10판/2. 직선운동

2-40 할리데이 10판 솔루션 일반물리학

짱세디럭스 2019. 7. 27. 04:57

v0=55[km/h]1000[m]1[km]1[h]3600[s]=27518[m/s]\begin{aligned} v_0&=55\ut{km/h}\cdot\frac{1000\ut{m}}{1\ut{km}}\cdot\frac{1\ut{h}}{3600\ut{s}} \\ &=\frac{275}{18}\ut{m/s}\\ \end{aligned} {v0=27518[m/s]a=5.18[m/s2]T=0.75[s]\begin{cases} v_0 = \frac{275}{18}\ut{m/s} \\ a=-5.18\ut{m/s^2} \\ T = 0.75\ut{s} \\ \end{cases}
(a) {xA3=40[m]tA=2.8[s]\begin{cases} x_{A3} = 40\ut{m} \\ t_A = 2.8\ut{s} \\ \end{cases} [Case A Still Run]\title{Case A Still Run} Δx=vt,ΔxA=v0tA=(27518[m/s])(2.8[s])=3859[m]42.77777777777778[m]>40[m]\begin{aligned} \Delta x&=vt, \\ \Delta x_A&=v_0t_A \\ &=(\frac{275}{18}\ut{m/s})(2.8\ut{s}) \\ &=\frac{385}{9}\ut{m}\\ &\approx 42.77777777777778\ut{m} > 40\ut{m}\\ \end{aligned} [Case A CAN Still Run]\therefore \title{Case A CAN Still Run} [Case A Brake]\title{Case A Brake} ΔxS=v0T=27518[m/s]0.75[s]=27524[m]\begin{aligned} \Delta x_S &=v_0T \\ &= \frac{275}{18}\ut{m/s}\cdot0.75\ut{s} \\ &= \frac{275}{24}\ut{m} \end{aligned} ta=tA0.75[s]=2.8[s]0.75[s]=2.05[s] \begin{aligned} t_a &= t_A-0.75\ut{s} \\ &= 2.8\ut{s}-0.75\ut{s} \\ &= 2.05\ut{s} \\ \end{aligned} Δx=v0t+12at2,Δxa=v0ta+12ata2=(27518[m/s])(2.05[s])+12(5.18[m/s2])(2.05[s])2=7356589360000[m] \begin{aligned} \Delta x &= v_0t+\frac{1}{2}at^2, \\ \Delta x_a &= v_0t_a+\frac{1}{2}at_a^2 \\ &= (\frac{275}{18}\ut{m/s})(2.05\ut{s})+\frac{1}{2}(-5.18\ut{m/s^2})(2.05\ut{s})^2 \\ &= \frac{7356589}{360000}\ut{m}\\ \end{aligned} xA=xS+xa=27524[m]+7356589360000[m]=11481589360000[m]31.89330277777778[m]<40[m] \begin{aligned} x_A &= x_S + x_a \\ &= \frac{275}{24}\ut{m}+\frac{7356589}{360000}\ut{m} \\ &= \frac{11481589}{360000}\ut{m} \\ &\approx 31.89330277777778\ut{m} < 40\ut{m} \end{aligned} [Case A CAN Brake]\therefore \title{Case A CAN Brake} [Case A Both Possible]\title{Case A Both Possible}
(b)
{xB3=32[m]tB=1.8[s]\begin{cases} x_{B3} = 32\ut{m} \\ t_B = 1.8\ut{s} \end{cases} [Case B Still Run]\title{Case B Still Run} Δx=vt,ΔxB=v0tB=(27518[m/s])(1.8[s])=552[m]=27.5[m]32[m]\begin{aligned} \Delta x&=vt, \\ \Delta x_B&=v_0t_B \\ &=(\frac{275}{18}\ut{m/s})(1.8\ut{s}) \\ &=\frac{55}{2}\ut{m}\\ &= 27.5\ut{m} \ngtr 32\ut{m}\\ \end{aligned} [Case B can NOT Still Run]\therefore \title{Case B can NOT Still Run} [Case B Brake]\title{Case B Brake} tb=tB0.75[s]=1.8[s]0.75[s]=1.05[s]\begin{aligned} t_b &= t_B-0.75\ut{s} \\ &= 1.8\ut{s}-0.75\ut{s} \\ &= 1.05\ut{s} \\ \end{aligned} Δx=v0t+12at2,Δxb=v0tb+12atb2=(27518[m/s])(1.05[s])+12(5.18[m/s2])(1.05[s])2=1582343120000[m] \begin{aligned} \Delta x &= v_0t+\frac{1}{2}at^2, \\ \Delta x_b &= v_0t_b+\frac{1}{2}at_b^2 \\ &= (\frac{275}{18}\ut{m/s})(1.05\ut{s})+\frac{1}{2}(-5.18\ut{m/s^2})(1.05\ut{s})^2 \\ &= \frac{1582343}{120000}\ut{m}\\ \end{aligned} xB=xS+xb=27524[m]+1582343120000[m]=98578140000[m]=24.644525[m]<32[m] \begin{aligned} x_B &= x_S + x_b \\ &= \frac{275}{24}\ut{m}+\frac{1582343}{120000}\ut{m} \\ &= \frac{985781}{40000}\ut{m} \\ &= 24.644525\ut{m} < 32\ut{m} \end{aligned} [Case B CAN Brake]\therefore \title{Case B CAN Brake} [Case B Must Brake]\title{Case B Must Brake}