11.8: Problem
- Page ID
- 32996
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\(\newcommand{\avec}{\mathbf a}\) \(\newcommand{\bvec}{\mathbf b}\) \(\newcommand{\cvec}{\mathbf c}\) \(\newcommand{\dvec}{\mathbf d}\) \(\newcommand{\dtil}{\widetilde{\mathbf d}}\) \(\newcommand{\evec}{\mathbf e}\) \(\newcommand{\fvec}{\mathbf f}\) \(\newcommand{\nvec}{\mathbf n}\) \(\newcommand{\pvec}{\mathbf p}\) \(\newcommand{\qvec}{\mathbf q}\) \(\newcommand{\svec}{\mathbf s}\) \(\newcommand{\tvec}{\mathbf t}\) \(\newcommand{\uvec}{\mathbf u}\) \(\newcommand{\vvec}{\mathbf v}\) \(\newcommand{\wvec}{\mathbf w}\) \(\newcommand{\xvec}{\mathbf x}\) \(\newcommand{\yvec}{\mathbf y}\) \(\newcommand{\zvec}{\mathbf z}\) \(\newcommand{\rvec}{\mathbf r}\) \(\newcommand{\mvec}{\mathbf m}\) \(\newcommand{\zerovec}{\mathbf 0}\) \(\newcommand{\onevec}{\mathbf 1}\) \(\newcommand{\real}{\mathbb R}\) \(\newcommand{\twovec}[2]{\left[\begin{array}{r}#1 \\ #2 \end{array}\right]}\) \(\newcommand{\ctwovec}[2]{\left[\begin{array}{c}#1 \\ #2 \end{array}\right]}\) \(\newcommand{\threevec}[3]{\left[\begin{array}{r}#1 \\ #2 \\ #3 \end{array}\right]}\) \(\newcommand{\cthreevec}[3]{\left[\begin{array}{c}#1 \\ #2 \\ #3 \end{array}\right]}\) \(\newcommand{\fourvec}[4]{\left[\begin{array}{r}#1 \\ #2 \\ #3 \\ #4 \end{array}\right]}\) \(\newcommand{\cfourvec}[4]{\left[\begin{array}{c}#1 \\ #2 \\ #3 \\ #4 \end{array}\right]}\) \(\newcommand{\fivevec}[5]{\left[\begin{array}{r}#1 \\ #2 \\ #3 \\ #4 \\ #5 \\ \end{array}\right]}\) \(\newcommand{\cfivevec}[5]{\left[\begin{array}{c}#1 \\ #2 \\ #3 \\ #4 \\ #5 \\ \end{array}\right]}\) \(\newcommand{\mattwo}[4]{\left[\begin{array}{rr}#1 \amp #2 \\ #3 \amp #4 \\ \end{array}\right]}\) \(\newcommand{\laspan}[1]{\text{Span}\{#1\}}\) \(\newcommand{\bcal}{\cal B}\) \(\newcommand{\ccal}{\cal C}\) \(\newcommand{\scal}{\cal S}\) \(\newcommand{\wcal}{\cal W}\) \(\newcommand{\ecal}{\cal E}\) \(\newcommand{\coords}[2]{\left\{#1\right\}_{#2}}\) \(\newcommand{\gray}[1]{\color{gray}{#1}}\) \(\newcommand{\lgray}[1]{\color{lightgray}{#1}}\) \(\newcommand{\rank}{\operatorname{rank}}\) \(\newcommand{\row}{\text{Row}}\) \(\newcommand{\col}{\text{Col}}\) \(\renewcommand{\row}{\text{Row}}\) \(\newcommand{\nul}{\text{Nul}}\) \(\newcommand{\var}{\text{Var}}\) \(\newcommand{\corr}{\text{corr}}\) \(\newcommand{\len}[1]{\left|#1\right|}\) \(\newcommand{\bbar}{\overline{\bvec}}\) \(\newcommand{\bhat}{\widehat{\bvec}}\) \(\newcommand{\bperp}{\bvec^\perp}\) \(\newcommand{\xhat}{\widehat{\xvec}}\) \(\newcommand{\vhat}{\widehat{\vvec}}\) \(\newcommand{\uhat}{\widehat{\uvec}}\) \(\newcommand{\what}{\widehat{\wvec}}\) \(\newcommand{\Sighat}{\widehat{\Sigma}}\) \(\newcommand{\lt}{<}\) \(\newcommand{\gt}{>}\) \(\newcommand{\amp}{&}\) \(\definecolor{fillinmathshade}{gray}{0.9}\)- Show using the component form of the cross product given by equation (11.4) that A × B = -B × A.
- A mass M is sliding on a frictionless table, but is attached to a string which passes through a hole in the center of the table as shown in Figure \(\PageIndex{8}\):. The string is gradually drawn in so the mass traces out a spiral pattern as shown in Figure \(\PageIndex{8}\):. The initial distance of the mass from the hole in the table is R and its initial tangential velocity is v. After the string is drawn in, the mass is a distance R′ from the hole and its tangential velocity is v′.
- Given R, v, and R′, find v′.
- Compute the change in the kinetic energy of the mass in going from radius R to radius R′.
- If the above change is non-zero, determine where the extra energy came from.
Figure \(\PageIndex{8}\):: Trajectory of a mass on a frictionless table attached to a string which passes through a hole in the table. The string is drawing the mass in.
- A car of mass 1000 kg is heading north on a road at 30 m s-1 which passes 2 km east of the center of town.
- Compute the angular momentum of the car about the center of town when the car is directly east of the town.
- Compute the angular momentum of the car about the center of town when it is 3 km north of the above point.
- The apparatus illustrated in Figure \(\PageIndex{9}\): is used to raise a bucket of mass M out of a well.
- What force F must be exerted to keep the bucket from falling back into the well?
- If the bucket is slowly raised a distance d, what work is done on the bucket by the rope attached to it?
- What work is done by the force F on the handle in the above case?
Figure \(\PageIndex{9}\):: A crank on a fixed axle turns a drum, thus winding the rope around the drum and raising the mass.
- Derive equations below.
- \(K_{\text {total }}=K_{\text {trans }}+K_{\text {intern }}=\left[M_{\text {total }} V_{c m}^{2} / 2\right]+\left[M_{1} v_{1}^{\prime 2} / 2+M_{2} v_{2}^{\prime 2} / 2\right] \text { . }\)
- \(\mathbf{L}_{\text {total }}=\mathbf{L}_{\text {orb }}+\mathbf{L}_{\text {spin }}=\left[M_{\text {total }} \mathbf{R}_{c m} \times \mathbf{V}_{c m}\right]+\left[M_{1} \mathbf{r}_{1}^{\prime} \times \mathbf{v}_{1}^{\prime}+M_{2} \mathbf{r}_{2}^{\prime} \times \mathbf{v}_{2}^{\prime}\right]\)
- A mass M is held up by the structure shown in Figure \(\PageIndex{10}\):. The support beam has negligible mass. Find the tension T in the diagonal wire. Hint: Compute the net torque on the support beam about point A due to the tension T and the weight of the mass M.
Figure \(\PageIndex{10}\):: A mass is supported by the tension in the diagonal wire. The support beam is free to pivot at point A.
- A system consists of two stars, one of mass M moving with velocity v1 = (0,v, 0) at position r1 = (d, 0, 0), the other of mass 2M with zero velocity at the origin.
- Find the center of mass position and velocity of the system of two stars.
- Find the spin angular momentum of the system.
- Find the internal kinetic energy of the system.
Figure \(\PageIndex{11}\):: A mass is supported by two strings.
Figure \(\PageIndex{12}\):: A ladder leaning against a wall is held in place the force F acting on the base of the ladder.
- A solid disk is rolling down a ramp tilted an angle θ from the horizontal. Compute the acceleration of the disk down the ramp and compare it with the acceleration of a block sliding down the ramp without friction.
- A mass M is suspended from the ceiling by two strings as shown in Figure \(\PageIndex{11}\):. Find the tensions in the strings.
- A man of mass M is a distance D up a ladder of length L which makes an angle \(\theta\) with respect to the vertical wall as shown in Figure \(\PageIndex{12}\):. Take the mass of the ladder to be negligible. Find the force F needed to keep the ladder from sliding if the wall and floor are frictionless and therefore can only exert normal forces A and B on the ladder.