fuzzy Sets
Commutative Monoids in Intuitionistic Fuzzy Sets S K Mala #1, Dr. MM Shanmugapriya *2 1 PhD Scholar in Mathematics, Karpagam University, Coimbatore, Tamilnadu- 641021 Assistant Professor of Mathematics,
Διαβάστε περισσότεραFractional Colorings and Zykov Products of graphs
Fractional Colorings and Zykov Products of graphs Who? Nichole Schimanski When? July 27, 2011 Graphs A graph, G, consists of a vertex set, V (G), and an edge set, E(G). V (G) is any finite set E(G) is
Διαβάστε περισσότεραMA 342N Assignment 1 Due 24 February 2016
M 342N ssignment Due 24 February 206 Id: 342N-s206-.m4,v. 206/02/5 2:25:36 john Exp john. Suppose that q, in addition to satisfying the assumptions from lecture, is an even function. Prove that η(λ = 0,
Διαβάστε περισσότεραk A = [k, k]( )[a 1, a 2 ] = [ka 1,ka 2 ] 4For the division of two intervals of confidence in R +
Chapter 3. Fuzzy Arithmetic 3- Fuzzy arithmetic: ~Addition(+) and subtraction (-): Let A = [a and B = [b, b in R If x [a and y [b, b than x+y [a +b +b Symbolically,we write A(+)B = [a (+)[b, b = [a +b
Διαβάστε περισσότεραLecture 21: Properties and robustness of LSE
Lecture 21: Properties and robustness of LSE BLUE: Robustness of LSE against normality We now study properties of l τ β and σ 2 under assumption A2, i.e., without the normality assumption on ε. From Theorem
Διαβάστε περισσότεραHomework 8 Model Solution Section
MATH 004 Homework Solution Homework 8 Model Solution Section 14.5 14.6. 14.5. Use the Chain Rule to find dz where z cosx + 4y), x 5t 4, y 1 t. dz dx + dy y sinx + 4y)0t + 4) sinx + 4y) 1t ) 0t + 4t ) sinx
Διαβάστε περισσότεραResearch Article Some Properties of Certain Class of Integral Operators
Hindawi Publishing Corporation Journal of Inequalities and Applications Volume 211, Article ID 53154, 1 pages doi:1.1155/211/53154 Research Article Some Properties of Certain Class of Integral Operators
Διαβάστε περισσότεραCyclic or elementary abelian Covers of K 4
Cyclic or elementary abelian Covers of K 4 Yan-Quan Feng Mathematics, Beijing Jiaotong University Beijing 100044, P.R. China Summer School, Rogla, Slovenian 2011-06 Outline 1 Question 2 Main results 3
Διαβάστε περισσότεραω ω ω ω ω ω+2 ω ω+2 + ω ω ω ω+2 + ω ω+1 ω ω+2 2 ω ω ω ω ω ω ω ω+1 ω ω2 ω ω2 + ω ω ω2 + ω ω ω ω2 + ω ω+1 ω ω2 + ω ω+1 + ω ω ω ω2 + ω
0 1 2 3 4 5 6 ω ω + 1 ω + 2 ω + 3 ω + 4 ω2 ω2 + 1 ω2 + 2 ω2 + 3 ω3 ω3 + 1 ω3 + 2 ω4 ω4 + 1 ω5 ω 2 ω 2 + 1 ω 2 + 2 ω 2 + ω ω 2 + ω + 1 ω 2 + ω2 ω 2 2 ω 2 2 + 1 ω 2 2 + ω ω 2 3 ω 3 ω 3 + 1 ω 3 + ω ω 3 +
Διαβάστε περισσότερα1. Introduction and Preliminaries.
Faculty of Sciences and Mathematics, University of Niš, Serbia Available at: http://www.pmf.ni.ac.yu/filomat Filomat 22:1 (2008), 97 106 ON δ SETS IN γ SPACES V. Renuka Devi and D. Sivaraj Abstract We
Διαβάστε περισσότεραA General Note on δ-quasi Monotone and Increasing Sequence
International Mathematical Forum, 4, 2009, no. 3, 143-149 A General Note on δ-quasi Monotone and Increasing Sequence Santosh Kr. Saxena H. N. 419, Jawaharpuri, Badaun, U.P., India Presently working in
Διαβάστε περισσότεραThe Number of Zeros of a Polynomial in a Disk as a Consequence of Restrictions on the Coefficients
The Number of Zeros of a Polynomial in a Disk as a Consequence of Restrictions on the Coefficients Robert Gardner Brett Shields Department of Mathematics and Statistics Department of Mathematics and Statistics
Διαβάστε περισσότεραLecture 15 - Root System Axiomatics
Lecture 15 - Root System Axiomatics Nov 1, 01 In this lecture we examine root systems from an axiomatic point of view. 1 Reflections If v R n, then it determines a hyperplane, denoted P v, through the
Διαβάστε περισσότεραPartial Differential Equations in Biology The boundary element method. March 26, 2013
The boundary element method March 26, 203 Introduction and notation The problem: u = f in D R d u = ϕ in Γ D u n = g on Γ N, where D = Γ D Γ N, Γ D Γ N = (possibly, Γ D = [Neumann problem] or Γ N = [Dirichlet
Διαβάστε περισσότεραSolutions to Exercise Sheet 5
Solutions to Eercise Sheet 5 jacques@ucsd.edu. Let X and Y be random variables with joint pdf f(, y) = 3y( + y) where and y. Determine each of the following probabilities. Solutions. a. P (X ). b. P (X
Διαβάστε περισσότεραStrain gauge and rosettes
Strain gauge and rosettes Introduction A strain gauge is a device which is used to measure strain (deformation) on an object subjected to forces. Strain can be measured using various types of devices classified
Διαβάστε περισσότεραPROPERTIES OF CERTAIN INTEGRAL OPERATORS. a n z n (1.1)
GEORGIAN MATHEMATICAL JOURNAL: Vol. 2, No. 5, 995, 535-545 PROPERTIES OF CERTAIN INTEGRAL OPERATORS SHIGEYOSHI OWA Abstract. Two integral operators P α and Q α for analytic functions in the open unit disk
Διαβάστε περισσότεραA Two-Sided Laplace Inversion Algorithm with Computable Error Bounds and Its Applications in Financial Engineering
Electronic Companion A Two-Sie Laplace Inversion Algorithm with Computable Error Bouns an Its Applications in Financial Engineering Ning Cai, S. G. Kou, Zongjian Liu HKUST an Columbia University Appenix
Διαβάστε περισσότεραSection 9.2 Polar Equations and Graphs
180 Section 9. Polar Equations and Graphs In this section, we will be graphing polar equations on a polar grid. In the first few examples, we will write the polar equation in rectangular form to help identify
Διαβάστε περισσότεραLecture 34 Bootstrap confidence intervals
Lecture 34 Bootstrap confidence intervals Confidence Intervals θ: an unknown parameter of interest We want to find limits θ and θ such that Gt = P nˆθ θ t If G 1 1 α is known, then P θ θ = P θ θ = 1 α
Διαβάστε περισσότεραPARTIAL NOTES for 6.1 Trigonometric Identities
PARTIAL NOTES for 6.1 Trigonometric Identities tanθ = sinθ cosθ cotθ = cosθ sinθ BASIC IDENTITIES cscθ = 1 sinθ secθ = 1 cosθ cotθ = 1 tanθ PYTHAGOREAN IDENTITIES sin θ + cos θ =1 tan θ +1= sec θ 1 + cot
Διαβάστε περισσότεραEXISTENCE OF POSITIVE SOLUTIONS FOR SINGULAR FRACTIONAL DIFFERENTIAL EQUATIONS
Electronic Journal of Differential Equations, Vol. 28(28), No. 146, pp. 1 9. ISSN: 172-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu (login: ftp) EXISTENCE
Διαβάστε περισσότεραChapter 3: Ordinal Numbers
Chapter 3: Ordinal Numbers There are two kinds of number.. Ordinal numbers (0th), st, 2nd, 3rd, 4th, 5th,..., ω, ω +,... ω2, ω2+,... ω 2... answers to the question What position is... in a sequence? What
Διαβάστε περισσότεραSOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM
SOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM Solutions to Question 1 a) The cumulative distribution function of T conditional on N n is Pr T t N n) Pr max X 1,..., X N ) t N n) Pr max
Διαβάστε περισσότεραMATH423 String Theory Solutions 4. = 0 τ = f(s). (1) dτ ds = dxµ dτ f (s) (2) dτ 2 [f (s)] 2 + dxµ. dτ f (s) (3)
1. MATH43 String Theory Solutions 4 x = 0 τ = fs). 1) = = f s) ) x = x [f s)] + f s) 3) equation of motion is x = 0 if an only if f s) = 0 i.e. fs) = As + B with A, B constants. i.e. allowe reparametrisations
Διαβάστε περισσότεραNew bounds for spherical two-distance sets and equiangular lines
New bounds for spherical two-distance sets and equiangular lines Michigan State University Oct 8-31, 016 Anhui University Definition If X = {x 1, x,, x N } S n 1 (unit sphere in R n ) and x i, x j = a
Διαβάστε περισσότεραOptimal Parameter in Hermitian and Skew-Hermitian Splitting Method for Certain Two-by-Two Block Matrices
Optimal Parameter in Hermitian and Skew-Hermitian Splitting Method for Certain Two-by-Two Block Matrices Chi-Kwong Li Department of Mathematics The College of William and Mary Williamsburg, Virginia 23187-8795
Διαβάστε περισσότεραThe k-α-exponential Function
Int Journal of Math Analysis, Vol 7, 213, no 11, 535-542 The --Exponential Function Luciano L Luque and Rubén A Cerutti Faculty of Exact Sciences National University of Nordeste Av Libertad 554 34 Corrientes,
Διαβάστε περισσότεραOn a four-dimensional hyperbolic manifold with finite volume
BULETINUL ACADEMIEI DE ŞTIINŢE A REPUBLICII MOLDOVA. MATEMATICA Numbers 2(72) 3(73), 2013, Pages 80 89 ISSN 1024 7696 On a four-dimensional hyperbolic manifold with finite volume I.S.Gutsul Abstract. In
Διαβάστε περισσότεραThe Negative Neumann Eigenvalues of Second Order Differential Equation with Two Turning Points
Applied Mathematical Sciences, Vol. 3, 009, no., 6-66 The Negative Neumann Eigenvalues of Second Order Differential Equation with Two Turning Points A. Neamaty and E. A. Sazgar Department of Mathematics,
Διαβάστε περισσότερα5. Choice under Uncertainty
5. Choice under Uncertainty Daisuke Oyama Microeconomics I May 23, 2018 Formulations von Neumann-Morgenstern (1944/1947) X: Set of prizes Π: Set of probability distributions on X : Preference relation
Διαβάστε περισσότεραOn the Galois Group of Linear Difference-Differential Equations
On the Galois Group of Linear Difference-Differential Equations Ruyong Feng KLMM, Chinese Academy of Sciences, China Ruyong Feng (KLMM, CAS) Galois Group 1 / 19 Contents 1 Basic Notations and Concepts
Διαβάστε περισσότεραLecture 13 - Root Space Decomposition II
Lecture 13 - Root Space Decomposition II October 18, 2012 1 Review First let us recall the situation. Let g be a simple algebra, with maximal toral subalgebra h (which we are calling a CSA, or Cartan Subalgebra).
Διαβάστε περισσότερα