2009
DOI: 10.1145/1639562.1639593
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State-dependent response times via fluid limits in shortest remaining processing time queues

Abstract: We consider a single server queue with renewal arrivals and i.i.d. service times, in which the server employs the Shortest Remaining Processing Time (SRPT) policy. We provide a fluid model (or formal law of large numbers approximation) for this system. The foremost payoff of our fluid model is a fluid level approximation for the state-dependent response time of a job of arbitrary size, that is, the amount of time it spends in the system, given an arbitrary system configuration at the time of its arrival.

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Cited by 8 publications
(12 citation statements)
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References 6 publications
(9 reference statements)
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“…One challenge associated with a detailed analysis of SRPT is that, due to the need to keep track of the remaining processing times of all jobs in the system, the state descriptor for an SRPT queue is infinite dimensional, even for exponentially distributed processing times. In order to describe the state of the system, Down, Gromoll, and Puha [8,9] introduce a measure valued process in which the state of the system at a given time is the finite nonnegative Borel measure on the nonnegative real line that puts a unit atom at the remaining processing time of each job in system. Under natural modeling assumptions and asymptotic conditions, they prove a fluid limit theorem (a functional law of large numbers) for this measure valued state descriptor.…”
Section: Introductionmentioning
confidence: 99%
“…One challenge associated with a detailed analysis of SRPT is that, due to the need to keep track of the remaining processing times of all jobs in the system, the state descriptor for an SRPT queue is infinite dimensional, even for exponentially distributed processing times. In order to describe the state of the system, Down, Gromoll, and Puha [8,9] introduce a measure valued process in which the state of the system at a given time is the finite nonnegative Borel measure on the nonnegative real line that puts a unit atom at the remaining processing time of each job in system. Under natural modeling assumptions and asymptotic conditions, they prove a fluid limit theorem (a functional law of large numbers) for this measure valued state descriptor.…”
Section: Introductionmentioning
confidence: 99%
“…The fluid-scaled counterparts of h r x and s r x arē i.e., the left-continuous and the right-continuous inverses ofF r , respectively. The following theorem formalizes and extends the interpretation of s · as the fluid analog of the state-dependent response time (see Down et al [8]). …”
Section: Fluid Limit Theoremsmentioning
confidence: 84%
“…Thus, for the sake of the proof of the fluid limit theorem justifying our fluid model as the first-order approximation of the queueing system under consideration (Theorem 4.6), it becomes necessary to provide exact asymptotics for the state-dependent response times in the pre-limit stochastic models. To this end, in Theorem 4.7 we establish fluid limits for these response times, which may be of independent interest, even in the G/G/1 case, as a theoretical justification of the fluid approximations for these quantities introduced by Down et al [8,9].…”
mentioning
confidence: 94%
“…A job's state-dependent response time is the time until it exits the system, conditional on the state of the system (the configuration of all current residual service times) when it arrives. The fluid limit Z * (•) can be used to calculate a fluid approximation s(x) to the state-dependent response time of a job of size x, as a function of an initial state ξ; see [5,4]. Thus Theorem 1 implies that, asymptotically on fluid scale, a job of size x arriving to a queue in state ξ will have the same state-dependent response time under SJF or SRPT.…”
Section: Implications For Comparing Performancementioning
confidence: 99%
“…Here, V * (t) = αtν for all t ≥ 0, and Z * (•) is almost surely an SRPT fluid model solution for data (α, ν) and initial condition Z * (0), equal in distribution to Z 0 ; see Theorem 5.16 in [4] as well as Section 2.2 in [4] for a definition of the fluid model solutions. Such fluid model solutions are analyzed in detail in [4,5]. Within the proof of (33), it is assumed by invoking the Skorohod representation theorem that all random elements are defined on a common probability space (Ω * , F * , P * ) such that, almost surely as r → ∞,…”
Section: Invariance Of Fluid Limitmentioning
confidence: 99%