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Zadatak 3

Statička stabilnost sa potrošačem kao impedansom: rešen zadatak

Zadatak i rešenje: prof. dr Andrija T. Sarić

Analiza elektroenergetskih sistema, TF Čačak

Zadatak

3. Za dati trofazni EES proveriti statičku stabilnost generatora. Opterećenje potrošača zameniti konstantnom impedansom.

GTP = 200 MWQ = 20 MVAr1l12 = 250 kmxv = 0,42 Ω/km2S = (100 + j50) MVAUr = 225 kVSGn = STn = 240 MVAUGn = 15,75 kVmT = 15,75/231 kV/kVxG = 185 %xT = 12 %Sk = 4000 MVAUk = 220 kV

Poznato

  • SGn=STn=240S_{Gn} = S_{Tn} = 240MVA
  • UGn=15,75U_{Gn} = 15{,}75kV
  • UTn=231U_{Tn} = 231kV
  • xG=185x_G = 185%
  • xT=12x_T = 12%
  • l12=250l_{12} = 250km
  • xv=0,42x_v = 0{,}42Ω/km
  • Sk=4000S_k = 4000MVA
  • Uk=220U_k = 220kV
  • Pp=100P_p = 100MW
  • Qp=50Q_p = 50MVAr
  • Ur=225U_r = 225kV
  • P=200P = 200MW
  • Q=20Q = 20MVAr

Rešenje

Reaktanse pojedinih elemenata (svedene na naponski nivo voda) su:

XG=xG(%)100⋅UGn2SGn⋅1mT2=185100⋅15,752240⋅231215,752=411,324 Ω;\begin{aligned} X_G &= \frac{x_G(\%)}{100} \cdot \frac{U_{Gn}^2}{S_{Gn}} \cdot \frac{1}{m_T^2} \\ &= \frac{185}{100} \cdot \frac{15{,}75^2}{240} \cdot \frac{231^2}{15{,}75^2} = 411{,}324\ \Omega; \end{aligned}
XT=uk(%)100⋅UTn2STn=12100⋅2312240=26,68 Ω;X_T = \frac{u_k(\%)}{100} \cdot \frac{U_{Tn}^2}{S_{Tn}} = \frac{12}{100} \cdot \frac{231^2}{240} = 26{,}68\ \Omega;
Xv=12xvL=12⋅0,42⋅250=52,5 Ω;X_v = \frac{1}{2}x_vL = \frac{1}{2} \cdot 0{,}42 \cdot 250 = 52{,}5\ \Omega;
Xk=Uk2Sk=22024000=12,1 Ω;X_k = \frac{U_k^2}{S_k} = \frac{220^2}{4000} = 12{,}1\ \Omega;
Z‾p=Ur2S2(P+jQ)=22521002+502(100+j50)=(405+j202,5) Ω.\begin{aligned} \ph{Z}_p &= \frac{U_r^2}{S^2}(P + \mathrm{j}Q) = \frac{225^2}{100^2 + 50^2}(100 + \mathrm{j}50) \\ &= (405 + \mathrm{j}202{,}5)\ \Omega. \end{aligned}

Ekvivalentna šema sistema je:

Ekvivalentna šema: elektromotorna sila E_Gf, reaktanse jX_G i jX_T do sabirnice napona V_r = 225/√3 kV, na kojoj je impedansa potrošača Z_p prema zemlji, pa jX_v i jX_k do napona mreže V_k.

Sopstvena impedansa koja se vidi iz čvora 1 je

Z‾=j(XG+XT)+j(Xv+Xk)Z‾pj(Xv+Xk)+Z‾p=(7,18+j497,868)=497,92 ej89,174∘=Z11ejβ.\begin{aligned} \ph{Z} &= \mathrm{j}(X_G + X_T) + \frac{\mathrm{j}(X_v + X_k)\ph{Z}_p}{\mathrm{j}(X_v + X_k) + \ph{Z}_p} \\ &= (7{,}18 + \mathrm{j}497{,}868) = 497{,}92\,\mathrm{e}^{\mathrm{j}89{,}174^\circ} = Z_{11}\mathrm{e}^{\mathrm{j}\beta}. \end{aligned}

To znači da je

β=89,174∘,ψ=π2−β=0,826∘.\beta = 89{,}174^\circ, \quad \psi = \frac{\pi}{2} - \beta = 0{,}826^\circ.

Sa zamenske šeme je elektromotorna sila iza sinhrone reaktanse generatora (izraz preveden na linijske napone i trofazne snage):

E‾G=Ur+QXG+TUr+jPXG+TUr=(263,933+j389,337) kV=470,366⋅ej55,866∘ kV.\begin{aligned} \ph{E}_G &= U_r + \frac{QX_{G+T}}{U_r} + \mathrm{j}\frac{PX_{G+T}}{U_r} = (263{,}933 + \mathrm{j}389{,}337)\ \text{kV} \\ &= 470{,}366 \cdot \mathrm{e}^{\mathrm{j}55{,}866^\circ}\ \text{kV}. \end{aligned}

Gubitak reaktivne snage u bloku generator-transformator je

ΔQ=XG+TP2+Q2Ur2=438 2002+2022252=349,538 MVAr,\Delta Q = X_{G+T}\frac{P^2 + Q^2}{U_r^2} = 438\,\frac{200^2 + 20^2}{225^2} = 349{,}538\ \text{MVAr},

tako da je unutrašnja snaga sinhronog generatora

QGun=Q+ΔQ=20+349,538=369,538 MVAr,Q_{Gun} = Q + \Delta Q = 20 + 349{,}538 = 369{,}538\ \text{MVAr},

Generator je statički stabilan ako je

∂PG∂δ=EG2Zcos⁡ψ−QGun>0,\frac{\partial P_G}{\partial\delta} = \frac{E_G^2}{Z}\cos\psi - Q_{Gun} > 0,

odnosno

∂PG∂δ=470,3662497,92cos⁡(0,826∘)−369,538=74,75>0.\frac{\partial P_G}{\partial\delta} = \frac{470{,}366^2}{497{,}92}\cos(0{,}826^\circ) - 369{,}538 = 74{,}75 > 0.

To znači da je sistem statički stabilan.

Rezultat

∂PG∂δ=74,75>0\dfrac{\partial P_G}{\partial\delta} = 74{,}75 > 0: sistem je statički stabilan.

Metod u predavanju

Slični zadaci

Teme

Stabilnost