1967
DOI: 10.1016/0017-9310(67)90130-5
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W. M. Kays, Convective Heat and Mass Transfer, 387 pp. McGraw-Hill, New York (1966)

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Cited by 21 publications
(40 citation statements)
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“…If the number of cells passed by an MT is assumed to be a random variable with uniform distribution on [ ], the probability mass function and its transform can be represented as (12) Then, the pdf of the residence time in an LA has Laplace transform as (13) where is computed from (2). From the property of Laplace transform [7], the first-order moment, i.e., the mean value of the residence time in the LA, is (14) As shown in Fig. 1, system and are assumed to be in macrocell and microcell tier, respectively.…”
Section: Calculation Of Intersystem Roaming Probabilitiesmentioning
confidence: 99%
“…If the number of cells passed by an MT is assumed to be a random variable with uniform distribution on [ ], the probability mass function and its transform can be represented as (12) Then, the pdf of the residence time in an LA has Laplace transform as (13) where is computed from (2). From the property of Laplace transform [7], the first-order moment, i.e., the mean value of the residence time in the LA, is (14) As shown in Fig. 1, system and are assumed to be in macrocell and microcell tier, respectively.…”
Section: Calculation Of Intersystem Roaming Probabilitiesmentioning
confidence: 99%
“…(The scheduling scheme at the sender is specific to the implementation, and beyond this paper's scope.) If the timeout value of NAK timer (18) is used in place of the timeout value of NAK timer (3), the expected time between the issuance of the first NAK and the nominal reception of the last bit of the last transmission spurt in (5) is replaced by (19) and thus, the expected file-delivery time is (20) in place of (7).…”
Section: Discussionmentioning
confidence: 99%
“…Recall that the expected time until any arrival among independent Poisson processes, each with arrival rate , is [7]. Consider independent Poisson processes, each of which terminates after the first arrival.…”
Section: Discussionmentioning
confidence: 99%
“…Details of probabilistic convolution can be found in the work of Drake [1967]. P T (n > 0jq z ) is the total within-crown gap probability of the canopy, and P h (njq z ), and P c (njq z ) are the probability for a beam of light at zenith angle q z passing n (n = 0, 1, 2, .…”
Section: Modeling Radiation Interception By Forest Canopiesmentioning
confidence: 99%