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<title>Department of Mathematics and Physics</title>
<link href="http://ir.tum.ac.ke/handle/123456789/181" rel="alternate"/>
<subtitle>Contains PDF journal articles for this department</subtitle>
<id>http://ir.tum.ac.ke/handle/123456789/181</id>
<updated>2026-06-13T17:37:57Z</updated>
<dc:date>2026-06-13T17:37:57Z</dc:date>
<entry>
<title>COMPUTING FUZZY SUBGROUPS OF SOME SPECIAL CYCLIC GROUPS</title>
<link href="http://ir.tum.ac.ke/handle/123456789/17600" rel="alternate"/>
<author>
<name>Makamba, Babington</name>
</author>
<author>
<name>Munywoki, Michael M.</name>
</author>
<id>http://ir.tum.ac.ke/handle/123456789/17600</id>
<updated>2024-05-29T00:00:38Z</updated>
<published>2019-01-01T00:00:00Z</published>
<summary type="text">COMPUTING FUZZY SUBGROUPS OF SOME SPECIAL CYCLIC GROUPS
Makamba, Babington; Munywoki, Michael M.
In this paper, we discuss the number of distinct fuzzy subgroups of the group Zpn × Zqm × Zr, m = 1, 2, 3 where p, q, r are distinct primes for any n ∈ Z + using the criss-cut method that was proposed by Murali and Makamba in their study of distinct fuzzy subgroups. The criss-cut method first establishes all the maximal chains of the subgroups of a group G and then counts the distinct fuzzy subgroups contributed&#13;
by each chain. In this paper, all the formulae for calculating the number of these distinct fuzzy subgroups are given in polynomial form.
https://doi.org/10.4134/CKMS.c180341
</summary>
<dc:date>2019-01-01T00:00:00Z</dc:date>
</entry>
<entry>
<title>Operator Equations, Operator Inequalities and Power Bounded Operators in Hilbert Spaces</title>
<link href="http://ir.tum.ac.ke/handle/123456789/17597" rel="alternate"/>
<author>
<name>Stephen, Ms Nyamusi Dorca</name>
</author>
<author>
<name>Kavila, Dr Mutie</name>
</author>
<id>http://ir.tum.ac.ke/handle/123456789/17597</id>
<updated>2024-05-28T00:00:50Z</updated>
<published>2017-11-01T00:00:00Z</published>
<summary type="text">Operator Equations, Operator Inequalities and Power Bounded Operators in Hilbert Spaces
Stephen, Ms Nyamusi Dorca; Kavila, Dr Mutie
This is a study on some operator equations, operator inequalities and power bounded operators in Hilbert&#13;
spaces. Looking at the operator equation TW = WS various properties on T, W and S such as; quasinormal, posinormal, hyponormal among others are satisfied, also on some operator inequalities the equivalence of constability of sequences of norms and its decomposition among other results are shown.
</summary>
<dc:date>2017-11-01T00:00:00Z</dc:date>
</entry>
<entry>
<title>A little more on ideals associated with sublocales</title>
<link href="http://ir.tum.ac.ke/handle/123456789/17595" rel="alternate"/>
<author>
<name>Ighedo, O.</name>
</author>
<author>
<name>Kivunga, G.W.</name>
</author>
<author>
<name>Stephen, D.N.</name>
</author>
<id>http://ir.tum.ac.ke/handle/123456789/17595</id>
<updated>2024-05-28T00:00:38Z</updated>
<published>2024-01-01T00:00:00Z</published>
<summary type="text">A little more on ideals associated with sublocales
Ighedo, O.; Kivunga, G.W.; Stephen, D.N.
As usual, let RL denote the ring of real-valued continuous functions on a completely regular frame L. Let βL and λL denote the StoneCech compactification of ˇ L and the Lindel¨of coreflection of L, respectively.  There is a natural way of associating with each sublocale of βL two ideals of RL, motivated by a similar situation in C(X). In [12], the authors go one step further and associate with each sublocale of λL an ideal of RL in a manner similar to one of the ways one does it for sublocales of βL. The intent in this paper is to augment [12] by considering two other coreflections; namely, the realcompact and the paracompact coreflections.&#13;
We show that M-ideals of RL indexed by sublocales of βL are precisely the intersections of maximal ideals of RL. An M-ideal of RL is grounded in case it is of the form MS for some sublocale S of L. A similar definition is given for an O-ideal of RL. We characterise M-ideals of RL indexed by spatial sublocales of βL, and O-ideals of RL indexed by closed sublocales of βL in&#13;
terms of grounded maximal ideals of RL.
https://doi.org/10.48308/cgasa.20.1.175
</summary>
<dc:date>2024-01-01T00:00:00Z</dc:date>
</entry>
<entry>
<title>Modelling Turbulence Using the Staggered Grid and Simplec Method</title>
<link href="http://ir.tum.ac.ke/handle/123456789/17499" rel="alternate"/>
<author>
<name>KIMUNGUYI, J. K.</name>
</author>
<author>
<name>GATHER, F. K.</name>
</author>
<author>
<name>AWUOR, K. O.</name>
</author>
<id>http://ir.tum.ac.ke/handle/123456789/17499</id>
<updated>2024-03-01T00:00:49Z</updated>
<published>2020-05-01T00:00:00Z</published>
<summary type="text">Modelling Turbulence Using the Staggered Grid and Simplec Method
KIMUNGUYI, J. K.; GATHER, F. K.; AWUOR, K. O.
In a natural convection, local density&#13;
differences and a resulting pressure gradient accelerate&#13;
the fluid. In this paper a numerical study of a turbulent,&#13;
natural convection problem is performed with an&#13;
incompressible fluid in a rectangular enclosure. At the&#13;
heated wall, the temperature distribution is a function&#13;
of temperature gradients. The objective of this study is&#13;
to conduct a numerical investigation of turbulent&#13;
natural convection in a 3-D cavity using the staggered&#13;
grid and the SIMPLEC method. The statisticalaveraging process of the mass, momentum and energy&#13;
governing equations introduces unknown turbulent&#13;
correlations into the mean flow equations which&#13;
represent the turbulent transport of momentum, heat&#13;
and mass, namely Reynolds stress () and heat flux (),&#13;
which are modeled using k- SST model. The ReynoldsAveraged Navier-stokes (RANS), energy and k- SST&#13;
turbulent equations are first non-dimensionalized and&#13;
the resulting equations are discretized using a staggered&#13;
and solved using SIMPLEC. From the results, both the&#13;
experimental data and simulation using the staggered&#13;
grid and SIMPLEC return a non-dimensional&#13;
temperature of 0.5 at the core of the cavity and almost&#13;
zero towards the cold and the natural turbulence flow is&#13;
responsible for temperature distribution. Further,&#13;
convective mass exchange is dominant in the centre of&#13;
the enclosure. The investigated Rayleigh number of this&#13;
study lies at Ra = 1.58.
</summary>
<dc:date>2020-05-01T00:00:00Z</dc:date>
</entry>
</feed>
