17 worked answers · short steps first, explanations when you need them
Chapter 6 Exercises
Textbook pages 101–103
Question 1
Where is the centre of mass of a uniform sphere, cylinder, ring and cube? Must a body’s centre of mass lie inside its material?
Steps only
Symmetry places the centre of mass at each shape’s geometric centre: the sphere’s centre, the cylinder’s midpoint on its axis, the ring’s centre, and the cube’s centre.
Answer
At each shape’s geometric centre. No; for example, a ring’s centre of mass is in its empty middle.
Question 2
In an HCl molecule, the nuclei are 1.27 Å apart. Chlorine is 35.5 times as massive as hydrogen. Find the molecule’s centre of mass, treating the nuclei as point masses.
Steps only
Put H at x=0 and Cl at x=1.27 Å. The centre of mass is X=(mH·0+mCl·1.27)/(mH+mCl).
Answer
The centre of mass is about 1.235 Å from H, or 0.035 Å from Cl.
Question 3
A child sits on a trolley moving at speed V along a smooth horizontal floor. The child stands and runs around on the trolley. What is the speed of the trolley-child system’s centre of mass?
Steps only
There is no net external horizontal force on the trolley-child system, so its total horizontal momentum and centre-of-mass velocity stay constant.
Answer
V; the centre-of-mass speed does not change.
Question 4
Show that the area of a triangle formed by vectors a and b is half the magnitude of a×b.
Steps only
The parallelogram made by a and b has base |a| and perpendicular height |b|sinθ, so its area is |a||b|sinθ.
Answer
Atriangle=½|a×b|.
Question 5
Explain why |a·(b×c)| gives the volume of the parallelepiped formed by vectors a, b and c.
Steps only
The magnitude |b×c| is the area of the base parallelogram. The component of a perpendicular to that base is the height.
Answer
Volume=|a·(b×c)|.
Question 6
A particle has position r=(x,y,z) and momentum p=(px,py,pz). Find the components of angular momentum and show that for motion in the xy-plane only the z-component remains.
Steps only
Angular momentum is L=r×p. Expanding the cross product gives Lx=ypz−zpy, Ly=zpx−xpz and Lz=xpy−ypx.
Answer
L=(ypz−zpy, zpx−xpz, xpy−ypx). In the xy-plane, only Lz can be non-zero.
Question 7
Two particles of mass m and speed v move in opposite directions along parallel lines separated by distance d. Show that the total angular momentum is the same about any chosen point.
Steps only
Their momenta are equal and opposite, so total momentum is zero. Shifting the origin by vector a changes total angular momentum by −a×Ptotal.
Answer
The angular momentum is independent of the chosen point; its magnitude is mvd.
Question 8
A 2 m non-uniform bar hangs at rest from two strings. The strings make 36.9° and 53.1° with the vertical at the left and right ends. Find the centre of gravity’s distance d from the left end.
Steps only
Let the left and right tensions be TL and TR. Horizontal balance gives 0.6TL=0.8TR, so TL=4TR/3. Vertical balance gives 0.8TL+0.6TR=W, hence TR=0.6W.
Answer
The centre of gravity is 0.72 m from the left end.
Question 9
A car has mass 1800 kg, axle separation 1.8 m and centre of gravity 1.05 m behind the front axle. Find the ground’s upward force on each front wheel and on each back wheel. Use g=9.8 m/s².
Steps only
Let total upward reactions at the front and back axles be Ff and Fb. Vertical balance gives Ff+Fb=mg. Taking moments about the front axle: Fb×1.8=mg×1.05.
Answer
Each front wheel: about 3.68×10³ N. Each back wheel: about 5.15×10³ N.
Question 10
Equal torques act for equal times on a hollow cylinder and a solid sphere of the same mass and radius. Which gains greater angular speed? The cylinder rotates about its symmetry axis; the sphere about a diameter.
Steps only
For the same torque, angular acceleration α=τ/I. The hollow cylinder has I=MR²; the solid sphere has I=2MR²/5.
Answer
The solid sphere gains greater angular speed.
Question 11
A 20 kg solid cylinder of radius 0.25 m spins at 100 rad/s. Find its rotational kinetic energy and angular momentum about its axis.
Steps only
For a solid cylinder, I=½MR²=½×20×0.25²=0.625 kg·m².
Answer
Rotational kinetic energy: 3125 J. Angular momentum: 62.5 kg·m²/s.
Question 12
A child spins on a frictionless turntable at 40 rev/min with arms out. Pulling the arms in reduces the child’s moment of inertia to 2/5 of its original value. (a) Find the new angular speed. (b) Why does rotational kinetic energy increase?
Steps only
With no external torque, angular momentum Iω is conserved. Therefore ωf=(Ii/If)ωi=(5/2)×40=100 rev/min.
Answer
(a) 100 rev/min. (b) Kinetic energy rises to 2.5 times its initial value because the child’s muscles do work.
Question 13
A 3 kg hollow cylinder of radius 0.40 m has a light rope wound around it. The rope is pulled with 30 N without slipping. Find the cylinder’s angular acceleration and the rope’s linear acceleration.
Steps only
For a hollow cylinder, I=MR²=3×0.40²=0.48 kg·m². The torque is τ=FR=30×0.40=12 N·m.
An engine applies torque 180 N·m to keep a rotor turning at 200 rad/s. Find the power required.
Steps only
Rotational power is P=τω.
Answer
36 kW.
Question 15
A uniform disk of radius R has a circular hole of radius R/2 removed. The hole’s centre is R/2 from the disk’s centre. Locate the centre of gravity of the remaining disk.
Steps only
Treat the removed hole as negative mass. If the complete disk has mass M, the hole has mass M/4. Put the original centre at x=0 and the hole centre at x=R/2.
Answer
The centre of gravity is R/6 from the original centre, on the side opposite the hole.
Question 16
A metre stick balances at its 50 cm mark. Two 5 g coins are placed at 12 cm, and the balance point moves to 45 cm. Find the stick’s mass.
Steps only
Take moments about the new balance point, 45 cm. The stick’s weight acts at 50 cm, 5 cm to the right; the 10 g of coins act 33 cm to the left.
Answer
66 g.
Question 17
An oxygen molecule has mass 5.30×10⁻²⁶ kg and moment of inertia 1.94×10⁻⁴⁶ kg·m². Its mean translational speed is 500 m/s. If rotational kinetic energy is 2/3 of translational kinetic energy, find its average angular speed.
Steps only
Translational energy is ½mv². Rotational energy is (2/3)(½mv²)=⅓mv², and it also equals ½Iω².