2-66 할리데이 11판 솔루션 일반물리학 {H=40[m]Δx=14[m]g=9.80665[m/s2] \begin{cases} H&=40\ut{m}\\ \Delta x &=14\ut{m}\\ g&=9.80665\ut{m/s^2} \end{cases} ⎩⎨⎧HΔxg=40[m]=14[m]=9.80665[m/s2] S=v0t+12at2,−H=(0)t+12(−g)t2H=12gt2 \begin{aligned} S&=v_0t+\frac{1}{2}at^2,\\ -H&=(0)t+\frac{1}{2}(-g)t^2\\ H&=\frac{1}{2}gt^2\\ \end{aligned} S−HH=v0t+21at2,=(0)t+21(−g)t2=21gt2 t=2Hg \begin{aligned} t&=\sqrt{\frac{2H}{g}} \end{aligned} t=g2H $$ \begin{aligned} v&=\frac{S}{t}\\ &=\frac{S}{\sqrt{\frac{2H}{g}}}\\ &=S\sqrt{\frac{g}{2H}}\\ &=(14)\sqrt{\frac{g}{2(40)}}\\ &=\frac{7}.. 11판/2. 직선운동 2024.01.19
2-65 할리데이 11판 솔루션 일반물리학 {d=0.65[m]vB=13vAg=9.80665[m/s2] \begin{cases} d&=0.65\ut{m}\\ v_B&=\frac{1}{3}v_A\\ g&=9.80665\ut{m/s^2} \end{cases} ⎩⎨⎧dvBg=0.65[m]=31vA=9.80665[m/s2] 2aS=v2−v022(−g)(d)=vB2−vA22(−g)(0.65)=(13vA)2−vA2 \begin{aligned} 2aS&=v^2-{v_0}^2\\ 2(-g)(d)&={v_B}^2-{v_A}^2\\ 2(-g)(0.65)&=\(\frac{1}{3}v_A\)^2-{v_A}^2 \end{aligned} 2aS2(−g)(d)2(−g)(0.65)=v2−v02=vB2−vA2=(31vA)2−vA2 $$ \begin{aligned} v_A&=\frac{3}{4} \sqrt{\frac{13g}{5}}\\ &=\frac{3 }{400}\sqrt{\frac{2549729}{10}}\ut{m/s}\\ &\approx 3.787113099050515\ut{m/s}\\ &\approx 3.8\ut{m/s}\\ \end{aligne.. 11판/2. 직선운동 2024.01.19
2-64 할리데이 11판 솔루션 일반물리학 {t1=1977/01/26t2=1983/09/18S=30600[km] \begin{cases} t_1&=1977/01/26\\ t_2&=1983/09/18\\ S&=30600\ut{km} \end{cases} ⎩⎨⎧t1t2S=1977/01/26=1983/09/18=30600[km] t2−t1=2426[day] \begin{aligned} t_2-t_1&=2426\ut{day}\\ \end{aligned} t2−t1=2426[day] $$ \begin{aligned} \bar v&=\frac{S}{t}\\ &=\frac{30600\ut{km}}{2426\ut{day}}\\ &=\frac{30600\ut{km}}{2426\ut{day}}\cdot\frac{1000\ut{m}}{1\ut{km}}\cdot\frac{1\ut{day}}{24\ut{h}}\cdot\frac{1\ut{h}}{3600\ut{s}}\\ &=\frac{2125}{14556}\ut{m/s}\\ &\approx 0.1.. 11판/2. 직선운동 2024.01.19
2-63 할리데이 11판 솔루션 일반물리학 {v=360[km/h]S=2.00[km] \begin{cases} v&=360\ut{km/h}\\ S&=2.00\ut{km} \end{cases} {vS=360[km/h]=2.00[km] 2aS=v2−v022a(2)=(360)2−02 \begin{aligned} 2aS&=v^2-{v_0}^2\\ 2a(2)&=(360)^2-{0}^2\\ \end{aligned} 2aS2a(2)=v2−v02=(360)2−02 a=32400[km/h2]=3.24×104[km/h2] \begin{aligned} a&=32400\ut{km/h^2}\\ &=3.24\times10^4\ut{km/h^2}\\ \end{aligned} a=32400[km/h2]=3.24×104[km/h2] 11판/2. 직선운동 2024.01.19
2-62 할리데이 11판 솔루션 일반물리학 {a=(5.0−1.2t)[m/s2]v(0)=2.7[m/s]x(0)=7.3[m] \begin{cases} a&=(5.0-1.2t)\ut{m/s^2}\\ v(0)&=2.7\ut{m/s}\\ x(0)&=7.3\ut{m}\\ \end{cases} ⎩⎨⎧av(0)x(0)=(5.0−1.2t)[m/s2]=2.7[m/s]=7.3[m] (a)\ab{a}(a) Δv=∫0ta dt=∫0t(5−1.2t) dt=5t−35t2 \begin{aligned} \Delta v&=\int_0^t a\dd t\\ &=\int_0^t (5-1.2t)\dd t\\ &=5t-\frac{3}{5}t^2 \end{aligned} Δv=∫0tadt=∫0t(5−1.2t)dt=5t−53t2 ∴v=v(0)+Δv=2.7+5t−35t2 \begin{aligned} \therefore v&=v(0)+\Delta v\\ &=2.7+5t-\frac{3}{5}t^2\\ \end{aligned} ∴v=v(0)+Δv=2.7+5t−53t2 a=5−1.2t1=0t1=256[s] \begin{aligned} a&=5-1.2t_1=0\\ t_1&=\frac{25}{6}\ut{s}\\ \end{aligned} at1=5−1.2t1=0=625[s] $$ \begin{.. 11판/2. 직선운동 2024.01.18
2-61 할리데이 11판 솔루션 일반물리학 {H=60[m]t1=t2−1.6[s]t2:Landg=9.80665[m/s2] \begin{cases} H&=60\ut{m}\\ t_1&=t_2-1.6\ut{s}\\ t_2&:\text{Land}\\ g&=9.80665\ut{m/s^2} \end{cases} ⎩⎨⎧Ht1t2g=60[m]=t2−1.6[s]:Land=9.80665[m/s2] S=v0t+12at2,−H=(0)t2+12(−g)t22H=12gt2260=12gt22 \begin{aligned} S&=v_0t+\frac{1}{2}at^2,\\ -H&=(0)t_2+\frac{1}{2}(-g){t_2}^2\\ H&=\frac{1}{2}g{t_2}^2\\ 60&=\frac{1}{2}g{t_2}^2\\ \end{aligned} S−HH60=v0t+21at2,=(0)t2+21(−g)t22=21gt22=21gt22 t2=230g \begin{aligned} t_2&=2\sqrt\frac{30}{g}\\ \end{aligned} t2=2g30 $$ \begin{aligned} t_1&=t_2-1.6\ut{s}\\ &=2\sqrt\frac{30}{g}-1.6\ut{s} \end{ali.. 11판/2. 직선운동 2024.01.18
2-60 할리데이 11판 솔루션 일반물리학 {vA=15[km/h]vB=30[km/h] \begin{cases} v_A&=15\ut{km/h}\\ v_B&=30\ut{km/h}\\ \end{cases} {vAvB=15[km/h]=30[km/h] vˉ=SA+SBtA+tB=2SSvA+SvB=21vA+1vB=2115+130[km/h]=20[km/h] \begin{aligned} \bar v&=\frac{S_A+S_B}{t_A+t_B}\\ &=\frac{2S}{\cfrac{S}{v_A}+\cfrac{S}{v_B}}\\ &=\frac{2}{\cfrac{1}{v_A}+\cfrac{1}{v_B}}\\ &=\frac{2}{\cfrac{1}{15}+\cfrac{1}{30}}\ut{km/h}\\ &=20\ut{km/h} \end{aligned} vˉ=tA+tBSA+SB=vAS+vBS2S=vA1+vB12=151+3012[km/h]=20[km/h] 11판/2. 직선운동 2024.01.18
2-59 할리데이 11판 솔루션 일반물리학 {t=4.8[s]v0=0v1=60[km/h]=503[m/s] \begin{cases} t&=4.8\ut{s}\\ v_0&=0\\ v_1&=60\ut{km/h}=\frac{50}{3}\ut{m/s}\\ \end{cases} ⎩⎨⎧tv0v1=4.8[s]=0=60[km/h]=350[m/s] (a)\ab{a}(a) v=v0+at,503=0+a(4.8) \begin{aligned} v&=v_0+at,\\ \frac{50}{3}&=0+a(4.8)\\ \end{aligned} v350=v0+at,=0+a(4.8) a=12536[m/s2]≈3.472222222222222[m/s2]≈3.5[m/s2] \begin{aligned} a&=\frac{125}{36}\ut{m/s^2}\\ &\approx 3.472222222222222\ut{m/s^2}\\ &\approx 3.5\ut{m/s^2}\\ \end{aligned} a=36125[m/s2]≈3.472222222222222[m/s2]≈3.5[m/s2] (b)\ab{b}(b) $$ \begin{aligned} S&=\frac{1}{2}(v+v_0)t,\\ &=\frac{1}{2}\(\frac{50}{3}+0\).. 11판/2. 직선운동 2024.01.18
2-58 할리데이 11판 솔루션 일반물리학 {t0:Startt1:Max Speedt2:StoptA:t0→1tB:t1→2 \begin{cases} t_0&:\text{Start}\\ t_1&:\text{Max Speed}\\ t_2&:\text{Stop}\\ t_A&:t_{0\rarr1}\\ t_B&:t_{1\rarr2}\\ \end{cases} ⎩⎨⎧t0t1t2tAtB:Start:Max Speed:Stop:t0→1:t1→2 {SA=2.1[m]v1=6.0[m/s]aB=−3.0[m/s2] \begin{cases} S_A&=2.1\ut{m}\\ v_1&=6.0\ut{m/s}\\ a_B&=-3.0\ut{m/s^2}\\ \end{cases} ⎩⎨⎧SAv1aB=2.1[m]=6.0[m/s]=−3.0[m/s2] [Time A]\title{Time A}[Time A] S=12(v+v0)t,SA=12(v1+v0)tA2.1=12(6+0)tA \begin{aligned} S&=\frac{1}{2}(v+v_0)t,\\ S_A&=\frac{1}{2}(v_1+v_0)t_A\\ 2.1&=\frac{1}{2}(6+0)t_A\\ \end{aligned} SSA2.1=21(v+v0)t,=21(v1+v0)tA=21(6+0)tA $$ \begin{aligned} t_A&=\frac{.. 11판/2. 직선운동 2024.01.18
2-57 할리데이 11판 솔루션 일반물리학 {S=1.20[m]v1=530[m/s] \begin{cases} S&=1.20\ut{m}\\ v_1&=530\ut{m/s}\\ \end{cases} {Sv1=1.20[m]=530[m/s] S=12(v+v0)t,1.2=12(530+0)t \begin{aligned} S&=\frac{1}{2}(v+v_0)t,\\ 1.2&=\frac{1}{2}(530+0)t\\ \end{aligned} S1.2=21(v+v0)t,=21(530+0)t t=61325[s]≈0.004528301886792453[s]≈4.54×10−3[s]≈4.54[ms] \begin{aligned} t&=\frac{6}{1325}\ut{s}\\ &\approx 0.004528301886792453\ut{s}\\ &\approx 4.54\times10^{-3}\ut{s}\\ &\approx 4.54\ut{ms}\\ \end{aligned} t=13256[s]≈0.004528301886792453[s]≈4.54×10−3[s]≈4.54[ms] 11판/2. 직선운동 2024.01.18