Zoezi la thermodynamiki lililofanyiwa kazi

Kukokotoa integrali ya umbo tofauti kwenye njia

Zoezi 6 · Somo 4Kanuni ya Kwanza ya Thermodynamiki

  • umbo tofauti
  • diferenshali kamili
  • kigezo cha Schwarz
  • integrali ya mstari

Toleo la kazi — zoezi hili bado liko chini ya ukaguzi.

Swali

Fikiria maumbo mawili tofauti

ω1=ydx+xdy,ω2=ydx,\omega_1 = y\,\mathrm{d}x + x\,\mathrm{d}y, \qquad \omega_2 = y\,\mathrm{d}x,

na njia tatu zinazounganisha asili O(0,0)O(0,0) na nukta M(1,1)M(1,1): njia γ1\gamma_1 ni kipande cha mlalo O(1,0)O\to(1,0) kikifuatwa na kipande cha wima (1,0)M(1,0)\to M; njia γ2\gamma_2 ni kipande cha wima O(0,1)O\to(0,1) kikifuatwa na kipande cha mlalo (0,1)M(0,1)\to M; na njia γ3\gamma_3 ni kipande cha mstari kinachounganisha OO moja kwa moja na MM.

  1. Onyesha kuwa ω1\omega_1 ni kamili kwa kupata funksioni ff ambayo ω1=df\omega_1=\mathrm{d}f.
  2. Kokotoa γ1ω1\int_{\gamma_1}\omega_1 na γ2ω1\int_{\gamma_2}\omega_1 kwa kuweka parameta kwa kila kipande. Pata tena jibu bila kukokotoa.
  3. Tumia kigezo cha Schwarz kwa ω2\omega_2. Tunaweza kuhitimisha nini?
  4. Kokotoa γ1ω2\int_{\gamma_1}\omega_2, γ2ω2\int_{\gamma_2}\omega_2 na γ3ω2\int_{\gamma_3}\omega_2. Toa maoni.

Kidokezo

Kidokezo
Kwenye kipande cha mlalo dy=0\mathrm{d}y=0, na kwenye kipande cha wima dx=0\mathrm{d}x=0: kila integrali hupunguzwa kuwa integrali rahisi.

Jibu la kina

Suluhisho
Swali la 1. f(x,y)=xyf(x,y)=xy inafaa, kwa sababu f/x=y\partial f/\partial x=y na f/y=x\partial f/\partial y=x.

Swali la 2. Kwa mkunjo uliowekewa parameta kwa t(x(t),y(t))t\mapsto\bigl(x(t),y(t)\bigr), tuna

γω1=[y(t)x(t)+x(t)y(t)]dt.\int_\gamma\omega_1 = \int \left[y(t)x'(t)+x(t)y'(t)\right]\,\mathrm{d}t.

Njia γ1\gamma_1 ni muungano wa vipande viwili. Kwenye cha kwanza, x(t)=tx(t)=t na y(t)=0y(t)=0, huku t[0,1]t\in[0,1]; hivyo dx=dt\mathrm{d}x=\mathrm{d}t na dy=0\mathrm{d}y=0. Kwenye cha pili, x(t)=1x(t)=1 na y(t)=ty(t)=t, bado t[0,1]t\in[0,1]; hivyo dx=0\mathrm{d}x=0 na dy=dt\mathrm{d}y=\mathrm{d}t. Kwa hiyo,

I1=γ1ω1=01(0×1+t×0)dt+01(t×0+1×1)dt=0+01dt=1.\begin{aligned} I_1 = \int_{\gamma_1}\omega_1 &= \int_0^1\left(0\times 1+t\times 0\right)\,\mathrm{d}t + \int_0^1\left(t\times 0+1\times 1\right)\,\mathrm{d}t \\ &= 0+\int_0^1\mathrm{d}t = 1. \end{aligned}

Kwa γ2\gamma_2, kipande cha kwanza kina x(t)=0x(t)=0, y(t)=ty(t)=t, kisha cha pili kina x(t)=tx(t)=t, y(t)=1y(t)=1, huku t[0,1]t\in[0,1] katika hali zote mbili. Hivyo

I2=γ2ω1=01(t×0+0×1)dt+01(1×1+t×0)dt=0+01dt=1.\begin{aligned} I_2 = \int_{\gamma_2}\omega_1 &= \int_0^1\left(t\times 0+0\times 1\right)\,\mathrm{d}t + \int_0^1\left(1\times 1+t\times 0\right)\,\mathrm{d}t \\ &= 0+\int_0^1\mathrm{d}t = 1. \end{aligned}

Thamani hizi mbili ni sawa. Tungeweza kutabiri bila hesabu: kwa kuwa ω1=df\omega_1=\mathrm{d}f na f(x,y)=xyf(x,y)=xy, integrali yake hutegemea ncha pekee,

γω1=f(M)f(O)=f(1,1)f(0,0)=1.\int_\gamma\omega_1=f(M)-f(O)=f(1,1)-f(0,0)=1.

Swali la 3. Tuandike ω2=A(x,y)dx+B(x,y)dy\omega_2=A(x,y)\,\mathrm{d}x+B(x,y)\,\mathrm{d}y. Hapa A(x,y)=yA(x,y)=y na B(x,y)=0B(x,y)=0. Kama umbo lingekuwa kamili, kigezo cha Schwarz kingetoa

Ay=Bx.\frac{\partial A}{\partial y}=\frac{\partial B}{\partial x}.

Lakini A/y=1\partial A/\partial y=1 ilhali B/x=0\partial B/\partial x=0. Derivativi mseto ni tofauti: kwa hiyo ω2\omega_2 si kamili. Integrali yake inaweza kutegemea njia kati ya OO na MM, kama hesabu inayofuata inavyoonyesha.

Swali la 4. Kwa kuwa ω2=ydx\omega_2=y\,\mathrm{d}x, ni badiliko la xx linalofanyika wakati yy si sifuri pekee linaloweza kuchangia integrali. Kwa kutumia tena uparametishaji wa awali, kwenye γ1\gamma_1 tunapata

J1=γ1ω2=010×1dt+01t×0dt=0.\begin{aligned} J_1 =\int_{\gamma_1}\omega_2 &=\int_0^1 0\times 1\,\mathrm{d}t +\int_0^1 t\times 0\,\mathrm{d}t \\ &=0. \end{aligned}

Kwenye γ2\gamma_2, kipande cha kwanza kina x(t)=0x(t)=0, hivyo dx=0\mathrm{d}x=0; kwenye cha pili, x(t)=tx(t)=t, y(t)=1y(t)=1 na dx=dt\mathrm{d}x=\mathrm{d}t. Basi

J2=γ2ω2=01t×0dt+011×1dt=1.\begin{aligned} J_2 =\int_{\gamma_2}\omega_2 &=\int_0^1 t\times 0\,\mathrm{d}t +\int_0^1 1\times 1\,\mathrm{d}t \\ &=1. \end{aligned}

Hatimaye, kipande cha ulalo γ3\gamma_3 kinawekwa parameta waziwazi kwa

x(t)=t,y(t)=t,t[0,1],x(t)=t,\qquad y(t)=t,\qquad t\in[0,1],

hivyo dx=dt\mathrm{d}x=\mathrm{d}t na dy=dt\mathrm{d}y=\mathrm{d}t. Tunapata

J3=γ3ω2=01y(t)x(t)dt=01tdt=12.J_3 =\int_{\gamma_3}\omega_2 =\int_0^1 y(t)x'(t)\,\mathrm{d}t =\int_0^1 t\,\mathrm{d}t =\frac12.

Njia zote tatu zina ncha zilezile lakini zinatoa thamani tatu tofauti: J1=0J_1=0, J2=1J_2=1 na J3=1/2J_3=1/2. Huu ndio utegemezi wa njia unaotambulisha umbo tofauti lisilo kamili.