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Equilibrium in 2D Simplified Revision Notes

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3.1.3 Equilibrium in 2D

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To approach equilibrium questions in 2D Mechanics, follow these key steps:

  1. Identify all forces: List all the forces acting on the object, including weight, tension, normal reaction, and friction.
  2. Resolve forces into components: Split each force into horizontal and vertical components, typically using trigonometry (sine and cosine functions for angled forces).
  3. Apply equilibrium conditions: For an object in equilibrium, the sum of forces in both directions must equal zero:
  • Fx=0\sum F_x = 0 (sum of horizontal forces)
  • Fy=0\sum F_y = 0 (sum of vertical forces)
  1. Solve the system of equations: Use the two equations to find unknown forces or angles. This method ensures that all forces balance, confirming that the object is in equilibrium.

Static Bodies in 2D

Concept:

  • A static body is an object that lies in equilibrium. In this scenario, all forces attached to the object sum to zero.
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Example:

  • Consider a scenario where a single piece of string is threaded through a particle, with the string being light and inextensible. The particle is held in equilibrium by two strings forming angles of 3030^\circ with the horizontal. Problem:

  • Given that the weight of the particle is 22g, find the tension TT in the strings. Solution:

  1. Resolve Forces in a Relevant Direction:
  • Consider the vertical direction for resolving forces.
  1. Vertical Forces:
Tsin30+Tsin302g=0T \sin 30^\circ + T \sin 30^\circ - 2g = 0
  • Since sin30=12\sin 30^\circ = \frac{1}{2}, the equation simplifies to:
2T122g=02T \cdot \frac{1}{2} - 2g = 0T2g=0T=2gNT - 2g = 0 \quad \Rightarrow \quad T = 2g \, \text{N}

Final Answer:

  • The tension in each string is T=2gNT = 2g \, \text{N}.

Mechanics Problems in 3D

Key Concept:

  • All mechanical concepts (equilibrium, F=maF = ma, SUVAT, etc.) apply in 3D as well as in 2D.

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Q1, (Jan 2005, Q3)

Problem Statement: A particle is in equilibrium when acted on by the forces(x7z),(4y5),and(547) \left(\begin{array}{c} x \\ -7 \\ z \end{array}\right), \left(\begin{array}{c} 4 \\ y \\ -5 \end{array}\right), and \left(\begin{array}{c} 5 \\ 4 \\ -7 \end{array}\right), where the units are Newtons.

  1. Find the values of xx, yy, and z.z.
  2. Calculate the magnitude of (547)\left(\begin{array}{c} 5 \\ 4 \\ -7 \end{array}\right).

Solution:

Part (i): Finding the Values of xx, yy, and zz

  1. Condition for Equilibrium:
  • Since the particle is in equilibrium, the sum of all forces must be zero:
(x7z)+(4y5)+(547)=(000)\left(\begin{array}{c} x \\ -7 \\ z \end{array}\right) + \left(\begin{array}{c} 4 \\ y \\ -5 \end{array}\right) + \left(\begin{array}{c} 5 \\ 4 \\ -7 \end{array}\right) = \left(\begin{array}{c} 0 \\ 0 \\ 0 \end{array}\right)
  1. Solve for xx, yy, and zz:
  • Equating the components:
x+4+5=0x=9x + 4 + 5 = 0 \quad \Rightarrow \quad x = -9 7+y+4=0y=3-7 + y + 4 = 0 \quad \Rightarrow \quad y = 3 z57=0z=12z - 5 - 7 = 0 \quad \Rightarrow \quad z = 12

Answer (i): x=9,y=3,z=12x = -9, y = 3, z = 12


Part (ii): Calculating the Magnitude

  1. Calculate the magnitude of (547)\left(\begin{array}{c} 5 \\ 4 \\ -7 \end{array}\right):
a=52+42+(7)2=25+16+49=90=310|\mathbf{a}| = \sqrt{5^2 + 4^2 + (-7)^2} = \sqrt{25 + 16 + 49} = \sqrt{90} = 3\sqrt{10}

Answer (ii): The magnitude is 3103\sqrt{10}.


Problem: Finding the Tension in the String and the Weight of the Bead

image
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Problem Statement:

  • A smooth bead Y is threaded on a light inextensible string.

  • The string is attached to two fixed points, XX and ZZ, which are on the same horizontal level.

  • The bead is in equilibrium, held by a horizontal force of magnitude 8N8 \, \text{N} acting parallel to ZXZX.

  • The bead YYis vertically below XX, and \angle XZY=30\angle XZY = 30^\circ. Find:

  • The tension in the string TT.

  • The weight of the bead WW.

Solution:

  1. Tension TT in the String:
  • Since the bead is in equilibrium and the string is inextensible, the tension is the same throughout the string.
  • Resolve forces horizontally:
Tcos30=8NT \cos 30^\circ = 8 \, \text{N} T=8cos30=832=163N1633NT = \frac{8}{\cos 30^\circ} = \frac{8}{\frac{\sqrt{3}}{2}} = \frac{16}{\sqrt{3}} \, \text{N} \approx \frac{16\sqrt{3}}{3} \, \text{N}
  1. Weight WW of the Bead:
  • Resolve forces vertically:
Tsin30+Tsin30=WT \sin 30^\circ + T \sin 30^\circ = W W=2×Tsin30W = 2 \times T \sin 30^\circ W=2×1633×12=1633sin30=83NW = 2 \times \frac{16\sqrt{3}}{3} \times \frac{1}{2} = \frac{16\sqrt{3}}{3} \, \sin30 ^\circ = \boxed {8\sqrt 3N}

Answer:

  • Tension T1633NT \approx \frac{16\sqrt{3}}{3} \, \text{N}
  • Weight W83NW \approx 8\sqrt{3} \, \text{N}

Problem: Tension in the String and Weight of the Bead

image
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Problem Statement:

  • A smooth bead YY is threaded on a light inextensible string. The ends of the string are attached to two fixed points, XX and ZZ, on the same horizontal level.

  • The bead is in equilibrium under a horizontal force of magnitude 8N8 \, \text{N} acting parallel to ZXZX.

  • The bead YY is vertically below XX, and ZXY=30\angle ZXY = 30^\circ. Objective:

  • Find the tension T T in the string.

  • Find the weight WW of the bead.


Solution:

  1. Resolving Forces Horizontally:
  • The horizontal component of the tension TT must balance the horizontal force:
8Tcos30=08 - T \cos 30^\circ = 0 Tcos30=8T \cos 30^\circ = 8 T=8cos30=832=1633NT = \frac{8}{\cos 30^\circ} = \frac{8}{\frac{\sqrt{3}}{2}} = \frac{16\sqrt{3}}{3} \, \text{N}
  1. Resolving Forces Vertically:
  • The vertical components of the tension TT must balance the weight WW:
Tsin30+Tcos60W=0T \sin 30^\circ + T \cos 60^\circ - W = 0
  • Substituting sin30=12\sin 30^\circ = \frac{1}{2} and cos60=12\cos 60^\circ = \frac{1}{2}:
T×12+T×12=WT \times \frac{1}{2} + T \times \frac{1}{2} = W W=1.5T2=Tsin30+Tcos60W = \frac{1.5T}{2} = T \sin 30^\circ + T \cos 60^\circ W=1633×32=83NW = \frac{16\sqrt{3}}{3} \times \frac{3}{2} = 8\sqrt{3} \, \text{N}

Final Answer:

  • Tension in the string TT is 1633N\frac{16\sqrt{3}}{3} \, \text{N}.
  • Weight of the bead WW is 83N8\sqrt{3} \, \text{N}.

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