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Circular strongly partially-balanced repeated measurement designs in periods of two different sizes using method of cyclic shifts (Rule II)
⁎Corresponding author. rashid.ahmed@iub.edu.pk (Rashid Ahmed)
-
Received: ,
Accepted: ,
This article was originally published by Elsevier and was migrated to Scientific Scholar after the change of Publisher.
Peer review under responsibility of King Saud University.
Abstract
Strongly balanced repeated measurement designs may be used in medicine, pharmacology, animal sciences and psychology with unequal period sizes. To avoid a large number of subjects, strongly partially-balanced repeated measurement designs are preferred. In this article, some infinite series are developed to generate the minimal strongly partially-balanced repeated measurement designs in periods of two different sizes using method of cyclic shifts (Rule II).
Keywords
05B05
62K10
62K05
Repeated measurement designs
Balanced repeated measurement designs
Strongly balanced repeated measurement designs
Circular strongly partially-balanced repeated measurement designs

1 Introduction
A repeated measurements design (RMD) is balanced with respect to the first-order residual effects if each treatment is immediately preceded same number of times, say λ′ times by each other treatment (excluding itself). Williams (1949, 1950) first initiated RMDs. Magda (1980) introduced the idea of a circular balanced RMDs. Cheng and Wu (1980) constructed balanced and strongly balanced RMD. RMD is strongly balanced with respect to the first-order residual effects if each treatment is immediately preceded λ′ times by each other treatment (including itself). Afsarinejed (1994) constructed balanced and strongly balanced minimal RMDs with unequal period sizes. RMDs in unequal period sizes are very useful if there is a restriction on the total number of treatments, some experimental units can receive on the total length of time while some experimental units can remain in the trial. Using method of cyclic shifts, Iqbal and Jones (1994) constructed (i) efficient RMDs with equal and unequal period sizes (ii) Strongly balanced RMDs for two unequal period sizes. Iqbal and Tahir (2009) constructed CSBRMD (circular strongly balanced RMDs) for some classes. Iqbal et al. (2010) constructed some first- and second-order CBRMD and CSBRMDs. Rasheed et al. (2018) developed some infinite series to obtain the minimal CSBRMDs in periods of three different sizes. The situations where minimal CSBRMDs cannot be constructed, minimal CSPBRMDs are preferred. RMD is strongly partially balanced if each treatment is not immediately preceded same number of times by each other treatment (including itself). If λ′i takes only two values as λ′1 = λ′2 + 1 then it is very close to the balanced. Strongly balanced and strongly partially-balanced RMDs are useful for the estimation of direct and residual effects independently. Minimal CSPBRMDs are preferred for the cases where minimal SBRMDs cannot be constructed. Jabeen et al. (2019) constructed minimal CSPBRMDs in equal period sizes almost for every cases. Using method of cyclic shifts (Rule I), Nazeer et al. (2018) constructed these designs in periods of two different sizes only for a few cases of v. For the remaining cases of v, minimal CSPBRMDs in periods of two different sizes could be constructed through method of cyclic shifts (Rule II) which should be constructed. Therefore, in this article, these designs are constructed for the remaining cases through method of cyclic shifts (Rule II).
The rest of the paper is organized as follows: In Section 2, method of cyclic shifts (Rule II) is explained to generate the CSPBRMDs in periods of two different sizes. In Section 3, efficiency of proposed designs is discussed. Using method of cyclic shifts (Rule II), some infinite series are developed in Section 4 to obtain minimal CSPBRMDs. These series are very useful for researchers and experimenters. They can get the required designs just by putting the values needed for the series. Contribution of this research is discussed in Section 5.
2 Method of cyclic shifts
In this article, Method of Cyclic Shifts introduced by Iqbal (1991) is used as a methodology for construction of the proposed designs. This method is preferred because it provides an easy construction of several types of cyclic designs such as (i) balanced incomplete block designs, (ii) polygonal designs, (iii) neighbor balanced designs, (iv) strongly balanced neighbor designs, (v) balanced RMDs, (vi) strongly balanced RMDs, (vii) weakly balanced RMDs, and (viii) strongly partially-balanced RMDs. All these designs can be constructed through this method in linear and circular periods/blocks of equal and unequal sizes. Furthermore, this method has edge over the existing methods because without studying the complete design, one can check the standard property of treatment balance and other balance properties such as for neighbor effects and residual effects, etc. Method of cyclic shifts (Rule II) is explained here briefly only for the construction of CSPBRMDs. For detail, see Iqbal & Tahir (2009) and Iqbal et al. (2010).
Rule II: Let S1 = [ , , …, ] and S2 = [ , , …, ]t be sets of shifts, where ≤ v − 2. If each element 0, 1, 2, …, v − 2 appears an equal number of times, say λ′ in a new set of shifts S*, where S* = [ , , …, , , , …, , v − 1-( + + …+ ) mod v − 1] then it will be CSBRMD in periods of sizes p1 & p2, otherwise CSPBRMD.
CSPBRMDs is constructed for v = 10, p1 = 6 and p2 = 4 through the following two sets of shifts.
S1 = [1,3,2,8,7], S2 = [4,0]t
B1
B2
B3
B4
B5
B6
B7
B8
B9
B10
B11
B12
B13
B14
B15
B16
B17
B18
03
14
25
36
47
58
60
71
82
09
19
29
39
49
59
69
79
89
10
21
32
43
54
65
76
87
08
40
51
62
73
84
05
16
27
38
41
52
63
74
85
06
17
28
30
44
55
66
77
88
00
11
22
33
64
75
86
07
18
20
31
42
53
94
95
96
97
98
90
91
92
93
56
67
78
80
01
12
23
34
45
35
46
57
68
70
81
02
13
24
3 Statistical model and efficiency of the design
In order to consider the efficiency of the constructed designs, the model for circular RMDs proposed by Davis and Hall (1969) is used.
Using the identities, D′D = R′D = bpIv, D′R = L, D′U = N, D′P = bEv,p, R′U = N, U′U = pIn, U′U = Ek,q, P′P = nIn. The reduced normal equations for and will be:
θ = Θ = , = , , ,
For the period of two different sizes information matrix can be presented as:
The information matrix for direct and residual effects denoted by and Θ respectively can be specified by their initial rows:
According to the duality presented in the model (1), both direct and residual effects share the same information matrix. The non-zero Eigen values of information matrix C* are called the canonical efficiency factors, see James and Wilkinson (1971) and Pearce et al. (1974). The canonical efficiency factor is calculated by working out harmonic mean of non-zero Eigen values of their respective information matrix relative to that of an orthogonal with the same number of treatments having same number of replications. It is further assume that σ2 is the same for the proposed design and the orthogonal design to which it is compared. The high value of Er shows that design is suitable for the estimation of residual effects. Our proposed designs have high value of Er, therefore, these designs are suitable for the estimation of residual effects while using periods of two different sizes.
4 Infinite Series to generate CSPBRMDs in periods of two different sizes
In this section, some infinite series are developed by method of cyclic shifts (Rule II) to generate minimal CSPBRMDs in periods of two different sizes. In the all following series, S* contains all values from 0, 1, 2, …, v − 1 either 0 or 1 time, therefore, all series provide minimal CSPBRMDs. Here ordered pairs {(0, v/2), (1, (v + 2)/2), …, ((v − 4)/2, v − 2), ((v − 2)/2, 0), (v/2, 1), …, (v − 2, (v − 2)/2), (v − 1, v − 1)} do not appear together while all other appear once in Series 3.1–3.9 while ordered pairs {(0, (v + 1)/2), (1, (v + 3)/2), …, ((v − 3)/2, v − 2), ((v − 1)/2, 0), ((v + 1)/2, 1), …, (v − 2, (v − 3)/2), (v − 1, v − 1)} do not appear together while all other appear once in Series 3.10 to 3.20. In these series sum of any two, three, …, (p − 2) consecutive elements should not be 0 (mod v). If so, reorder the elements.
Series 4.1: CSPBRMDs can be constructed for v = 2mi + 4, m > 2, i integer, p1 = 2 m and p2 = 4 through the following (i + 1) sets of shifts.
Sj+1 = [mj + 1, mj + 2, …, mj + m, v − 2-mj, v − 3-mj, …, v − m-mj]; j = 0, 1, …, i − 1.
Si+1 = [0, (v − 2)/2]t
v
m
i
p1
p2
Sets of Shifts
Er
10
3
1
6
4
[1,2,3,8,7] + [0,4]t
0.83
16
3
2
6
4
[1,2,3,14,13] + [4,5,6,11,10] + [0,7]t
0.83
12
4
1
8
4
[1,2,3,4,10,9,8] + [0,5]t
0.86
20
4
2
8
4
[1,2,3,4,18,17,16] + [5,6,7,8,14,13,12] + [0,9]t
0.86
Sj+1 = [mj + 1, mj + 2, …, mj + m, v − 2-mj, v − 3-mj, …, v − m-mj]; j = 0, 1, …, i − 1.
Si+1 = [0, (v − 4)/2, (v − 2)/2, (v + 2)/2]t
v
m
i
p1
p2
Sets of Shifts
Er
14
4
1
8
6
[1,2,3,4,12,11,10] + [0,5,6,8]t
0.89
22
4
2
8
6
[1,2,3,4,20,19,18] + [5,6,7,8,16,15,14] + [0,9,10,12]t
0.88
16
5
1
10
6
[1,2,3,4,5,14,13,12,11] + [0,6,7,9]t
0.91
26
5
2
10
6
[1,2,3,4,5,24,23,22,21] + [6,7,8,9,10,19,18,17,16] + [0,11,12,14]t
0.90
Sj+1 = [mj + 1, mj + 2, …, mj + m, v − 2-mj, v − 3-mj, …, v − m-mj]; j = 0, 1, …, i − 1.
Si+1 = [0, (v − 6)/2, (v − 4)/2, (v − 2)/2, (v + 2)/2, (v + 4)/2]t
v
m
i
p1
p2
Sets of Shifts
Er
18
5
1
10
8
[1,2,3,4,5,16,15,14,13] + [0,6,7,8,10,11]t
0.92
28
5
2
10
8
[1,2,3,4,5,26,25,24,23] + [6,7,8,9,10,21,20,19,18] + [0,11,12,13,15,16]t
0.91
20
6
1
12
8
[1,2,3,4,5,6,18,17,16,15,14] + [0,7,8,9,11,12]t
0.93
32
6
2
12
8
[1,2,3,4,5,6,30,29,28,27,26] + [7,8,9,10,11,12,24,23,22,21,20] + [0,13,14,15,17,18]t
0.93
Sj+1 = [mj + 1, mj + 2, …, mj + m, v − 2-mj, v − 3-mj, …, v − m-mj]; j = 0, 1, …, i − 1.
Si+1 = [0, (v − 6)/2, (v − 4)/2, (v − 2)/2, (v + 2)/2, (v + 4)/2]t
Si+1 = [0, (v − 8)/2, (v − 6)/2, (v − 4)/2, (v − 2)/2, (v + 2)/2, (v + 4)/2, (v + 6)/2]t
v
m
i
p1
p2
Sets of Shifts
Er
22
6
1
12
10
[1,2,3,4,5,6,20,19,18,17,16] + [0,7,8,9,10,12,13,14]t
0.94
34
6
2
12
10
[1,2,3,4,5,6,32,31,30,29,28] + [7,8,9,10,11,12,26,25,24,23,22] + [0,13,14,15,16,18,19,20]t
0.93
24
7
1
14
10
[1,2,3,4,5,6,7,22,21,20,19,18,17] + [0,8,9,10,11,13,14,15]t
0.95
38
7
2
14
10
[1,2,3,4,5,6,7,36,35,34,33,32,31] + [8,9,10,11,12,13,14,29,28,27,26,25,24] + [0,15,16,17,18,20,21,22]t
0.94
Sj+1 = [mj + 1, mj + 2, …, mj + m, v − 2-mj, v − 3-mj, …, v − m-mj]; j = 0, 1, …, i − 1.
Si+1 = [0, (v − 10)/2, (v − 8)/2, (v − 6)/2, (v − 4)/2, (v − 2)/2, (v + 2)/2, (v + 4)/2, (v + 6)/2, (v + 8)/2]t
v
m
i
p1
p2
Sets of Shifts
Er
26
7
1
14
12
[1,2,3,4,5,6,7,24,23,22,21,20,19] + [0,8,9,10,11,12,14,15,16,17]t
0.81
40
7
2
14
12
[1,2,3,4,5,6,7,38,37,36,35,34,33] + [8,9,10,11,12,13,14,31,30,29,28,27,26] + [0,15,16,17,18,19,21,22,23,24]t
0.94
28
8
1
16
12
[1,2,3,4,5,6,7,8,26,25,24,23,22,21,20] + [0,9,10,11,12,13,15,16,17,18]t
0.96
44
8
2
16
12
[1,2,3,4,5,6,7,8,42,41,40,39,38,37,36] + [9,10,11,12,13,14,15,16,34,33,32,31,30,29,28] + [0,17,18,19,20,21,23,24,25,26]t
0.95
S1 = [1, 2, …, m, v − 2, v − 3, …, v − 1-m];
S2 = [(v − 2)/2]t
v
m
p1
p2
Sets of Shifts
Er
8
2
5
3
[1,2,6,5] + [3]t
0.80
10
3
7
3
[1,2,3,8,7,6] + [4]t
0.85
12
4
9
3
[1,2,3,4,10,9,8,7] + [5]t
0.89
S1 = [1, 2, …, m, v − 2, v − 3, …, v − 1-m];
S2 = [(v − 4)/2, (v − 2)/2, (v + 2)/2]t
v
m
p1
p2
Sets of Shifts
Er
12
3
7
5
[1,2,3,10,9,8] + [4,5,7]t
0.88
14
4
9
5
[1,2,3,4,12,11,10,9] + [5,6,8]t
0.90
16
5
11
5
[1,2,3,4,5,14,13,12,11,10] + [6,7,9]t
0.89
S1 = [1, 2, …, m, v − 2, v − 3, …, v − 1-m];
S2 = [(v − 6)/2, (v − 4)/2, (v − 2)/2, (v + 2)/2, (v + 4)/2]t
v
m
p1
p2
Sets of Shifts
Er
16
4
9
7
[1,2,3,4,14,13,12,11] + [5,6,7,9,10]t
0.92
18
5
11
7
[1,2,3,4,5,16,15,14,13,12] + [6,7,8,10,11]t
0.93
20
6
13
7
[1,2,3,4,5,6,18,17,16,15,14,13] + [7,8,9,11,12]t
0.94
S1 = [1, 2, …, m, v − 2, v − 3, …, v − 1-m];
S2 = [(v − 8)/2, (v − 6)/2, (v − 4)/2, (v − 2)/2, (v + 2)/2, (v + 4)/2, (v + 6)/2]t
v
m
p1
p2
Sets of Shifts
Er
20
5
11
9
[1,2,3,4,5,18,17,16,15,14] + [6,7,8,9,11,12,13]t
0.94
22
6
13
9
[1,2,3,4,5,6,20,19,18,17,16,15] + [7,8,9,10,12,13,14]t
0.93
24
7
15
9
[1,2,3,4,5,6,7,22,21,20,19,18,17,16] + [8,9,10,11,13,14,15]t
0.95
Sj+1 = [mj + 1, mj + 2, …, mj + m, v − 2-mj, v − 3-mj, …, v − m-mj]; j = 0, 1, …, i − 1.
Si+1 = [0, (v − 3)/2, (v − 1)/2]t
v
m
i
p1
p2
Sets of Shifts
Er
11
3
1
6
5
[1,2,3,9,8] + [0,4,5]t
0.85
17
3
2
6
5
[1,2,3,15,14] + [4,5,6,12,11] + [0,7,8]t
0.85
13
4
1
8
5
[1,2,3,4,11,10,9] + [0,5,6]t
0.88
21
4
2
8
5
[1,2,3,4,19,18,17] + [5,6,7,8,15,14,13] + [0,9,10]t
0.88
Sj+1 = [mj + 1, mj + 2, …, mj + m, v − 2-mj, v − 3-mj, …, v − m-mj]; j = 0, 1, …, i − 1.
Si+1 = [0, (v − 5)/2, (v − 3)/2, (v − 1)/2, (v + 3)/2]t
v
m
i
p1
p2
Sets of Shifts
Er
15
4
1
8
7
[1,2,3,4,13,12,11] + [0,5,6,7,9]t
0.91
23
4
2
8
7
[1,2,3,4,21,20,19] + [5,6,7,8,17,16,15] + [0,9,10,11,13]t
0.89
17
5
1
10
7
[1,2,3,4,5,15,14,13,12] + [0,6,7,8,10]t
0.92
27
5
2
10
7
[1,2,3,4,5,25,24,23,22] + [6,7,8,9,10,20,19,18,17] + [0,11,12,13,15]t
0.91
Sj+1 = [mj + 1, mj + 2, …, mj + m, v − 2-mj, v − 3-mj, …, v − m-mj]; j = 0, 1, …, i − 1.
Si+1 = [0, (v − 7)/2, (v − 5)/2, (v − 3)/2, (v − 1)/2, (v + 3)/2, (v + 5)/2]t
v
m
i
p1
p2
Sets of Shifts
Er
19
5
1
10
9
[1,2,3,4,5,17,16,15,14] + [0,6,7,8,9,11,12]t
0.93
29
5
2
10
9
[1,2,3,4,5,27,26,25,24] + [6,7,8,9,10,22,21,20,19] + [0,11,12,13,14,16,17]t
0.92
21
6
1
12
9
[1,2,3,4,5,6,19,18,17,16,15] + [0,7,8,9,10,12,13]t
0.94
33
6
2
12
9
[1,2,3,4,5,6,31,30,29,28,27] + [7,8,9,10,11,12,25,24,23,22,21] + [0,13,14,15,16,18,19]t
0.93
Sj+1 = [mj + 1, mj + 2, …, mj + m, v − 2-mj, v − 3-mj, …, v − m-mj]; j = 0, 1, …, i − 1.
Si+1 = [0, (v − 9)/2, (v − 7)/2, (v − 5)/2, (v − 3)/2, (v − 1)/2, (v + 3)/2, (v + 5)/2, (v + 7)/2]t
v
m
i
p1
p2
Sets of Shifts
Er
23
6
1
12
11
[1,2,3,4,5,6,16,17,18,19,20] + [0,7,8,9,10,11,13,14,15]t
0.94
35
6
2
12
11
[1,2,3,4,5,6,33,32,31,30,29] + [7,8,9,10,11,12,27,26,25,24,23] + [0,13,14,15,16,17,19,20,21]t
0.93
25
7
1
14
11
[1,2,3,4,5,6,7,23,22,21,20,19,18] + [0,8,9,10,11,12,14,15,16]t
0.95
39
7
2
14
11
[1,2,3,4,5,6,7,37,36,35,34,33,32] + [8,9,10,11,12,13,14,30,29,28,27,26,25] + [0,15,16,17,18,19,21,22,23]t
0.94
Sj+1 = [mj + 1, mj + 2, …, mj + m, v − 2-mj, v − 3-mj, …, v − m-mj]; j = 0, 1, …, i − 1.
Si+1 = [0, (v − 11)/2, (v − 9)/2, …, (v − 1)/2, (v + 3)/2, (v + 5)/2, (v + 7)/2, (v + 9)/2]t
v
m
i
p1
p2
Sets of Shifts
Er
27
7
1
14
13
[1,2,3,4,5,6,7,25,24,23,22,21,20] + [0,8,9,10,11,12,13,15,16,17,18]t
0.82
41
7
2
14
13
[1,2,3,4,5,6,7,39,38,37,36,35,34] + [8,9,10,11,12,13,14,32,31,30,29,28,27] + [0,15,16,17,18,19,20,22,23,24,25]t
0.85
29
8
1
16
13
[1,2,3,4,5,6,7,8,27,26,25,24,23,22,21] + [0,9,10,11,12,13,14,16,17,18,19]t
0.83
45
8
2
16
13
[1,2,3,4,5,6,7,8,43,42,41,40,39,38,37] + [9,10,11,12,13,14,15,16,35,34,33,32,31,30,29] + [0,17,18,19,20,21,22,24,25,26,27]t
0.87
S1 = [1, 2, …, m, v − 2, v − 3, …, v − 1-m];
Sj+2 = [2j + m + 1, 2j + m + 2, v − 2-m-2j]; j = 0, 1, …, i − 2.
Si+1 = [(v − 3)/2, (v − 1)/2]t
v
m
i
p1
p2
Sets of Shifts
Er
9
2
1
5
4
[1,2,7,6] + [3,4]t
0.82
13
2
2
5
4
[1,2,11,10] + [3,4,9] + [5,6]t
0.80
11
3
1
7
4
[1,2,3,9,8,7] + [4,5]t
0.86
15
3
2
7
4
[1,2,3,13,12,11] + [4,5,10] + [6,7]t
0.86
S1 = [1, 2, …, m, v − 2, v − 3, …, v − 1-m];
Sj+2 = [3j + m + 1, 3j + m + 2, 3j + m + 3, v − 2-m-3j, v − 3-m-3j]; j = 0, 1, …, i − 2.
Si+1 = [(v − 5)/2, (v − 3)/2, (v − 1)/2, (v + 3)/2]t
v
m
i
p1
p2
Sets of Shifts
Er
13
3
1
7
6
[1,2,3,11,10,9] + [4,5,6,8]t
0.89
19
3
2
7
6
[1,2,3,17,16,15] + [4,5,6,14,13] + [7,8,9,11]t
0.88
15
4
1
9
6
[1,2,3,4,13,12,11,10] + [5,6,7,9]t
0.91
21
4
2
9
6
[1,2,3,4,19,18,17,16] + [5,6,7,15,14] + [8,9,10,12]t
0.90
S1 = [1, 2, …, m, v − 2, v − 3, …, v − 1-m];
Sj+2 = [4j + m + 1, 4j + m + 2, 4j + m + 3, 4j + m + 4, v − 2-m-4j, v − 3 m-4j, v − 4-m-4j]; j = 0,1, …, i − 2.
Si+1 = [(v − 7)/2, (v − 5)/2, (v − 3)/2, (v − 1)/2, (v + 5)/2, (v + 3)/2]t
v
m
i
p1
p2
Sets of Shifts
Er
17
4
1
9
8
[1,2,3,4,15,14,13,12] + [5,6,7,8,11,10]t
0.92
25
4
2
9
8
[1,2,3,4,23,22,21,20] + [5,6,7,8,19,18,17] + [9,10,11,12,15,14]t
0.91
19
5
1
11
8
[1,2,3,4,5,17,16,15,14,13] + [6,7,8,9,12,11]t
0.93
27
5
2
11
8
[1,2,3,4,5,25,24,23,22,21] + [6,7,8,9,20,19,18] + [10,11,12,13,16,15]t
0.92
S1 = [1, 2, …, m, v − 2, v − 3, …, v − 1-m];
Sj+2 = [5j + m + 1, 5j + m + 2, …, 5j + m + 5, v − 2-m-5j, v − 3-m-5j, …, v − 5-m-5j]; j = 0, 1, …, i − 2.
Si+1 = [(v − 9)/2, (v − 7)/2, (v − 5)/2, (v − 3)/2, (v − 1)/2, (v + 7)/2, (v + 3)/2, (v + 5)/2]t
v
m
i
p1
p2
Sets of Shifts
Er
21
5
1
11
10
[1,2,3,4,5,19,18,17,16,15] + [6,7,8,9,10,14,13,12]t
0.84
31
5
2
11
10
[1,2,3,4,5,29,28,27,26,25] + [6,7,8,9,10,24,23,22,21] + [11,12,13,14,15,17,18,19]t
0.81
23
6
1
13
10
[1,2,3,4,5,6,21,20,19,18,17,16] + [7,8,9,10,11,13,14,15]t
0.86
33
6
2
13
10
[1,2,3,4,5,6,31,30,29,28,27,26] + [7,8,9,10,11,25,24,23,22] + [12,13,14,15,16,18,19,20]
0.82
S1 = [1, 2, …, m, v − 2, v − 3, …, v − 1-m];
Sj+2 = [6j + m + 1, 6j + m + 2, …, 6j + m + 6, v − 2-m-6j, v − 3-m-6j, …, v − 6-m-6j]; j = 0, 1, …, i − 2.
Si+1 = [(v − 11)/2, (v − 9)/2, …, (v − 1)/2, (v + 9)/2, (v + 7)/2 , (v + 5)/2, (v + 3)/2]t
v
m
i
p1
p2
Sets of Shifts
Er
25
6
1
13
12
[1,2,3,4,5,6,23,22,21,20,19,18] + [7,8,9,10,11,12,17,16,15,14]t
0.80
37
6
2
13
12
[1,2,3,4,5,6,35,34,33,32,31,30] + [7,8,9,10,11,12,29,28,27,26,25] + [13,14,15,16,17,18,23,22,21,20]t
0.84
27
7
1
15
12
[1,2,3,4,5,6,7,25,24,23,22,21,20,19] + [8,9,10,11,12,13,18,17,16,15]t
0.88
39
7
2
15
12
[1,2,3,4,5,6,7,37,36,35,34,33,32,31] + [8,9,10,11,12,13,30,29,28,27,26] + [14,15,16,17,18,19,24,23,22,21]t
0.90
S1 = [1, 2, …, m, v − 2, v − 3, …, v − 1-m];
Sj+2 = [7j + m + 1, 7j + m + 2, …, 7j + m + 7, v − 2-m-7j, v − 3-m-7j, …, v − 7-m-7j]; j = 0, 1, …, i − 2.
Si+1 = [ (v − 13)/2, (v − 11)/2, …, (v + 11)/2, (v + 9)/2 , (v + 7)/2, (v + 5)/2,(v + 3)/2]t
v
m
i
p1
p2
Sets of Shifts
Er
29
7
1
15
14
[1,2,3,4,5,6,7,27,26,25,24,23,22,21] + [8,9,10,11,12,13,14,20,19,18,17,16]t
0.96
43
7
2
15
14
[1,2,3,4,5,6,7,41,40,39,38,37,36,35] + [8,9,10,11,12,13,14,34,33,32,31,30,29] + [15,16,17,18,19,20,21,27,26,25,24,23]t
0.90
31
8
1
17
14
[1,2,3,4,5,6,7,8,29,28,27,26,25,24,23,22] + [9,10,11,12,13,14,15,21,20,19,18,17]t
0.96
45
8
2
17
14
[1,2,3,4,5,6,7,8,43,42,41,40,39,38,37,36] + [9,10,11,12,13,14,15,35,34,33,32,31,30] + [16,17,18,19,20,21,22,28,27,26,25,24]t
0.95
5 Contribution of this research
Strongly balanced and strongly partially-balanced RMDs are useful for the estimation of direct and residual effects independently. The situations where minimal CSBRMDs cannot be constructed, minimal CSPBRMDs are preferred. In this article, some series are developed which are new one and provide the minimal CSPBRMDs in periods of two different sizes with high efficiency to balance out the residual effects. These designs can be used in the experiments to investigate (i) whether the perceived velocity of a moving point on a computer screen is affected by relative cues such as the presence of either vertical or horizontal lines and the amount of spacing between them, (ii) chronic conditions in clinical trials, (iii) the effect of chlorhexidine gluconate in dental plaque re-growth, (iv) different methods of preoxygenation, and (iv) cellulose membranes. These designs are also useful in asthma trial to compare doses of Budesonide and Fluticasone. Other areas where proposed designs may be applied are agricultural animal feeding trials, bioassay, bioequivalence studies, biomedical or physiological measurements, consumer trials, questionnaires, taste testing experiments, etc.
Acknowledgements
Authors are thankful to the editor and reviewers for their valuable suggestions. Authors Rashid Ahmed and H. M. Kashif Rasheed are highly grateful also to the Higher Education Commission Pakistan Research and Development Division National Research Program for Universities for providing grant for this research. Grant No: 6294/ Punjab/NRPU/R&D/HEC/2016.
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