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doi:10.1155/2009/829735

Research Article

Positive Solutions for Boundary Value Problems

of Second-Order Functional Dynamic Equations on

Time Scales

Ilkay Yaslan Karaca

Department of Mathematics, Ege University, Bornova, 35100 Izmir, Turkey

Correspondence should be addressed to Ilkay Yaslan Karaca,ilkay.karaca@ege.edu.tr

Received 3 February 2009; Accepted 26 February 2009

Recommended by Alberto Cabada

Criteria are established for existence of least one or three positive solutions for boundary value problems of second-order functional dynamic equations on time scales. By this purpose, we use a fixed-point index theorem in cones and Leggett-Williams fixed-point theorem.

Copyrightq2009 Ilkay Yaslan Karaca. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

1. Introduction

In a recent paper 1, by applying a fixed-point index theorem in cones, Jiang and Weng studied the existence of positive solutions for the boundary value problems described by second-order functional differential equations of the form

yx rxfyωx0, 0< x <1, αyxβyx ξx, ax≤0, γyx δyx ηx, 1≤xb.

1.1

Aykut 2 applied a cone fixed-point index theorem in cones and obtained sufficient conditions for the existence of positive solutions of the boundary value problems of functional difference equations of the form

−Δ2yn1 fn, yωn, na, b, αyn−1−βΔyn−1 ξn, nτ1, a

, γyn δΔyn ηn, nb, τ2

.

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In this article, we are interested in proving the existence and multiplicity of positive solutions for the boundary value problems of a second-order functional dynamic equation of the form

yΔ∇t qtyt ft, yωt, ta, b, αyρtβyΔρtξt, tτ1, a

, γyt δyΔt ηt, tb, τ2

.

1.3

Throughout this paper we letTbe any time scalenonempty closed subset ofRanda, b

be a subset ofTsuch thata, b {t∈T, atb},and fortτ1, a, tis not right scattered

and left dense at the same time.

Some preliminary definitions and theorems on time scales can be found in books3,4 which are excellent references for calculus of time scales.

We will assume that the following conditions are satisfied.

H1qt∈ Ca, b, qt≥0.

H2f :a, b×R → Ris continuous with respect toyandft, y≥0 fory∈R, where

Rdenotes the set of nonnegative real numbers.

H3ωtdefined ona, bsatisfies

cinfωt:atb< b,

dsupωt:atb> a. 1.4

LetE1:{tE:aωtρb}be nonempty subset of

E:ta, b:aωtb. 1.5

H4α, β, γ, δ≥0, αβ >0, γδ >0;

ifqt≡0 atb,thenαγ >0;−γ/δ∈ R forδ >0, whereRdenotes the set of all positively regressive and rd-continuous functions.

H5ξt and ηt are defined on τ1, σa and b, στ2, respectively, where τ1 :

min{a, c}, τ2:max{b, d}; furthermore,ξa ηb 0;

ξσt≥0, fortτ1, a

asβ0;

a

t

ξse α/βs,0∇s≥0, fortτ1, a

asβ >0;

ηt≥0, for tb, τ2

asδ0;

eγ/δt,0

t

b

ηseγ/δσs,s≥0, fortb, τ2

asδ >0.

(3)

There have been a number of works concerning of at least one and multiple positive solutions for boundary value problems recent years. Some authors have studied the problem for ordinary differential equations, while others have studied the problem for difference equations, while still others have considered the problem for dynamic equations on a time scale 5–10. However there are fewer research for the existence of positive solutions of the boundary value problems of functional differential, difference, and dynamic equations

1,2,11–13.

Our problem is a dynamic analog of the BVPs1.1and1.2. But it is more general than them. Moreover, conditions for the existence of at least one positive solution were studied for the BVPs 1.1 and 1.2. In this paper, we investigate the conditions for the existence of at least one or three positive solutions for the BVP1.3. The key tools in our approach are the following fixed-point index theorem14, and Leggett-Williams fixed-point theorem15.

Theorem 1.1see14. LetEbe Banach space andKEbe a cone inE. Letr > 0, and define

Ωr {xK:x< r}. AssumeArKis a completely continuous operator such thatAx /x forxΩr.

iIfAuuforuΩr, theniA,Ωr, K 1.

iiIfAuuforuΩr, theniA,Ωr, K 0.

Theorem 1.2see15. LetPbe a cone in the real Banach spaceE. Set

Pr :

x∈ P:x< r,

Pψ, p, q:x∈ P:pψx, xq.

1.7

Suppose thatA:Pr → Pr is a completely continuous operator andψ is a nonnegative continuous concave functional onPwithψxxfor allx∈ Pr. If there exists0 < p < q < srsuch that the following conditions hold:

i{x∈ Pψ, q, s:ψx> q}/{}andψAx> qfor allx∈ Pψ, q, s;

iiAx< pforxp;

iiiψAx> qforx∈ Pψ, q, rwithAx> s.

ThenAhas at least three fixed pointsx1, x2,andx3inPrsatisfying

(4)

2. Preliminaries

First, we give the following definitions of solution and positive solution of BVP1.3.

Definition 2.1. We say a functionytis a solution of BVP1.3if it satisfies the following.

1ytis nonnegative onρτ1, στ2.

2yt 1;tastρτ1, a, where1;t:ρτ1, a → 0,∞is defined as

1;t

⎧ ⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎩

eα/βt,0

1

β a

t

ξse α/βs,0∇se α/βa,0ya

, if β >0,

1

αξ

σt, if β0.

2.1

3yt 2;tastb, στ2, where2;t:b, στ2 → 0,∞is defined as

2;t

⎧ ⎪ ⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎪ ⎩

eγ/δt,0

1

δ t

b

ηseγ/δσs,seγ/δb,0yb

, ifδ >0,

1

γηt, ifδ0.

2.2

4yisΔ-differentiable,yΔ : ρa, b → Ris∇-differentiable ona, band yΔ∇ :

a, b → Ris continuous.

5−yΔ∇t qtyt ft, yωt,forta, b.

Furthermore, a solutionytof1.3is called a positive solution ifyt>0 forta, b.

Denote byϕtandψtthe solutions of the corresponding homogeneous equation

yΔ∇t qtyt 0, ta, b, 2.3

under the initial conditions

ϕρaβ, ϕΔρaα,

ψb δ, ψΔbγ. 2.4

Set

DWtψ, ϕ ψtϕΔtψΔtϕt. 2.5

Since the Wronskian of any two solutions of 2.3 is independent of t, evaluating at t ρa, tband using the initial conditions2.4yield

(5)

Using the initial conditions2.4, we can deduce from2.3forϕtandψt, the following equations:

ϕt βαtρa t

ρa

τ

ρaqsϕssΔτ, 2.7

ψt δγbt b

t

b

τ

qsψssΔτ. 2.8

See8.

Lemma 2.2see8. Under the conditions (H1) and the first part of (H4) the solutionsϕtand ψtpossess the following properties:

ϕt≥0, tρa, σb, ψt≥0, tρa, b, ϕt>0, tρa, σb, ψt>0, tρa, b, ϕΔt≥0, tρa, b, ψΔt≤0, tρa, b.

2.9

LetGt, sbe the Green function for the boundary value problem:

yΔ∇t qtyt 0, ta, b, αyρaβyΔρa0,

γyb δyΔb 0,

2.10

given by

Gt, s 1 D

ψtϕs, ifρastσb,

ψsϕt, ifρatsσb, 2.11

whereϕtandψtare given in2.7and2.8, respectively. It is obvious from2.6,H1 andH4, thatD >0 holds.

Lemma 2.3. Assume the conditions (H1) and (H4) are satisfied. Then

i0≤Gt, sGs, sfort, sρa, b,

iiGt, s≥ΓGs, sforta, ρbandsρa, b,

where

Γ minI1, I2

(6)
(7)
(8)

where definitionKandLemma 2.3that

(9)

Lemma 2.5. A:KKis completely continuous.

Lemma 2.6. If

lim v→0

ft, v

v, vlim→∞

ft, v

v, 2.27

for allta, b, then there exist0 < r0 < R0 <such thatiA, Kr, K 0, for0 < rr0and iA, KR, K 0, forRR0.

Proof. ChooseM >0 such that

Γ2M

E1

Gs, ss >1. 2.28

By using the first equality of2.27, we can chooser0>0 such that

ft, vMv, 0≤vr0. 2.29

Ifu∂Kr0< rr0, then fort0∈a, ρb, we have

Aut0 b

ρaG

t0, s

fs, uωsu0

ωss

≥Γ

b

ρaGs, sf

s, uωsu0

ωss

≥Γ

E1

Gs, sfs, uωss

≥ΓM

E1

Gs, suωss

≥Γ2uM

E1

Gs, ss

>u.

2.30

Therefore we get

Au>u,u∂Kr. 2.31

Thus, we have fromTheorem 1.1,iA, Kr, K 0, for 0 < rr0. On the other hand, the

second equality of2.27implies for everyM >0, there is anR0> r0, such that

(10)

Here we chooseM >0 satisfying2.28. Foru∂KR, RR0, we have definition ofKRthat

ut≥Γu ΓR, ta, ρb. 2.33

It follows from2.32that

Aut0 b

ρa

Gt0, s

fs, uωsu0

ωss

≥Γ

b

ρaGs, sf

s, uωsu0

ωss

≥Γ

E1

Gs, sfs, uωss

≥ΓM

E1

Gs, suωss

≥Γ2MR

E1

Gs, ss

> Ru.

2.34

This shows that

Au>u,uKR. 2.35

Thus, byTheorem 1.1, we conclude thatiA, KR, K 0 forRR0. The proof is therefore

complete.

3. Existence of One Positive Solution

In this section, we investigate the conditions for the existence of at least one positive solution of the BVP1.3.

In the next theorem, we will also assume that the following condition onft, v.

H6:

lim inf v→0 tmina,b

ft, v

v > kλ1, lim supv→∞ max ta,b

ft, v

v < qλ1, 3.1

wherek >0 is large enough such that

kΓ

E1

ϕ1ssb

(11)

andq >0 is small enough such that

Theorem 3.1. If (H1)–(H6) are satisfied, then the BVP1.3has at least one positive solution.

Proof. Fix 0< m <1< m1and letf1u umum1foru≥0. Then,f1usatisfies2.27. Define

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We now prove thatHt, u/ufor allt∈0,1andu∂Kr1. In fact, if there existst0 ∈0,1

and the boundary conditions

αu1

by parts in the left-hand side two times, we obtain

(13)

We also have

λ1 b

ρaϕ1su1ssλ1

u1b

ρaϕ1ss. 3.14

Equations3.13and3.14lead to

λ1≥λ1

k. 3.15

This is impossible. ThusHt, u/uforu∂Kr1 andt ∈ 0,1. By3.7and the homotopy

invariance of the fixed-point indexsee11, we get that

iA, Kr1, K

iH0,·, Kr1, K

iH1,·, Kr1, K

i A, Kr1, K

0. 3.16

On the other hand, according to the second inequality ofH6, there exist >0 andR> R0

such that

ft, u1−

u, u > R, ta, b. 3.17

We define

C: max

atb,0≤uRft, u

1−

u1, 3.18

then it follows that

ft, u1−

uC, u≥0, ta, b. 3.19

DefineH1 :0,KKbyH1t, u tAu, thenH1is a completely continuous operator.

We claim that there existsR1≥Rsuch that

(14)

In fact, ifH1t0, u1 u1for someu1∈Kand 0≤t0≤1, then

λ1 b

ρau11ss

b

ρaf

s, u1

ωsu0

ωsϕ1ss

q

λ1−

q

u1u0 b

ρaϕ1ssC

b

ρaϕ1ss

q

λ1−

q

u1 b

ρaϕ1ssC1

b

ρaϕ1ss,

3.21

λ1 b

ρau11ssλ1

ρb

ρau11ss

λu1 ρb

ρa

ϕ1ss

λ1qu1 b

ρa

ϕ1ss,

3.22

whereC11−/qu0C.Combining3.21with3.22, we have

u1 C1

R1. 3.23

LetR1max{R,R1}1.Then we get

H1t, u/u, fort∈0,1, uK,uR1. 3.24

Consequently, by the homotopy invariance of the fixed-point index, we have

iA, KR1, K

iH11,·, KR1, K

iH10,·, KR1, K

iΘ, KR1, K

1, 3.25

whereΘis zero operator. Use3.16and3.25to conclude that

iA, KR1\Kr1, K

iA, KR1, K

iA, Kr1, K

1−01. 3.26

Hence,Ahas a fixed point inKR1\Kr1.

Letyt ut u0t. Sinceyt utforta, band 0 < r1 ≤ u ua,b

ya,bR1.

H7

lim sup v→0 tmax∈a,b

ft, v v < qλ1,

lim inf v→∞ tmin∈a,b

ft, v

v > kλ1, ξt≡0, ηt≡0.

(15)

Theorem 3.2. If (H1)–(H5) and (H7) are satisfied, then the BVP 1.3 has at least one positive solution.

Proof. DefineH1 : 0,KKbyH1t, u tAu, thenH1 is a completely continuous

operator. By the first inequality inH7, there exist >0 and 0< r1≤r0such that

ft, v1−

v,ta, b,0≤vr1. 3.28

We claim thatH1t, u/ufor 0 ≤ t ≤ 1 andu∂Kr1. In fact, if there exist 0 ≤ t0 ≤ 1 and u1 ∈∂Kr1 such thatH1t0, u1 u1, thenu1tsatisfies the boundary condition3.11. Since ξt≡0, ηt≡0, we haveu0t≡0. Then we have

uΔ1∇t qtu1t t0f

t, u1

ωt, atb. 3.29

Multiplying the last equation byϕ1tintegrating fromatob, by3.28, we obtain

λ1 b

ρa

ϕ1su1sst0 b

ρa

fs, u1

ωsϕ1ss

b

ρa

fs, u1

ωsϕ1ss

1−u1

b

ρaϕ1ss,

3.30

then we have

λ1 b

ρau11ssλ1

ρb

ρau11ss

λu1 ρb

ρa

ϕ1ss

λ1qu1 b

ρa

ϕ1ss.

3.31

Equations3.30and3.31lead to

λ1qλq1−. 3.32

This is impossible. By homotopy invariance of the fixed-point index, we get that

iA, Kr1, K

iH11,·, Kr1, K

iH10,·, Kr1, K

iΘ, Kr1, K

(16)

DefineH:0,KKbyHt, u 1−tAutAu , thenHis a completely continuous

then, it is obvious that

(17)

Consequently, by3.8and the homotopy invariance of the fixed-point index, we have

iA, KR1, K

iH0,·, KR1, K

iH1,·, KR1, K

i A, KR1, K

0. 3.40

In view of3.33and3.40, we obtain

iA, KR1\Kr1, K

iA, KR1, K

iA, Kr1, K

0−1−1. 3.41

Therefore,Ahas a fixed point inKR1\Kr1. The proof is completed.

Corollary 3.3. Using the following (H8) or (H9) instead of (H6) or (H7), the conclusions of Theorems 3.1and3.2are true. Forta, b,

H8

lim v→0

ft, v

v

, lim

v→∞

ft, v

v

0 sublinear; 3.42

H9

lim v→0

ft, v

v

0, lim v→∞

ft, v

v

superlinear, ξt≡0, ηt≡0. 3.43

4. Existence of Three Positive Solutions

In this section, usingTheorem 1.2the Leggett-Williams fixed-point theoremwe prove the existence of at least three positive solutions to the BVP1.3.

Define the continuous concave functional ψ : K → 0,∞ to be ψu : minta,ρbut, and the constants

M:

min ta,ρb

ρb

ρa

Gt, ss 1

, 4.1

N:

b

ρaGs, ss. 4.2

Theorem 4.1. Suppose there exists constants0< p < q < q/Γ≤rsuch that

D1ft, v< p/Nforta, b, v∈0, p;

D2ft, vqMforta, ρb, vq, q/Γ;

D3one of the following is satisfied:

alim supv→ ∞maxta,bft, v/v<1/N,

(18)

where Γ,M, and R, are as defined in2.12,4.1, 4.2, respectively. Then the boundary value problem1.3has at least three positive solutionsu1, u2,andu3satisfying

u1< p, min

ta,ρbu2t> q, p <u3 witht∈mina,ρbu3t< q. 4.3

Proof. The technique here similar to that used in5Again the coneK, the operatorAis the same as in the previous sections. For alluKwe haveψuu.IfuKr, thenur and the conditionaofD3imply that

lim sup v→ ∞ tmax∈a,b

ft, v v <

1

N. 4.4

Thus there exist aζ > 0 and < 1/Rsuch that ifv > ζ, then maxta,bft, v/v < . For

λ:max{ft, v:v∈0, ζ, ta, b}, we haveft, vfor allv≥0, for allta, b.

Pick any

r >max

q

Γ,

λ

1/N

. 4.5

ThenuKr implies that

Au max

ta,b

b

ρa

Gt, sfs, uωss

uλN < rNr1−N r. 4.6

ThusA:KrKr.

The condition b of D3 implies that there exists a positive number r such that

ft, vr/Nforta, bandv∈0, r. IfuKr, then

Au max

ta,b

b

ρa

Gt, sfs, uωss

r N

Nr. 4.7

ThusA: KrKr.Consequently, the assumptionD3holds, then there exist a numberr such thatr > q/ΓandA:KrKr.

The remaining conditions ofTheorem 1.2will now be shown to be satisfied.

ByD1and argument above, we can get thatA:KpKp.Hence, conditioniiof Theorem 1.2is satisfied.

We now consider conditioniofTheorem 1.2. ChooseuKtsq/2 forta, b, wheresq/Γ. ThenuKtKψ, q, q/ΓandψuK ψsq/2> q,so that{Kψ, p, q/Γ:

ψu> q}/{}. ForuKψ, q, q/Γ, we havequtq/Γ,ta, ρb. Combining with

D2, we get

(19)

forta, ρb. Thus, we have

ψAu min

ta,ρb

b

ρaGt, sf

s, uωss

> min ta,ρb

ρb

ρaGt, sf

s, uωssqM

M q.

4.9

As a result,uKψ, q, syieldsψAu> q.

Lastly, we considerTheorem 1.2iii. Recall that A : KK. IfuKψ, q, rand

Au> q/Γ, then

ψAu min

ta,ρbAut≥ΓAu>Γ q

Γ q. 4.10

Thus, all conditions ofTheorem 1.2are satisfied. It implies that the TPBVP1.3has at least three positive solutionsu1, u2, u3with

u1< p, ψu2> q, p <u3 with ψu3< q. 4.11

5. Examples

Example 5.1. LetT{n/2:n∈N0}.Consider the BVP:

yΔ∇t yt

y2t−1, t∈0,3⊂T, yρt−2yΔρtt2, t∈−1,0,

3yt 4yΔt t−3, t∈3,5.

5.1

Thena0, b3, τ1−1, τ25, α1, β2, γ 3, δ4,and

qt 1, ξt t2, ηt t3, ft, vv, ωt 2t1. 5.2

Since limv→0ft, v/v ∞, limvft, v/v 0. It is clear thatH1–H5andH8 are satisfied. Thus, byCorollary 3.3, the BVP5.1has at least one positive solution.

Example 5.2. Let us introduce an example to illustrate the usage ofTheorem 4.1. Let

T

4n2

n29 :n∈N0

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Consider the TPBVP:

yΔ∇t 500y

2t21 y2t21300, t

2 5,2

,

y0 0, yΔt 0, t∈2,5.

5.4

Thena2/5, b2, τ12/5, τ25, α1, β0, δ1, γ 0,and

ωt t21, ξt

t−2

5

2

, ηt 0, ft, v 500v

2

v2300. 5.5

The Green function of the BVP5.4has the form

Gt, s ⎧ ⎪ ⎪ ⎨ ⎪ ⎪ ⎩

s, if 0≤st≤ 64

25,

t, if 0≤ts≤ 64

25.

5.6

Clearly,fis continuous and increasing0,∞. We can also see thatαγ >0. By2.12,4.1, and4.2, we getΓ 1/5, M65/32, andN11496/4225.

Now we check that D1, D2, and b of D3 are satisfied. To verify D1, as

f1/10 0.01666611113, we takep1/10, then

fy< p

N 0.03675191371, y∈0, p 5.7

andD1holds. Note thatf3/2 3.722084367, when we setq3/2,

fyqM3.046875000, yq,5q 5.8

holds. It means thatD2is satisfied. Letr 1500, we have

fy≤500< r

N 551.2787056, y∈0, r, 5.9

from limy→ ∞fy 500, so thatbofD3is met. Summing up, there exist constantsp

1/10, q3/2,andr 1500 satisfying

0< p < q < qΓ < r. 5.10

Thus, byTheorem 4.1, the TPBVP5.4has at least three positive solutionsy1, y2, y3with

y1< 1

10, ψy2> 3 2,

1

10 <y3 withψy3< 3

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References

1 D. Jiang and P. Weng, “Existence of positive solutions for boundary value problems of second-order functional-differential equations,”Electronic Journal of Qualitative Theory of Differential Equations, no. 6, pp. 1–13, 1998.

2 N. Aykut, “Existence of positive solutions for boundary value problems of second-order functional difference equations,”Computers & Mathematics with Applications, vol. 48, no. 3-4, pp. 517–527, 2004.

3 M. Bohner and A. Peterson,Dynamic Equations on Time Scales: An Introduction with Applications, Birkh¨auser, Boston, Mass, USA, 2001.

4 M. Bohner and A. Peterson, Eds.,Advances in Dynamic Equations on Time Scales, Birkh¨auser, Boston, Mass, USA, 2003.

5 D. R. Anderson, “Existence of solutions for nonlinear multi-point problems on time scales,”Dynamic Systems and Applications, vol. 15, no. 1, pp. 21–33, 2006.

6 D. R. Anderson, R. Avery, J. Davis, J. Henderson, and W. Yin, “Positive solutions of boundary value problems,” inAdvances in Dynamic Equations on Time Scales, pp. 189–249, Birkh¨auser, Boston, Mass, USA, 2003.

7 D. R. Anderson, R. Avery, and A. Peterson, “Three positive solutions to a discrete focal boundary value problem,”Journal of Computational and Applied Mathematics, vol. 88, no. 1, pp. 103–118, 1998.

8 F. M. Atici and G. Sh. Guseinov, “On Green’s functions and positive solutions for boundary value problems on time scales,”Journal of Computational and Applied Mathematics, vol. 141, no. 1-2, pp. 75–99, 2002.

9 C. J. Chyan, J. M. Davis, J. Henderson, and W. K. C. Yin, “Eigenvalue comparisons for differential equations on a measure chain,”Electronic Journal of Differential Equations, vol. 1998, no. 35, pp. 1–7, 1998.

10 J. M. Davis, P. W. Eloe, and J. Henderson, “Comparison of eigenvalues for discrete Lidstone boundary value problems,”Dynamic Systems and Applications, vol. 8, no. 3-4, pp. 381–388, 1999.

11 C.-Z. Bai and J.-X. Fang, “Existence of multiple positive solutions for functional differential equations,”Computers & Mathematics with Applications, vol. 45, no. 12, pp. 1797–1806, 2003.

12 J. M. Davis, K. R. Prasad, and W. K. C. Yin, “Nonlinear eigenvalue problems involving two classes of functional differential equations,”Houston Journal of Mathematics, vol. 26, no. 3, pp. 597–608, 2000.

13 E. R. Kaufmann and Y. N. Raffoul, “Positive solutions for a nonlinear functional dynamic equation on a time scale,”Nonlinear Analysis: Theory, Methods & Applications, vol. 62, no. 7, pp. 1267–1276, 2005.

14 D. J. Guo and V. Lakshmikantham,Nonlinear Problems in Abstract Cones, vol. 5 ofNotes and Reports in Mathematics in Science and Engineering, Academic Press, Boston, Mass, USA, 1988.

References

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4.10 A diagrammatic representation of the relationship between the lexical items ‘tea’ / ‘war’ and the canonical conceptual oppositions on which they are

• To deliver three groupwork programmes in Calderdale Women’s Centre, which address the impact of domestic violence on positive parenting and relationship building.. Year