9709/43

Mathematics 9709/43October/November 2018

Cambridge A-Level · Mechanics · worked solutions for every part, with the mark scheme

7
questions
50
marks
75
minutes

Topics Kinematics of Motion in a Straight Line · Forces and Equilibrium · Energy, Work and Power · Newton's Laws of Motion

Q14MForces and EquilibriumFree sample

A small smooth ring RR of mass 0.2 kg0.2\text{ kg} is threaded onto a light inextensible string ARBARB. The two ends of the string are attached to points AA and BB on a sloping roof inclined at 4545^\circ to the horizontal. A horizontal force of magnitude P NP\text{ N}, acting in the plane ARBARB, is applied to the ring. The section BRBR of the string is perpendicular to the roof and the section ARAR of the string is inclined at 7070^\circ to the horizontal (see diagram). The system is in equilibrium. Find the tension in the string and the value of PP.

DifficultyMedium-Easy
Worked solution

Approach

The ring RR is in equilibrium under the action of three forces: its weight acting vertically downwards, the horizontal force PP acting to the left, and the tension TT in the string. Since the ring is smooth, the tension is uniform throughout the string ARBARB. We resolve the tension into its vertical and horizontal components using the given angles, then apply the equilibrium conditions (sum of vertical forces = 0, sum of horizontal forces = 0) to find TT and PP. We take g=10 m/s2g = 10 \text{ m/s}^2.

Working

The forces acting on the ring RR are:

  • Weight W=0.2g=0.2×10=2 NW = 0.2g = 0.2 \times 10 = 2 \text{ N} acting vertically downwards.
  • Horizontal force PP acting to the left.
  • Tension TT along RARA, inclined at 7070^\circ to the horizontal (pulling up and to the left).
  • Tension TT along RBRB. Since the roof is inclined at 4545^\circ to the horizontal and RBRB is perpendicular to the roof, RBRB is inclined at 4545^\circ to the horizontal (pulling up and to the right).

Resolving vertically (upwards positive):

The upward components of the tension balance the downward weight.

Tsin70+Tsin45=0.2gT(sin70+sin45)=2\begin{aligned} T \sin 70^\circ + T \sin 45^\circ &= 0.2g \\ T(\sin 70^\circ + \sin 45^\circ) &= 2 \end{aligned}

Substitute the values sin700.9397\sin 70^\circ \approx 0.9397 and sin450.7071\sin 45^\circ \approx 0.7071:

T(0.9397+0.7071)=2T(0.9397 + 0.7071) = 2 T(1.6468)=2T(1.6468) = 2 T=21.64681.214 NT = \frac{2}{1.6468} \approx 1.214 \text{ N}

Rounding to 3 significant figures:

T=1.21 NT = 1.21 \text{ N}

Resolving horizontally (rightwards positive):

The rightward component of the tension along RBRB balances the leftward force PP and the leftward component of the tension along RARA.

Tcos45=P+Tcos70T \cos 45^\circ = P + T \cos 70^\circ

Rearranging to solve for PP:

P=T(cos45cos70)P = T(\cos 45^\circ - \cos 70^\circ)

Substitute T=1.21447T = 1.21447 and the values cos450.7071\cos 45^\circ \approx 0.7071 and cos700.3420\cos 70^\circ \approx 0.3420:

P=1.21447(0.70710.3420)P = 1.21447(0.7071 - 0.3420) P=1.21447(0.3651)P = 1.21447(0.3651) P0.4434 NP \approx 0.4434 \text{ N}

Rounding to 3 significant figures:

P=0.443 NP = 0.443 \text{ N}

Answer

The tension in the string is 1.21 N1.21 \text{ N} and the value of PP is 0.443 N0.443 \text{ N}.

Final answer

T = 1.21 N, P = 0.443 N

Detailed explanation

Walkthrough

First, we identify all the forces acting on the ring RR. The ring has a mass of 0.2 kg0.2 \text{ kg}, so its weight is 0.2g0.2g acting vertically downwards. Using g=10 m/s2g = 10 \text{ m/s}^2, the weight is 2 N2 \text{ N}. A horizontal force PP acts to the left. The string ARBARB passes through the smooth ring, meaning the tension TT is the same in both sections ARAR and BRBR.

Next, we determine the directions of the tension forces. Section ARAR is given as inclined at 7070^\circ to the horizontal. From the diagram, AA is above and to the left of RR, so the tension along ARAR pulls the ring up and to the left at 7070^\circ to the horizontal. Section BRBR is perpendicular to the roof. The roof is inclined at 4545^\circ to the horizontal. A line perpendicular to a 4545^\circ slope is at 4545^\circ to the horizontal. From the diagram, BB is above and to the right of RR, so the tension along BRBR pulls the ring up and to the right at 4545^\circ to the horizontal.

To find the tension TT, we resolve forces vertically. The upward vertical components of the two tension forces must balance the downward weight. This gives the equation Tsin70+Tsin45=0.2gT \sin 70^\circ + T \sin 45^\circ = 0.2g. Substituting g=10g = 10 and solving for TT yields T1.21 NT \approx 1.21 \text{ N}.

To find PP, we resolve forces horizontally. The rightward horizontal component of the tension along BRBR must balance the leftward force PP and the leftward horizontal component of the tension along ARAR. This gives the equation Tcos45=P+Tcos70T \cos 45^\circ = P + T \cos 70^\circ. Rearranging for PP and substituting the value of TT yields P0.443 NP \approx 0.443 \text{ N}.

Key Takeaways

  • In equilibrium problems involving a smooth ring on a string, the tension is uniform throughout the string.
  • Forces can be resolved into perpendicular components (usually horizontal and vertical) to apply the equilibrium condition F=0\sum F = 0.
  • Geometrical relationships (like a line being perpendicular to a slope) must be used to correctly determine the angles of the forces.

Common Mistakes

  • Forgetting that the tension is the same in both sections of the string because the ring is smooth.
  • Incorrectly determining the angle of BRBR with the horizontal; it is 4545^\circ, not 9090^\circ or 4545^\circ to the vertical (though 4545^\circ to the vertical is the same as 4545^\circ to the horizontal, care must be taken with the components).
  • Sign errors when resolving horizontally; ensuring that leftward and rightward forces are correctly assigned.
  • Using g=9.8g = 9.8 or g=9.81g = 9.81 instead of g=10g = 10, which is standard for this syllabus unless specified otherwise (the mark scheme values confirm g=10g=10 is used here).

Things to Be Careful About

  • Always check the direction of the forces to ensure correct signs in the resolution equations.
  • The angle 7070^\circ is given to the horizontal, so the vertical component uses sin70\sin 70^\circ and the horizontal component uses cos70\cos 70^\circ.
  • Ensure the final answers are given to an appropriate number of significant figures (3 s.f. is standard).
  • Verify that the geometry makes sense: the sum of the upward vertical components must equal the weight, and the sum of the leftward horizontal components must equal the sum of the rightward horizontal components.
Techniques used
identify forces on the ringresolve forces verticallyresolve forces horizontallyuse uniform tension in a smooth string

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