11판/12. 평형과 탄성

12-30 할리데이 11판 솔루션 일반물리학

짱세디럭스 2024. 10. 9. 16:57
{m1=40.0[kg]=4mm2=10.0[kg]=mL=0.800[m]g=9.80665[m/s2] \begin{cases} m_1&=40.0\ut{kg}=4m\\ m_2&=10.0\ut{kg}=m\\ L&=0.800\ut{m}\\ g&=9.80665\ut{m/s^2} \end{cases} {ΣFy=0Στ=0 \begin{cases} \Sigma F_{y}&=0\\ \Sigma \tau&=0\\ \end{cases} {0=NA+NBm1gm2g0=r1m1gr2m2g+rBNB \begin{cases} 0&=N_A+N_B-m_1g-m_2g\\ 0&=-r_1m_1g-r_2m_2g+r_BN_B\\ \end{cases} {NA=rBr1rBm1g+rBr2rBm2gNB=r1rBm1g+r2rBm2g \begin{cases} N_A&=\cfrac{r_B-r_1}{r_B}m_1g+\cfrac{r_B-r_2}{r_B}m_2g\\ N_B&=\cfrac{r_1}{r_B}m_1g+\cfrac{r_2}{r_B}m_2g\\ \end{cases} {rB=L2r1=r2L4 \begin{cases} r_B&={L\over2}\\ r_1&=r_2-{L\over4} \end{cases} {NA=(710r2L)mgNB=(2+10r2L)mg \begin{cases} N_A&=\br{7-10\cdot\cfrac{r_2}{L}}mg\\ N_B&=\br{-2+10\cdot\cfrac{r_2}{L}}mg\\ \end{cases} (a,b)\ab{a,b} r2=L2, r_2={L\over2}, {NA=2mg=196.133[N]196[N]NB=3mg=294.1995[N]294[N] \begin{cases} N_A&=2mg=196.133\ut{N}\approx 196\ut{N}\\ N_B&=3mg=294.1995\ut{N}\approx 294\ut{N}\\ \end{cases} (c,d)\ab{c,d} r2=L4, r_2={L\over4}, {NA=92mg=441.29925[N]441[N]NB=12mg=49.03325[N]49.0[N] \begin{cases} N_A&={9\over2}mg=441.29925\ut{N}\approx 441\ut{N}\\ N_B&={1\over2}mg=49.03325\ut{N}\approx 49.0\ut{N}\\ \end{cases} (e)\ab{e} NA=(710r2L)mg=0, \begin{aligned} N_A&=\br{7-10\cdot\cfrac{r_2}{L}}mg=0,\\ \end{aligned} r2=710L \begin{aligned} r_2&={7\over10}L \end{aligned} m2NB=r2rB=710L12L=L5=425[m]=0.160[m]=16.0[cm] \begin{aligned} \therefore \overline{ m_2 N_B}&=r_2-r_B\\ &={7\over10}L-{1\over2}L\\ &={L\over5}\\ &={4\over25}\ut{m}\\ &=0.160\ut{m}\\ &=16.0\ut{cm}\\ \end{aligned}