THE M/G/1 FEEDBACK RETRIAL QUEUE WITH TWO TYPES OF CUSTOMERS. Yong Wan Lee

Μέγεθος: px
Εμφάνιση ξεκινά από τη σελίδα:

Download "THE M/G/1 FEEDBACK RETRIAL QUEUE WITH TWO TYPES OF CUSTOMERS. Yong Wan Lee"

Transcript

1 Bull. Korean Math. Soc. 42 (2005), No. 4, pp THE M/G/1 FEEDBACK RETRIAL QUEUE WITH TWO TYPES OF CUSTOMERS Yong Wan Lee Abstract. In M/G/1 retrial queueing system with two types of customers and feedback, we derived the joint generating function of the number of customers in two groups by using the supplementary variable method. It is shown that our results are consistent with those already known in the literature when δ k = 0(k = 1, 2), λ 1 = 0 or λ 2 = Introduction In recent years there have been significant contributions to the retrial queueing system. Choi and Park3 investigated an M/G/1 retrial queue with two types of customers in which the service distributions for both types of customers are the same. Thereafter, Falin et al.7 investigate much the same model of Choi and Park3, in which they assumed different service distributions for both types of customers. Recently Choi et al.1 studied an M/G/1 retrial queueing system with two types of calls and finite capacity. In this paper we deal with feedback retrial queue with two types of customers where after being served each customer either joins the retrial group or departs the system permanently. The phenomena of feedback in the retrial queueing systems are occurred in many practical situation; for instance telecommunication system where message turned out error at destination sends again. In section 2, we describe the model. In section 3, we use the supplementary variable method to derive the joint generating function of the number of customers in the two groups and the mean queue size. Received November 11, Mathematics Subject Classification: 60K25, 90B22. Key words and phrases: feedback retrial queue, supplementary variable method, retrial time, stationary distribution. This work was supported by a grant from 2003 Research Fund of Andong National University.

2 876 Yong Wan Lee In section 4 we show that our results are consistent with those already known in the literature when δ k = 0 (k = 1, 2), λ 1 = 0 or λ 2 = Mathematical model We consider a single server queueing system in which two different types of customers arrive according to independent Poisson streams with rates λ 1 and λ 2, respectively. See the block diagram of feedback retrial queue with two types of customers in Figure 1. δ 1 Priority queue Poisson arrival(λ 1 ) Poisson arrival(λ 2 ) Server b 1 (x) b 2 (x) exp(ν) Retrial group Figure 1. M/G/1 feedback retrial queue with two types δ 2 1 δ 1 1 δ 2 Customers from the Poisson flow with rate λ 1 (the Poisson flow with rate λ 2, respectively) can be identified as priority customers (non-priority customers, respectively) in the system. If an arriving priority customer finds the server idle, he immediately starts to receive service. If he finds the server busy, he is queued in the priority group and then served in accordance with some discipline such as FCFS or random order. On the other hand, when an arriving non-priority customer finds the server idle, he obtains service immediately. If he finds the server busy, he joins the retrial group in order to seek service again after a random amount of time. He persists this way until he is eventually served. All the customers in the retrial group behave independently of each other. The retrial time (the time interval between two consecutive attempts made by a customer in the retrial group) is exponentially distributed with mean 1 ν and is independent of all previous retrial times and all other stochastic process in the system.

3 The M/G/1 feedback retrial queue with two types of customers 877 The service times of both types of customers are independent of each other. The service time B k has a general distribution with p.d.f. b k (x) and mean b k, k = 1, 2, where k = 1 is related to the priority customers and k = 2 is related to the non-priority customers. Let b k (θ) = 0 e θx b k (x)dx be the Laplace transform of service time B k, k = 1, 2. A priority customer who has received service departs the system with probability 1 δ 1 or return to the priority group for more service with probability δ 1. A non-priority customer who has received service leaves the system with probability 1 δ 2 or rejoins the retrial group with probability δ The joint distribution of queue sizes We define the following random variables in order to characterize our system at an arbitrary time; N 1 (t) = the number of customers in the priority group (excluding the customer in the service) at time t, N 2 (t) = the number of customers in the retrial group at time t, X(t) = the residual service time of the customer in the service at time t, 0, when serve is idle at time t, ξ(t) = 1, when server services the priority customer at time t, 2, when server services the non-priority customer at time t. Then the stochastic process X(t) = (ξ(t), N 1 (t), N 2 (t), X(t); t 0) is the Markovian process with state space {0, 1, 2} Z 2 + R + and denote by (ξ, N 1, N 2, X) the limiting random variable of (ξ(t), N 1 (t), N 2 (t), X(t)). We define the related probabilities; q j = P {ξ = 0, N 2 = j}, j = 0, 1, 2,... ; p kij (x)dx = P {ξ = k, N 1 = i, N 2 = j, X (x, x + dx}, k = 1, 2, i, j = 0, 1, 2,..., and x 0; and their Laplace transforms p kij (θ) = e θx p kij (x)d x, k = 1, 2, i, j = 0, 1, 2, Note that p kij (0) = 0 p kij (x)d x = P {ξ = k, N 1 = i, N 2 = j} is the steady state probability that there are i customers in the priority

4 878 Yong Wan Lee group, j customers in the retrial group and the server services the k- type customer. The usual arguments lead to the following system of difference equations; (1a) (1b) (1c) (1d) (λ 1 + λ 2 + jν)q j = (1 δ 1 )p 10j (0) + (1 δ 2 )p 20j (0) + δ 2 p 20j 1 (0), p 10j(x) = (λ 1 + λ 2 )p 10j (x) + λ 1 b 1 (x)q j + λ 2 p 10j 1 (x) + δ 1 b 1 (x)p 10j (0) + (1 δ 1 )b 1 (x)p 11j (0) + δ 2 b 1 (x)p 21j 1 (0) + (1 δ 2 )b 1 (x)p 21j (0), p 1ij(x) = (λ 1 + λ 2 )p 1ij (x) + λ 1 p 1i 1j (x) + λ 2 p 1ij 1 (x) + δ 1 b 1 (x)p 1ij (0) + (1 δ 1 )b 1 (x)p 1i+1j (0) + δ 2 b 1 (x)p 2i+1j 1 (0) + (1 δ 2 )b 1 (x)p 2i+1j (0), p 20j(x) = (λ 1 + λ 2 )p 20j (x) + λ 2 b 2 (x)q j + (j + 1)νb 2 (x)q j+1 + λ 2 p 20j 1 (x), (1e) p 2ij(x) = (λ 1 + λ 2 )p 2ij (x) + λ 1 p 2i 1j (x) + λ 2 p 2ij 1 (x) + λ 2 p 2ij 1 (x), where i = 1, 2,..., j = 0, 1, 2,..., p kij = 0 for i, j < 0, k = 1, 2 and any x 0. By taking Laplace transform (1b) (1e), we obtain (2b) (2c) (2d) {θ (λ 1 + λ 2 )}p 10j(θ) + λ 2 p 10j 1(θ) = p 10j (0) λ 1 b 1(θ)q j δ 1 b 1(θ)p 10j (0) (1 δ 1 )b 1(θ)p 11j (0) δ 2 b 1(θ)p 21j 1 (0) (1 δ 2 )b 1(θ)p 21j (0), {θ (λ 1 +λ 2 )}p 1ij(θ) + λ 1 p 1i 1j(θ) + λ 2 p 1ij 1(θ) = p 1ij (0) δ 1 b 1(θ)p 1ij (0) (1 δ 1 )b 1(θ)p 1i+1j (0) δ 2 b 1(θ)p 2i+1j 1(0) (1 δ 2 )b 1(θ)p 2i+1j (0), {θ (λ 1 + λ 2 )}p 20j(θ) + λ 2 p 20j 1(θ) = p 20j (0) λ 2 b 2(θ)q j (j + 1)νb 2(θ)q j+1, (2e) {θ (λ 1 + λ 2 )}p 2ij(θ) + λ 1 p 2i 1j(θ) + λ 2 p 2ij 1(θ) = p 2ij (0).

5 The M/G/1 feedback retrial queue with two types of customers 879 We introduce the following generating function for complex z with z 1, Q( ) = q j z j 2, P ki (θ, ) = P ki (0, ) = j=0 j=0 j=0 p kij (θ)zj 2, k = 1, 2, p kij (0)z j 2, k = 1, 2. Multiplying equations (1a) and (2b) (2e) by z j 2 and summing over all j, we obtain the following basic system equations; (3a) (λ 1 + λ 2 )Q( ) + ν Q ( ) = (1 δ 1 )P 10 (0, ) + (1 δ 2 + δ 2 )P 20 (0, ), (3b) (3c) (3d) {θ (λ 1 + λ 2 ) + λ 2 }P10(θ, ) = (1 δ 1 b 1(θ))P 10 (0, ) λ 1 b 1(θ)Q( ) (1 δ 1 )b 1(θ)P 11 (0, ) (1 δ 2 + δ 2 )b 1(θ)P 21 (0, ), {θ (λ 1 +λ 2 ) + λ 2 }P1i(θ, ) + λ 1 P1i 1(θ, ) = (1 δ 1 b 1(θ))P 1i (0, ) (1 δ 1 )b 1(θ)P 1i+1 (0, ) (1 δ 2 + δ 2 )b 1(θ)P 2i+1 (0, ), {θ (λ 1 + λ 2 )+λ 2 }P20(θ, ) = P 20 (0, ) λ 2 b 2(θ)Q( ) νb 2(θ)Q ( ), (3e) {θ (λ 1 + λ 2 ) + λ 2 }P2i(θ, ) + λ 1 P2i 1(θ, ) = P 2i (0, ). Define the generating functions of Pk (θ,, ) and P k (0,, ) for k = 1, 2 as follows; Pk (θ,, ) = Pki (θ, )z1, i i=0 P k (0,, ) = P ki (0, )z1. i i=0 Note that Pk (0,, ) = E(z N 1 1 zn 2 2 ; ξ = k) which is the joint generating function of (N 1, N 2 ) when the server services the k-type customer.

6 880 Yong Wan Lee Multiplying equations (3b) (3e) by z1 i obtain and summing over all i, we (4a) (4b) {θ λ 1 (1 ) λ 2 (1 )}P 1 (θ,, ) = {1 δ 1 b 1(θ) (1 δ 1)b 1 (θ) }P 1 (0,, ) (1 δ 2 + δ 2 )b 1 (θ) P 2 (0,, ) + (1 δ 1)b 1 (θ) P 10 (0, ) + (1 δ 2 + δ 2 )b 1 (θ) P 20 (0, ) λ 1 b z 1(θ)Q( ), 1 {θ λ 1 (1 ) λ 2 (1 )}P 2 (θ,, ) = P 2 (0,, ) λ 2 b 2(θ)Q( ) νb 2(θ)Q ( ). By choosing θ = λ 1 (1 ) + λ 2 (1 )into (4a) and (4b), we eliminate P 1 (θ,, ) and P 2 (θ,, ) from (4a) and (4b) respectively and obtain (5) { (1 δ 1 + δ 1 )β 1 (, )}P 1 (0,, ) = β 1 (, ){(1 δ 2 + δ 2 )P 2 (0,, ) + λ 1 Q( ) (1 δ 1 )P 10 (0, ) (1 δ 2 + δ 2 )P 20 (0, )}, (6) P 2 (0,, ) = β 2 (, ){λ 2 Q( ) + νq ( )}, where β k (, ) = b k (λ 1(1 ) + λ 2 (1 )), k = 1, 2. Now we consider the function (7) h(, ) = (1 δ 1 + δ 1 )β 1 (, ). By using Rouche s theorem it follows that for each with < 1, there is a unique solution = φ( ) of the equation h(, ) = 0 in the unit circle, i.e., h(φ( ), ) = φ( ) (1 δ 1 + δ 1 φ( ))β 1 (φ( ), ) = 0. On the other hand, since h(, ) = 1 (δ 1 + λ 1 b 1 ) > 0, z1 = =1 we conclude that = φ( ) is analytic on < 1 and is continuous at = 1 and φ(1) = 1 by the implicit function theorem. It is necessary

7 The M/G/1 feedback retrial queue with two types of customers 881 to know the first and second derivatives of φ( ) at = 1 for late use. These are derived as follows φ λ 2 b 1 (1) = 1 (δ 1 + λ 1 b 1 ), (8) φ (1) = 2δ 1(1 δ 1 )λ 2 2 b2 1 + (1 δ 1) 2 λ 2 2 E(b2 1 ) {1 (δ 1 + λ 1 b 1 )} 3. By substituting = φ( ) into (5), P 1 (0,, ) is eliminated, and we get (9) (1 δ 2 + δ 2 )P 2 (0, φ( ), ) + λ 1 φ( )Q( ) = (1 δ 1 )P 10 (0, ) + (1 δ 2 + δ 2 )P 20 (0, ). By substituting = φ( ) into (6), we obtain (10) P 2 (0, φ( ), ) = β 2 (φ( ), ){λ 2 Q( ) + νq ( )}. From (9) and (10), we obtain (11) (1 δ 1 )P 10 (0, ) + (1 δ 2 + δ 2 )P 20 (0, ) = {λ 1 φ( ) + (1 δ 2 + δ 2 )λ 2 β 2 (φ( ), )}Q( ) + (1 δ 2 + δ 2 )νβ 2 (φ( ), )Q ( ). By equating (3a) and (11), we obtain the differential equation (12) Q 1 ( ) = ν{(1 δ 2 + δ 2 )β 2 (φ( ), ) } λ 1 (1 φ( )) + λ 2 {1 (1 δ 2 + δ 2 )β 2 (φ( ), )} Q( ), whose solution is (13) ν (1 δ 2 + δ 2 x)β 2 (φ(x), x) x Q( ) = C exp {λ 1 (1 φ(x)) + λ 2 {1 (1 δ 2 + δ 2 x)β 2 (φ(x), x)}}d x. Substituting (12) into (6) yields (14) P 2 (0,, ) = {λ 1(1 φ( )) + λ 2 (1 )}β 2 (, ) (1 δ 2 + δ 2 )β 2 (φ( ), ) Q( ).

8 882 Yong Wan Lee Substituting (11), (12), and (14) into (5) yields (15) (1 δ 2 + δ 2 ) P 1 (0,, ) = β 1 (, ) (1 δ 2 + δ 2 )β 2 (φ( ), ) {λ 1(1 φ( )) + λ 2 (1 )}{β 2 (φ( ), ) β 2 (, )} (1 δ 1 + δ 1 )β 1 (, ) λ 1 (φ( ) ) + Q( ). (1 δ 1 + δ 1 )β 1 (, ) Finally, we will calculate P k (0,, ). Letting θ = 0 in (4a) and (4b) gives (16) {λ 1 (1 ) + λ 2 (1 )}P1 (0,, ) ( = 1 δ 1 1 δ ) 1 P 1 (0,, ) 1 δ 2 + δ 2 P 2 (0,, ) + 1 δ 1 P 10 (0, ) + 1 δ 2 + δ 2 P 20 (0, ) λ 1 Q( ), (17) {λ 1 (1 ) + λ 2 (1 )}P 2 (0,, ) = P 2 (0,, ) λ 2 Q( ) νq ( ). We obtain from (16) using (11), (14), and (15) (18) P1 β 1 (, ) 1 λ 1 (φ( ) ) (0,, ) = λ 1 ( 1) + λ 2 ( 1) (1 δ 1 + δ 1 )β 1 (, ) + (1 δ 2 + δ 2 ){λ 1 (1 φ( )) + λ 2 (1 )} (1 δ 2 + δ 2 )β 2 (φ( ), ) β 2(φ( ), ) β 2 (, ) Q( ). (1 δ 1 + δ 1 )β 1 (, ) From (12), (14), and (17), we obtain (19) P2 (0,, ) = {λ 1(1 φ( )) + λ 2 (1 )}{1 β 2 (, )} (1 δ 2 + δ 2 )β 2 (φ( ), ) Q( ) λ 1 (1 ) + λ 2 (1 ). To determine C, we need to find P k (0, 1, 1), k = 1, 2. First letting 1 and then 1 in (18) and (19). Using φ(1) = 1 and (8) we obtain by

9 The M/G/1 feedback retrial queue with two types of customers 883 the L Hospital rule that (20) P1 (0, 1, 1) = lim C β(z 1, 1) 1 λ 1 (1 ) z1 1 λ 1 ( 1) (1 δ 1 + δ 1 )β 1 (, 1) 1 β 2 (, 1) λ 1 φ (1) λ 2 + (1 δ 1 + δ 1 )β 1 (, 1) δ 2 + (λ 1 φ (1) + λ 2 )b 2 1 = C λ 1 b 1 (1 δ 2 ){1 (δ 1 + λ 1 b 1 )} {1 (δ 1 + λ 1 b 1 )}(1 δ 2 ){1 (δ 1 + λ 1 b 1 )} λ 2 b 2 (1 δ 1 ), (21) P2 (0, 1, 1) = lim C 1 β 2(, 1) λ 1 φ (1) λ 2 z1 1 λ 1 (1 ) δ 2 + (λ 1 φ (1) + λ 2 )b 2 1 λ 2 b 2 (1 δ 1 ) = C (1 δ 2 ){1 (δ 1 + λ 1 b 1 )} λ 2 b 2 (1 δ 1 ). From the total probability Q(1) + P1 (0, 1, 1) + P 2 (0, 1, 1) = 1, we obtain C = (1 δ 2){1 (δ 1 + λ 1 b 1 )} λ 2 b 2 (1 δ 1 ) (1 δ 1 ){1 (δ 1 + λ 1 b 1 )} + λ 1 b 1 (1 δ 2 ), that is, the probability that the server is idle, and P 1 (0, 1, 1) + P 2 (0, 1, 1) = (1 δ 1){1 (δ 1 + λ 1 b 1 ) + λ 2 b 2 } (1 δ 2 )(1 δ 1 2λ 1 b 1 ) (1 δ 1 ){1 (δ 1 + λ 1 b 1 )} + λ 1 b 1 (1 δ 2 ) as the probability that the server is busy. Thus we have the theorem. Theorem 3.1. The stationary distribution of (ξ, N 1, N 2 ) has the following generating functions (22) Q( ) = E(z N 2 2 ; ξ = 0) = (1 δ 2){1 (δ 1 + λ 1 b 1 )} λ 2 b 2 (1 δ 1 ) (1 δ 1 ){1 (δ 1 + λ 1 b 1 )} + λ 1 b 1 (1 δ 2 ) exp 1 1 ν 1 (1 δ 2 + δ 2 x)β 2 (φ(x), x) x { λ 1 (1 φ(x)) + λ 2 {1 (1 δ 2 + δ 2 x)β 2 (φ(x), x)} } d x,

10 884 Yong Wan Lee (23) P 1 (0,, ) = E(z N 1 1 zn 2 2 ; ξ = 1) = (1 δ 2){1 (δ 1 + λ 1 b 1 )} λ 2 b 2 (1 δ 1 ) (1 δ 1 ){1 (δ 1 + λ 1 b 1 )} + λ 1 b 1 (1 δ 2 ) β 1 (, ) 1 λ 1 (φ( ) ) λ 1 ( 1) + λ 2 ( 1) (1 δ 1 + δ 1 )β 1 (, ) + (1 δ 2 + δ 2 ){λ 1 (1 φ( )) + λ 2 (1 )} {(1 δ 1 + δ 1 )β 1 (, ) )} {β 2 (φ( ), ) β 2 (, )} {(1 δ 2 + δ 2 )β 2 (φ( ), ) } exp 1 1 λ 1 (1 φ(x)) + λ 2 {1 (1 δ 2 + δ 2 x)β 2 (φ(x), x)} d x, ν (1 δ 2 + δ 2 x)β 2 (φ(x), x) x (24) P 2 (0,, ) = E(z N 1 1 zn 2 2 : ξ = 2) = (1 δ 2){1 (δ 1 + λ 1 b 1 )} λ 2 b 2 (1 δ 1 ) (1 δ 1 ){1 (δ 1 + λ 1 b 1 )} + λ 1 b 1 (1 δ 2 ) {λ 1 (1 φ( )) + λ 2 (1 )}{1 β 2 (, )} {λ 1 (1 ) + λ 2 (1 )}{(1 δ 2 + δ 2 )β 2 (φ( ), ) } exp 1 1 λ 1 (1 φ(x)) + λ 2 {1 (1 δ 2 + δ 2 x)β 2 (φ(x), x)} d x. ν (1 δ 2 + δ 2 x)β 2 (φ(x), x) x 4. Special cases (a) When δ k = 0 k = 1, 2, our model becomes the M/G/1 retrial queueing system with priority customers studied by Falin, Artalejo and Martin7. In this case, equations (22), (23), and (24) reduce to Q( ) = E(z N 2 2 ; ξ = 0) = {1 (λ 1b 1 + λ 2 b 2 )} exp 1 1 λ 1 (1 φ(x)) + λ 2 (1 b 2 (λ 1 + λ 2 λ 1 φ(x) λ 2 x)) ν b 2 (λ d x, 1 + λ 2 λ 1 φ(x) λ 2 x) x P1 (0,, ) = E(z N 1 1 zn 2 2 ; ξ = 1) λ 1 (φ( ) ) = b 1 (λ + λ 1(1 φ( )) + λ 2 (1 ) 1 + λ 2 λ 1 λ 2 ) b 1 (λ 1 + λ 2 λ 1 λ 2 ) b 2 (λ 1 + λ 2 λ 1 φ( ) λ 2 ) b 2 (λ 1 + λ 2 λ 1 λ 2 ) b 2 (λ Q( ), 1 + λ 2 φ( ) λ 2 )

11 The M/G/1 feedback retrial queue with two types of customers 885 P 2 (0,, ) = E(z N 1 1 zn 2 2 ; ξ = 2) = λ 1(1 φ( )) + λ 2 (1 ) λ 1 (1 ) + λ 2 (1 ) 1 b 2 (λ 1 + λ 2 λ 1 λ 2 ) b 2 (λ Q( ), 1 + λ 2 λ 1 φ( ) λ 2 ) which agree with Theorem 3 in Falin, Artalejo and Martin7. (b) When b k (x) = b(x) and δ k = 0, k = 1, 2, our model becomes the M/G/1 retrial queue with Bernoulli schedule with λ 1 = qλ and λ 2 = pλ(q = 1 p) studied by Choi and Park3. In this case φ( ) = b (λ λqφ( ) λp ), equations (22), (23), and (24) reduce to E(z N 2 2 ; ξ = 0) = (1 λb) exp λ 1 1 φ(x) ν φ(x) x d x, E(z N 1 1 zn 2 2 ; ξ 0) = (1 (λ qλ pλ ) 1 λb)b q + p 1 φ( ) b (λ qλ pλ ) 1 φ( ) exp which agree with Theorem in Choi and Park 3. λ ν 1 1 φ(x) φ(x) x d x, (c) When λ 1 = 0 and δ k = 0, k = 1, 2, our model becomes the M/G/1 retrial queue. In this case N 1 = 0. Equations (22), (23), and (24) reduce to E(z N 2 2 ; ξ = 0) = (1 λ 2b 2 ) exp λ b 2 (λ 2 λ 2 x) ν b 2 (λ 2 λ 2 x) x d x, E(z N 2 2 ; ξ = 2) = (1 λ 2b 2 ) 1 b 2 (λ 2 λ 2 ) b 2 (λ 2 λ 2 ) exp λ 2 ν 1 1 b 2 (λ 2 λ 2 x) b 2 (λ 2 λ 2 x) x d x which agree with Theorem 6 in Falin5. The generating function of queue length in the system is E(z N 2 2 ; ξ = 0) + E(z N 2 2 ; ξ = 2) which equals (1 λ 2 b 2 )(1 )b 2 (λ 2 λ 2 ) b 2 (λ exp λ b 2 (λ 2 λ 2 x) 2 λ 2 ) ν b 2 (λ 2 λ 2 x) x d x. This result agree with (3.11) in Yang and Templeton9. (d) When λ 2 = 0 and δ k = 0, k = 1, 2, our model becomes the ordinary M/G/1 queue. In this case φ( ) = b 1 (λ 1 λ 1 ), N 2 = 0. Equations (22) and (23) reduce to,

12 886 Yong Wan Lee P (ξ = 0) = 1 λ 1 b 1, E(z N 1 1 ; ξ = 1) = (1 λ 1b 1 ) b 1 (λ 1 λ 1 ) 1 b 1 (λ 1 λ 1 ). The generating function of the queue length in the system is Q(1) + P (0,, 1) which equals (1 λ 1 b 1 )( 1)b 1 (λ 1 λ 1 ) b 1 (λ. 1 λ 1 ) This is the Pollaczek-Khinchin formula. (e) When λ 1 = 0, our model becomes the M/G/1 feedback retrial queue. In this case φ( ) = b 1 (λ 2 λ 2 ), N 1 = 0. Equation (22) and (23) reduce to E(z N 2 2 ; ξ = 0) = {1 (δ 2 + λ 2 b 2 )} exp λ (1 δ 2 + δ 2 x)b 2 (λ 2 λ 2 x) ν (1 δ 2 + δ 2 x)b 2 (λ 2 λ 2 x) x d x, E(z N 2 2 ; ξ = 2) = {1 (δ 2 + λ 2 b 2 )}{1 b 2 (λ 2 λ 2 )} (1 δ 2 + δ 2 )b 2 (λ 2 λ 2 ) exp λ 2 ν 1 1 (1 δ 2 + δ 2 x)b 2 (λ 2 λ 2 x) (1 δ 2 + δ 2 x)b 2 (λ 2 λ 2 x) x d x. References 1 B. D. Choi, K. B. Choi, and Y. W. Lee, M/G/1 retrial queueing system with two types of calls and finite capacity, Queueing Systems 19 (1995), B. D. Choi and V. G. Kulkarni, Feedback retrial queueing system, Stochastic Model Related field (1992), B. D. Choi and K. K. Park, The M/G/1 retrial queue with Bernoulli schedule, Queueing Systems 7 (1990), B. D. Choi, K. K. Park, and Y. W. Lee, Retrial queues with Bernoulli feedback, Proc. Workshops Math. Phys. 2 (1990), G. I. Falin, A single-line system with secondary orders, Engineering Cybernet. 17 (1979), no. 2, G. I. Falin, A survey of retrial queues, Queueing systems 7 (1990), G. I. Falin, J. R. Artalejo, and M. Martin, On the single server retrial queue with priority customers, Queueing systems 14 (1993), D. Gross and C. M. Harris, Foundamentals of Queueing Theory, John Wiley and Sons, 1985.

13 The M/G/1 feedback retrial queue with two types of customers T. Yang and J. G. C. Templeton, A survey on retrial queues, Queueing systems 2 (1987), Department of Mathematics Education, Andong National University, Kyungbuk , Korea ywlee@andong.ac.kr

2 Composition. Invertible Mappings

2 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 περισσότερα

Phys460.nb Solution for the t-dependent Schrodinger s equation How did we find the solution? (not required)

Phys460.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 περισσότερα

HOMEWORK 4 = G. In order to plot the stress versus the stretch we define a normalized stretch:

HOMEWORK 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 περισσότερα

4.6 Autoregressive Moving Average Model ARMA(1,1)

4.6 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 περισσότερα

Jesse Maassen and Mark Lundstrom Purdue University November 25, 2013

Jesse 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 περισσότερα

Homework 3 Solutions

Homework 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 περισσότερα

5.4 The Poisson Distribution.

5.4 The Poisson Distribution. The worst thing you can do about a situation is nothing. Sr. O Shea Jackson 5.4 The Poisson Distribution. Description of the Poisson Distribution Discrete probability distribution. The random variable

Διαβάστε περισσότερα

Math221: HW# 1 solutions

Math221: 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 περισσότερα

3.4 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. 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 περισσότερα

Areas and Lengths in Polar Coordinates

Areas 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 περισσότερα

Areas and Lengths in Polar Coordinates

Areas 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 περισσότερα

Section 8.3 Trigonometric Equations

Section 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 περισσότερα

Congruence Classes of Invertible Matrices of Order 3 over F 2

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 περισσότερα

Απόκριση σε Μοναδιαία Ωστική Δύναμη (Unit Impulse) Απόκριση σε Δυνάμεις Αυθαίρετα Μεταβαλλόμενες με το Χρόνο. Απόστολος Σ.

Απόκριση 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 περισσότερα

forms This gives Remark 1. How to remember the above formulas: Substituting these into the equation we obtain with

forms 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 περισσότερα

Example Sheet 3 Solutions

Example 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 περισσότερα

derivation of the Laplacian from rectangular to spherical coordinates

derivation 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 περισσότερα

Concrete Mathematics Exercises from 30 September 2016

Concrete 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 περισσότερα

Solutions to Exercise Sheet 5

Solutions 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 περισσότερα

Fourier Series. MATH 211, Calculus II. J. Robert Buchanan. Spring Department of Mathematics

Fourier 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 περισσότερα

D Alembert s Solution to the Wave Equation

D 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 περισσότερα

Second Order Partial Differential Equations

Second 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 περισσότερα

ST5224: Advanced Statistical Theory II

ST5224: 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 περισσότερα

Other Test Constructions: Likelihood Ratio & Bayes Tests

Other 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 περισσότερα

SCITECH Volume 13, Issue 2 RESEARCH ORGANISATION Published online: March 29, 2018

SCITECH 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 περισσότερα

Homework 8 Model Solution Section

Homework 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 περισσότερα

SOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM

SOLUTIONS 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 περισσότερα

Partial Differential Equations in Biology The boundary element method. March 26, 2013

Partial 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 περισσότερα

EE512: Error Control Coding

EE512: 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 περισσότερα

Queueing Theory I. Summary. Little s Law Queueing System Notation Stationary Analysis of Elementary Queueing Systems. M/M/1 M/M/m M/M/1/K

Queueing Theory I. Summary. Little s Law Queueing System Notation Stationary Analysis of Elementary Queueing Systems. M/M/1 M/M/m M/M/1/K Queueing Theory I Suary Little s Law Queueing Syste Notation Stationary Analysis of Eleentary Queueing Systes M/M/ M/M/ M/M// Little s Law a(t): the process that counts the nuber of arrivals up to t. d(t):

Διαβάστε περισσότερα

Matrices and Determinants

Matrices 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 περισσότερα

Statistical Inference I Locally most powerful tests

Statistical 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 περισσότερα

C.S. 430 Assignment 6, Sample Solutions

C.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 περισσότερα

The Simply Typed Lambda Calculus

The 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 περισσότερα

Homomorphism in Intuitionistic Fuzzy Automata

Homomorphism 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 περισσότερα

Exercises 10. Find a fundamental matrix of the given system of equations. Also find the fundamental matrix Φ(t) satisfying Φ(0) = I. 1.

Exercises 10. Find a fundamental matrix of the given system of equations. Also find the fundamental matrix Φ(t) satisfying Φ(0) = I. 1. Exercises 0 More exercises are available in Elementary Differential Equations. If you have a problem to solve any of them, feel free to come to office hour. Problem Find a fundamental matrix of the given

Διαβάστε περισσότερα

Solution Series 9. i=1 x i and i=1 x i.

Solution Series 9. i=1 x i and i=1 x i. Lecturer: Prof. Dr. Mete SONER Coordinator: Yilin WANG Solution Series 9 Q1. Let α, β >, the p.d.f. of a beta distribution with parameters α and β is { Γ(α+β) Γ(α)Γ(β) f(x α, β) xα 1 (1 x) β 1 for < x

Διαβάστε περισσότερα

Ordinal Arithmetic: Addition, Multiplication, Exponentiation and Limit

Ordinal 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 περισσότερα

Chapter 6: Systems of Linear Differential. be continuous functions on the interval

Chapter 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 περισσότερα

SCHOOL OF MATHEMATICAL SCIENCES G11LMA Linear Mathematics Examination Solutions

SCHOOL 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 περισσότερα

CHAPTER 25 SOLVING EQUATIONS BY ITERATIVE METHODS

CHAPTER 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 περισσότερα

Appendix to On the stability of a compressible axisymmetric rotating flow in a pipe. By Z. Rusak & J. H. Lee

Appendix 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 περισσότερα

Problem Set 3: Solutions

Problem 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 περισσότερα

On a four-dimensional hyperbolic manifold with finite volume

On 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 περισσότερα

6.3 Forecasting ARMA processes

6.3 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 περισσότερα

CHAPTER 48 APPLICATIONS OF MATRICES AND DETERMINANTS

CHAPTER 48 APPLICATIONS OF MATRICES AND DETERMINANTS CHAPTER 48 APPLICATIONS OF MATRICES AND DETERMINANTS EXERCISE 01 Page 545 1. Use matrices to solve: 3x + 4y x + 5y + 7 3x + 4y x + 5y 7 Hence, 3 4 x 0 5 y 7 The inverse of 3 4 5 is: 1 5 4 1 5 4 15 8 3

Διαβάστε περισσότερα

Every set of first-order formulas is equivalent to an independent set

Every 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 περισσότερα

( y) Partial Differential Equations

( 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 περισσότερα

A Bonus-Malus System as a Markov Set-Chain. Małgorzata Niemiec Warsaw School of Economics Institute of Econometrics

A Bonus-Malus System as a Markov Set-Chain. Małgorzata Niemiec Warsaw School of Economics Institute of Econometrics A Bonus-Malus System as a Markov Set-Chain Małgorzata Niemiec Warsaw School of Economics Institute of Econometrics Contents 1. Markov set-chain 2. Model of bonus-malus system 3. Example 4. Conclusions

Διαβάστε περισσότερα

Econ 2110: Fall 2008 Suggested Solutions to Problem Set 8 questions or comments to Dan Fetter 1

Econ 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

SOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM

SOLUTIONS 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 περισσότερα

Srednicki Chapter 55

Srednicki 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 περισσότερα

Bayesian statistics. DS GA 1002 Probability and Statistics for Data Science.

Bayesian statistics. DS GA 1002 Probability and Statistics for Data Science. Bayesian statistics DS GA 1002 Probability and Statistics for Data Science http://www.cims.nyu.edu/~cfgranda/pages/dsga1002_fall17 Carlos Fernandez-Granda Frequentist vs Bayesian statistics In frequentist

Διαβάστε περισσότερα

Finite Field Problems: Solutions

Finite 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 περισσότερα

Section 7.6 Double and Half Angle Formulas

Section 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 περισσότερα

The challenges of non-stable predicates

The challenges of non-stable predicates The challenges of non-stable predicates Consider a non-stable predicate Φ encoding, say, a safety property. We want to determine whether Φ holds for our program. The challenges of non-stable predicates

Διαβάστε περισσότερα

b. Use the parametrization from (a) to compute the area of S a as S a ds. Be sure to substitute for ds!

b. Use the parametrization from (a) to compute the area of S a as S a ds. Be sure to substitute for ds! MTH U341 urface Integrals, tokes theorem, the divergence theorem To be turned in Wed., Dec. 1. 1. Let be the sphere of radius a, x 2 + y 2 + z 2 a 2. a. Use spherical coordinates (with ρ a) to parametrize.

Διαβάστε περισσότερα

Coefficient Inequalities for a New Subclass of K-uniformly Convex Functions

Coefficient 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 περισσότερα

Parametrized Surfaces

Parametrized Surfaces Parametrized Surfaces Recall from our unit on vector-valued functions at the beginning of the semester that an R 3 -valued function c(t) in one parameter is a mapping of the form c : I R 3 where I is some

Διαβάστε περισσότερα

ω 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

ω 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 περισσότερα

Fractional Colorings and Zykov Products of graphs

Fractional 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 περισσότερα

ANSWERSHEET (TOPIC = DIFFERENTIAL CALCULUS) COLLECTION #2. h 0 h h 0 h h 0 ( ) g k = g 0 + g 1 + g g 2009 =?

ANSWERSHEET (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 περισσότερα

Second Order RLC Filters

Second 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 περισσότερα

Mock Exam 7. 1 Hong Kong Educational Publishing Company. Section A 1. Reference: HKDSE Math M Q2 (a) (1 + kx) n 1M + 1A = (1) =

Mock Exam 7. 1 Hong Kong Educational Publishing Company. Section A 1. Reference: HKDSE Math M Q2 (a) (1 + kx) n 1M + 1A = (1) = Mock Eam 7 Mock Eam 7 Section A. Reference: HKDSE Math M 0 Q (a) ( + k) n nn ( )( k) + nk ( ) + + nn ( ) k + nk + + + A nk... () nn ( ) k... () From (), k...() n Substituting () into (), nn ( ) n 76n 76n

Διαβάστε περισσότερα

Probability and Random Processes (Part II)

Probability and Random Processes (Part II) Probability and Random Processes (Part II) 1. If the variance σ x of d(n) = x(n) x(n 1) is one-tenth the variance σ x of a stationary zero-mean discrete-time signal x(n), then the normalized autocorrelation

Διαβάστε περισσότερα

Approximation of distance between locations on earth given by latitude and longitude

Approximation 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 περισσότερα

Section 9.2 Polar Equations and Graphs

Section 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 περισσότερα

6.1. Dirac Equation. Hamiltonian. Dirac Eq.

6.1. 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 περισσότερα

Practice Exam 2. Conceptual Questions. 1. State a Basic identity and then verify it. (a) Identity: Solution: One identity is csc(θ) = 1

Practice 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 περισσότερα

Chapter 6: Systems of Linear Differential. be continuous functions on the interval

Chapter 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 περισσότερα

ES440/ES911: CFD. Chapter 5. Solution of Linear Equation Systems

ES440/ES911: CFD. Chapter 5. Solution of Linear Equation Systems ES440/ES911: CFD Chapter 5. Solution of Linear Equation Systems Dr Yongmann M. Chung http://www.eng.warwick.ac.uk/staff/ymc/es440.html Y.M.Chung@warwick.ac.uk School of Engineering & Centre for Scientific

Διαβάστε περισσότερα

CHAPTER 101 FOURIER SERIES FOR PERIODIC FUNCTIONS OF PERIOD

CHAPTER 101 FOURIER SERIES FOR PERIODIC FUNCTIONS OF PERIOD CHAPTER FOURIER SERIES FOR PERIODIC FUNCTIONS OF PERIOD EXERCISE 36 Page 66. Determine the Fourier series for the periodic function: f(x), when x +, when x which is periodic outside this rge of period.

Διαβάστε περισσότερα

w o = R 1 p. (1) R = p =. = 1

w o = R 1 p. (1) R = p =. = 1 Πανεπιστήµιο Κρήτης - Τµήµα Επιστήµης Υπολογιστών ΗΥ-570: Στατιστική Επεξεργασία Σήµατος 205 ιδάσκων : Α. Μουχτάρης Τριτη Σειρά Ασκήσεων Λύσεις Ασκηση 3. 5.2 (a) From the Wiener-Hopf equation we have:

Διαβάστε περισσότερα

ΚΥΠΡΙΑΚΗ ΕΤΑΙΡΕΙΑ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 19/5/2007

ΚΥΠΡΙΑΚΗ ΕΤΑΙΡΕΙΑ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 19/5/2007 Οδηγίες: Να απαντηθούν όλες οι ερωτήσεις. Αν κάπου κάνετε κάποιες υποθέσεις να αναφερθούν στη σχετική ερώτηση. Όλα τα αρχεία που αναφέρονται στα προβλήματα βρίσκονται στον ίδιο φάκελο με το εκτελέσιμο

Διαβάστε περισσότερα

k A = [k, k]( )[a 1, a 2 ] = [ka 1,ka 2 ] 4For the division of two intervals of confidence in R +

k 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 περισσότερα

The k-α-exponential Function

The 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 περισσότερα

Lecture 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 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 περισσότερα

[1] P Q. Fig. 3.1

[1] P Q. Fig. 3.1 1 (a) Define resistance....... [1] (b) The smallest conductor within a computer processing chip can be represented as a rectangular block that is one atom high, four atoms wide and twenty atoms long. One

Διαβάστε περισσότερα

Uniform Convergence of Fourier Series Michael Taylor

Uniform 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 περισσότερα

Inverse trigonometric functions & General Solution of Trigonometric Equations. ------------------ ----------------------------- -----------------

Inverse 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 περισσότερα

Potential Dividers. 46 minutes. 46 marks. Page 1 of 11

Potential Dividers. 46 minutes. 46 marks. Page 1 of 11 Potential Dividers 46 minutes 46 marks Page 1 of 11 Q1. In the circuit shown in the figure below, the battery, of negligible internal resistance, has an emf of 30 V. The pd across the lamp is 6.0 V and

Διαβάστε περισσότερα

The Probabilistic Method - Probabilistic Techniques. Lecture 7: The Janson Inequality

The Probabilistic Method - Probabilistic Techniques. Lecture 7: The Janson Inequality The Probabilistic Method - Probabilistic Techniques Lecture 7: The Janson Inequality Sotiris Nikoletseas Associate Professor Computer Engineering and Informatics Department 2014-2015 Sotiris Nikoletseas,

Διαβάστε περισσότερα

Higher Derivative Gravity Theories

Higher Derivative Gravity Theories Higher Derivative Gravity Theories Black Holes in AdS space-times James Mashiyane Supervisor: Prof Kevin Goldstein University of the Witwatersrand Second Mandelstam, 20 January 2018 James Mashiyane WITS)

Διαβάστε περισσότερα

Differential equations

Differential equations Differential equations Differential equations: An equation inoling one dependent ariable and its deriaties w. r. t one or more independent ariables is called a differential equation. Order of differential

Διαβάστε περισσότερα

Strain gauge and rosettes

Strain 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 περισσότερα

Lecture 2. Soundness and completeness of propositional logic

Lecture 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 περισσότερα

Problem Set 9 Solutions. θ + 1. θ 2 + cotθ ( ) sinθ e iφ is an eigenfunction of the ˆ L 2 operator. / θ 2. φ 2. sin 2 θ φ 2. ( ) = e iφ. = e iφ cosθ.

Problem Set 9 Solutions. θ + 1. θ 2 + cotθ ( ) sinθ e iφ is an eigenfunction of the ˆ L 2 operator. / θ 2. φ 2. sin 2 θ φ 2. ( ) = e iφ. = e iφ cosθ. Chemistry 362 Dr Jean M Standard Problem Set 9 Solutions The ˆ L 2 operator is defined as Verify that the angular wavefunction Y θ,φ) Also verify that the eigenvalue is given by 2! 2 & L ˆ 2! 2 2 θ 2 +

Διαβάστε περισσότερα

6. MAXIMUM LIKELIHOOD ESTIMATION

6. MAXIMUM LIKELIHOOD ESTIMATION 6 MAXIMUM LIKELIHOOD ESIMAION [1] Maximum Likelihood Estimator (1) Cases in which θ (unknown parameter) is scalar Notational Clarification: From now on, we denote the true value of θ as θ o hen, view θ

Διαβάστε περισσότερα

DERIVATION OF MILES EQUATION FOR AN APPLIED FORCE Revision C

DERIVATION OF MILES EQUATION FOR AN APPLIED FORCE Revision C DERIVATION OF MILES EQUATION FOR AN APPLIED FORCE Revision C By Tom Irvine Email: tomirvine@aol.com August 6, 8 Introduction The obective is to derive a Miles equation which gives the overall response

Διαβάστε περισσότερα

Statistics 104: Quantitative Methods for Economics Formula and Theorem Review

Statistics 104: Quantitative Methods for Economics Formula and Theorem Review Harvard College Statistics 104: Quantitative Methods for Economics Formula and Theorem Review Tommy MacWilliam, 13 tmacwilliam@college.harvard.edu March 10, 2011 Contents 1 Introduction to Data 5 1.1 Sample

Διαβάστε περισσότερα

Additional Results for the Pareto/NBD Model

Additional Results for the Pareto/NBD Model Additional Results for the Pareto/NBD Model Peter S. Fader www.petefader.com Bruce G. S. Hardie www.brucehardie.com January 24 Abstract This note derives expressions for i) the raw moments of the posterior

Διαβάστε περισσότερα

PROPERTIES OF CERTAIN INTEGRAL OPERATORS. a n z n (1.1)

PROPERTIES 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 περισσότερα

Econ Spring 2004 Instructor: Prof. Kiefer Solution to Problem set # 5. γ (0)

Econ Spring 2004 Instructor: Prof. Kiefer Solution to Problem set # 5. γ (0) Cornell University Department of Economics Econ 60 - Spring 004 Instructor: Prof. Kiefer Solution to Problem set # 5. Autocorrelation function is defined as ρ h = γ h γ 0 where γ h =Cov X t,x t h =E[X

Διαβάστε περισσότερα

New bounds for spherical two-distance sets and equiangular lines

New 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 περισσότερα

2. THEORY OF EQUATIONS. PREVIOUS EAMCET Bits.

2. THEORY OF EQUATIONS. PREVIOUS EAMCET Bits. EAMCET-. THEORY OF EQUATIONS PREVIOUS EAMCET Bits. Each of the roots of the equation x 6x + 6x 5= are increased by k so that the new transformed equation does not contain term. Then k =... - 4. - Sol.

Διαβάστε περισσότερα

A Note on Intuitionistic Fuzzy. Equivalence Relation

A 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 περισσότερα

ECE Spring Prof. David R. Jackson ECE Dept. Notes 2

ECE Spring Prof. David R. Jackson ECE Dept. Notes 2 ECE 634 Spring 6 Prof. David R. Jackson ECE Dept. Notes Fields in a Source-Free Region Example: Radiation from an aperture y PEC E t x Aperture Assume the following choice of vector potentials: A F = =

Διαβάστε περισσότερα

Math 6 SL Probability Distributions Practice Test Mark Scheme

Math 6 SL Probability Distributions Practice Test Mark Scheme Math 6 SL Probability Distributions Practice Test Mark Scheme. (a) Note: Award A for vertical line to right of mean, A for shading to right of their vertical line. AA N (b) evidence of recognizing symmetry

Διαβάστε περισσότερα

Reminders: linear functions

Reminders: linear functions Reminders: linear functions Let U and V be vector spaces over the same field F. Definition A function f : U V is linear if for every u 1, u 2 U, f (u 1 + u 2 ) = f (u 1 ) + f (u 2 ), and for every u U

Διαβάστε περισσότερα

A Two-Sided Laplace Inversion Algorithm with Computable Error Bounds and Its Applications in Financial Engineering

A 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 περισσότερα