CAIE A-Level Further Math 3.3 Circular motion Question Bank
Practise circular motion by resolving forces, using v = rω and applying energy to particles in horizontal and vertical circles.
- Syllabus
- 2028–2030
- Course
- Further Mathematics 9231
- Level
- AS
Practise circular motion by resolving forces, using v = rω and applying energy to particles in horizontal and vertical circles.
A particle P of mass m is attached to one end of a light inextensible rod of length 3 a. An identical particle Q is attached to the other end of the rod. The rod is smoothly pivoted at a point O on the rod, where O Q=x. The system, of rod and particles, rotates about O in a vertical plane.
At an instant when the rod is vertical, with P above Q, the particle P is moving horizontally with speed u. When the rod has turned through an angle of 60∘ from the vertical, the speed of P is 2ag, and the tensions in the two parts of the rod, OP and OQ, have equal magnitudes.
Show that the speed of Q when the rod has turned through an angle of 60∘ from the vertical is
Angular speeds of P and Q are equal,
so xνQ=3a−xνP
M1
vQ=3a−x2xag
A1
Shown convincingly: angular speeds equal stated.
AG
2
Find x in terms of a.
For P:T+mgcos60∘=3a−xm×4ag
B1
For Q:T−mgcos60∘=xmvQ2
B1
Eliminate T:−mgcos60∘+3a−xm⋅4ag=mgcos60∘+xmvQ2
M1
3a−xm×4ag=1+(3a−x)2mx4ag4a(3a−x)=(3a−x)2+4ax,x2+2ax−3a2=0
M1
Solve to find x.
Obtain 3-term quadratic equation.
(x−a)(x+3a)=0,x=a
A1
5
Find u in terms of a and g.
Additional page
If you use the following page to complete the answer to any question, the question number must be clearly shown.
B1
KEs correct.
Energy changes from initial position:
Gain in KE of P:21m(4ag−u2)
Loss in KE of Q:21m((2u)2−vQ2)
Loss in GPE of P=mg(3a−x)(1−cos60∘)(=mga)
Gain in GPE of Q=mgx(1−cos60∘)(=21mga)
B1FT
GPEs correct.
21m(4ag−u2)−21m((2u)2−vQ2)=−mgx(1−cos60∘)+mg(3a−x)(1−cos60∘)
M1
Energy equation.
Simplify: 4ag−45u2+ag=agu2=516ag,u=545ag
A1
AEF
4
One end of a light inextensible string of length a is attached to a fixed point O. The other end of the string is attached to a particle of mass m. The string is taut and makes an angle θ with the downward vertical through O, where cosθ=32. The particle moves in a horizontal circle with speed v.
Find v in terms of a and g.
↑Tcosθ=mg
B1
→Tsinθ=asinθmv2
B1
Eliminate T and substitute for θ
M1
v=65ag
A1
4