2013: Problems 5-6

Topic: Dynamics
Concepts: Newton’s laws, Scale reading


Solution:

The scale reads the normal force NN and assumes it is the weight mgmg. The measured mass is then mscale=N/gm_{\text{scale}}=N/g. If the elevator has acceleration aa upward, we have

Nmg=maN-mg=ma
N=m(g+a)N=m(g+a)

so

mscale=Ng=m(1+ag)m_{\text{scale}}=\frac{N}{g}=m\left(1+\frac{a}{g }\right)

In the beginning, the elevator is at rest so a=0a=0 and mscale=m=80kgm_{\text{scale}}=m=80\,\mathrm{kg}. Once the elevator starts moving, the acceleration can be found from the measured mass,

a=g(mscalem1)a=g\left(\frac{m_{\text{scale}}}{m}-1\right)

Thus, between t=2st=2\,\mathrm{s} and 4s4\,\mathrm{s} we have acceleration

a1=(10m/s2)(60kg80kg1)=2.5m/s2a_1=(10\,\mathrm{m/s^2})\left(\frac{60\,\mathrm{kg}}{80\,\mathrm{kg}}-1\right)=-2.5\,\mathrm{m/s^2}

Between t=22st=22\,\mathrm{s} and 24s24\,\mathrm{s} we have acceleration

a2=(10m/s2)(100kg80kg1)=2.5m/s2a_2=(10\,\mathrm{m/s^2})\left(\frac{100\,\mathrm{kg}}{80\,\mathrm{kg}}-1\right)=2.5\,\mathrm{m/s^2}

The student has maximum downward velocity after the downward acceleration of the elevator but before it slows down with upward acceleration. This is from t=4st=4\,\mathrm{s} to 22s22\,\mathrm{s} so the answer is C.

Topic: Kinematics
Concepts: 5 kinematics equations, Motion graphs


Solution:

We found in the previous problem the acceleration of the elevator as a function of time:

where we take the positive direction to point downwards. To find the height of the building, we calculate the distance the elevator traveled from beginning to end. Between t=2st=2\,\mathrm{s} and 4s4\,\mathrm{s} (Δt1=4s2s=2s\Delta t_1=4\,\mathrm{s}-2\,\mathrm{s}=2\,\mathrm{s}), the elevator accelerates from rest so

d1=12a(Δt1)2=12(2.5m/s2)(2s)2=5md_1=\frac{1}{2}a(\Delta t_1)^2=\frac{1}{2}(2.5\,\mathrm{m/s^2})(2\,\mathrm{s})^2=5\,\mathrm{m}

At t=4st=4\,\mathrm{s}, the elevator is moving with velocity v=aΔt1=(2.5m/s2)(2s)=5m/sv=a\Delta t_1=(2.5\,\mathrm{m/s^2})(2\,\mathrm{s})=5\,\mathrm{m/s}. From t=4st=4\,\mathrm{s} to 22s22\,\mathrm{s} (Δt2=22s4s=18s\Delta t_2=22\,\mathrm{s}-4\,\mathrm{s}=18\,\mathrm{s}), the elevator moves at constant velocity so

d2=vΔt2=(5m/s)(18s)=90md_2=v\Delta t_2=(5\,\mathrm{m/s})(18\,\mathrm{s})=90\,\mathrm{m}

From t=22st=22\,\mathrm{s} to t=24st=24\,\mathrm{s} (Δt3=24s22s=2s\Delta t_3=24\,\mathrm{s}-22\,\mathrm{s}=2\,\mathrm{s}), the elevator decelerates to rest so

d3=vΔt312a(Δt3)2=(5m/s)(2s)12(2.5m/s2)(2s)2=5md_3=v\Delta t_3-\frac{1}{2}a(\Delta t_3)^2=(5\,\mathrm{m/s})(2\,\mathrm{s})-\frac{1}{2}(2.5\,\mathrm{m/s^2})(2\,\mathrm{s})^2=5\,\mathrm{m}

Thus,

h=d1+d2+d3=5m+90m+5m=100mh=d_1+d_2+d_3=5\,\mathrm{m}+90\,\mathrm{m}+5\,\mathrm{m}=100\,\mathrm{m}

so the answer is C.

Leave a Reply

This site uses Akismet to reduce spam. Learn how your comment data is processed.

Join 259 other subscribers

F=ma Training Program
Group (2026)
Individual (2026)

1D elastic collision 1D inelastic collision 5 kinematics equations Angular kinematics Atwood machine Buoyant force Circular motion Circular orbits Conservation of angular momentum Conservation of energy Conservation of linear momentum Dimensional analysis Effective spring constant Elliptical orbits Energy dissipation Error propagation Fictitious forces Fma: Collisions Fma: Dynamics Fma: Energy Fma: Fluids Fma: Gravity Fma: Kinematics Fma: Oscillatory Motion Fma: Other Fma: Rigid Bodies Fma: System of Masses Forces in mechanics Free fall Inclined plane Kinetic energy Limiting cases Mass-spring system Moments of inertia Motion graphs Newton's laws Power Projectile motion Relative velocity Rolling motion Simple harmonic motion Statics Torque Torque from weight Work-energy theorem

Discover more from Kevin S. Huang

Subscribe now to keep reading and get access to the full archive.

Continue reading