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#### Page No 242:

#### Question 9.1:

A
steel wire of length 4.7 m and cross-sectional area 3.0 × 10^{–5}
m^{2}
stretches by the same amount as a copper wire of length 3.5 m and
cross-sectional area of 4.0 × 10^{–5}
m^{2}
under a given load. What is the ratio of the Young’s modulus of
steel to that of copper?

#### Answer:

Length of the steel
wire, *L*_{1} = 4.7 m

Area of cross-section
of the steel wire, *A*_{1} = 3.0 × 10^{–5}
m^{2}

Length of the copper
wire, *L*_{2} = 3.5 m

Area of cross-section
of the copper wire, *A*_{2} = 4.0 × 10^{–5}
m^{2}

Change in length = Δ*L*_{1}
= Δ*L*_{2} = Δ*L*

Force applied in both
the cases = *F*

Young’s modulus of the steel wire:

_{
} … (*i*)

Young’s modulus of the copper wire:

Dividing (*i*) by
(*ii*), we get:

The ratio of Young’s modulus of steel to that of copper is 1.79 : 1.

#### Page No 242:

#### Question 9.2:

Figure 9.11 shows the strain-stress curve for a given material. What are (a) Young’s modulus and (b) approximate yield strength for this material?

#### Answer:

**(a)** It is clear from the given graph that for stress 150 ×
10^{6} N/m^{2}, strain is 0.002.

∴Young’s modulus, *Y*

Hence, Young’s modulus for the given material is 7.5 ×10^{10}
N/m^{2}.

**(b)** The yield strength of a material is the maximum stress
that the material can sustain without crossing the elastic limit.

It is clear from the given graph that the approximate yield strength
of this material is 300 × 10^{6} Nm/^{2} or 3 ×
10^{8} N/m^{2}.

#### Page No 243:

#### Question 9.3:

The stress-strain graphs for materials **A** and **B **are shown in Fig. 9.12.

The graphs are drawn to the same scale.

(a) Which of the materials has the greater Young’s modulus?

(b) Which of the two is the stronger material?

#### Answer:

**Answer: (a) A**
**(b) A**

**(a)** For a given strain, the stress for material **A** is
more than it is for material **B**, as shown in the two graphs.

Young’s modulus

For
a given strain, if the stress for a material is more, then Young’s
modulus is also greater for that material. Therefore, Young’s
modulus for material **A** is greater than it is for material **B**.

**(b)** The amount of stress required for fracturing a material,
corresponding to its fracture point, gives the strength of that
material. Fracture point is the extreme point in a stress-strain
curve. It can be observed that material **A** can withstand more
strain than material **B**. Hence, material **A** is stronger
than material **B**.

#### Page No 243:

#### Question 9.4:

Read the following two statements below carefully and state, with reasons, if it is true or false.

**(a)** The
Young’s modulus of rubber is greater than that of steel;

**(b)** The
stretching of a coil is determined by its shear modulus.

#### Answer:

**Answer: (a) **False
**(b) **True

**(a)** For a given
stress, the strain in rubber is more than it is in steel.

Young’s modulus,

For a constant stress:

Hence, Young’s modulus for rubber is less than it is for steel.

**(b) **Shear modulus is the ratio of the applied stress to the
change in the shape of a body. The stretching of a coil changes its
shape. Hence, shear modulus of elasticity is involved in this
process.

#### Page No 243:

#### Question 9.5:

Two wires of diameter 0.25 cm, one made of steel and the other made of brass are loaded as shown in Fig. 9.13. The unloaded length of steel wire is 1.5 m and that of brass wire is 1.0 m. Compute the elongations of the steel and the brass wires.

#### Answer:

Elongation of the steel
wire = 1.49 × 10^{–4} m

Elongation of the brass
wire = 1.3 × 10^{–4} m

Diameter of the wires,
*d* = 0.25 m

Hence, the radius of the wires, = 0.125 cm

Length of the steel
wire, *L*_{1} = 1.5 m

Length of the brass
wire, *L*_{2} = 1.0 m

Total force exerted on the steel wire:

*F*_{1} =
(4 + 6) g = 10 × 9.8 = 98 N

Young’s modulus for steel:

Where,

Δ*L*_{1}
= Change in the length of the steel wire

*A*_{1} =
Area of cross-section of the steel wire

Young’s modulus
of steel, *Y*_{1} = 2.0 × 10^{11} Pa

Total force on the brass wire:

*F*_{2} =
6 × 9.8 = 58.8 N

Young’s modulus for brass:

Elongation of the steel
wire = 1.49 × 10^{–4} m

Elongation of the brass
wire = 1.3 × 10^{–4} m

#### Page No 244:

#### Question 9.6:

The edge of an aluminium cube is 10 cm long. One face of the cube is firmly fixed to a vertical wall. A mass of 100 kg is then attached to the opposite face of the cube. The shear modulus of aluminium is 25 GPa. What is the vertical deflection of this face?

#### Answer:

Edge of the aluminium cube, *L* = 10 cm = 0.1 m

The mass attached to the cube, *m* = 100 kg

Shear modulus (η) of
aluminium = 25 GPa = 25 × 10^{9} Pa

Shear modulus, η

Where,

*F* = Applied force = *m*g = 100 × 9.8 = 980 N

*A* = Area of one of the faces of the cube = 0.1 × 0.1
= 0.01 m^{2}

Δ*L* = Vertical deflection of the cube

= 3.92 × 10^{–7} m

The vertical deflection of this face of the cube is 3.92 ×10^{–7}
m.

#### Page No 244:

#### Question 9.7:

Four identical hollow cylindrical columns of mild steel support a big structure of mass 50,000 kg. The inner and outer radii of each column are 30 cm and 60 cm respectively. Assuming the load distribution to be uniform, calculate the compressional strain of each column.

#### Answer:

Mass of the big
structure, *M *= 50,000 kg

Inner radius of the
column, *r* = 30 cm = 0.3 m

Outer radius of the
column, *R* = 60 cm = 0.6 m

Young’s modulus
of steel, *Y* = 2 × 10^{11} Pa

Total force exerted, *F*
= *M*g = 50000 × 9.8 N

Stress = Force exerted on a single column = 122500 N

Young’s modulus,
*Y*

Where,

Area, *A* = π
(*R*^{2} – *r*^{2}) = π
((0.6)^{2} – (0.3)^{2})

= 7.22 × 10^{–7}

Hence, the
compressional strain of each column is 7.22 × 10^{–7}.

#### Page No 244:

#### Question 9.8:

A piece of copper having a rectangular cross-section of 15.2 mm × 19.1 mm is pulled in tension with 44,500 N force, producing only elastic deformation. Calculate the resulting strain?

#### Answer:

Length of the piece of copper, *l* = 19.1 mm = 19.1 ×
10^{–3} m

Breadth of the piece of copper, *b* = 15.2 mm = 15.2 ×
10^{–3} m

Area of the copper piece:

A = *l × b*

= 19.1 × 10^{–3} × 15.2 × 10^{–3}

= 2.9 × 10^{–4} m^{2}

Tension force applied on the piece of copper, *F* = 44500 N

Modulus of elasticity of copper, η
= 42 × 10^{9} N/m^{2}

Modulus of elasticity, η

= 3.65 × 10^{–3}

#### Page No 244:

#### Question 9.9:

A
steel cable with a radius of 1.5 cm supports a chairlift at a ski
area. If the maximum stress is not to exceed 10^{8
}N m^{–2},
what is the maximum load the cable can support?

#### Answer:

Radius of the steel
cable, *r* = 1.5 cm = 0.015 m

Maximum allowable
stress = 10^{8} N m^{–2}

Maximum stress =

∴Maximum force = Maximum stress × Area of cross-section

= 10^{8} × π
(0.015)^{2}

= 7.065 × 10^{4} N

Hence, the cable can
support the maximum load of 7.065 × 10^{4} N.

#### Page No 244:

#### Question 9.10:

A rigid bar of mass 15 kg is supported symmetrically by three wires each 2.0 m long. Those at each end are of copper and the middle one is of iron. Determine the ratio of their diameters if each is to have the same tension.

#### Answer:

The tension force acting on each wire is the same. Thus, the extension in each case is the same. Since the wires are of the same length, the strain will also be the same.

The relation for Young’s modulus is given as:

Where,

*F* = Tension force

*A* = Area of cross-section

*d *= Diameter of the wire

It can be inferred from equation (*i*) that

Young’s modulus for iron, *Y*_{1} = 190 × 10^{9} Pa

Diameter of the iron wire = *d*_{1}

Young’s modulus for copper, *Y*_{2 }= 120 × 10^{9} Pa

Diameter of the copper wire = *d*_{2}

Therefore, the ratio of their diameters is given as:

#### Page No 244:

#### Question 9.11:

A 14.5 kg mass, fastened to the end of a steel wire of unstretched length 1.0 m, is whirled in a vertical circle with an angular velocity of 2 rev/s at the bottom of the circle. The cross-sectional area of the wire is 0.065 cm^{2}. Calculate the elongation of the wire when the mass is at the lowest point of its path.

#### Answer:

Mass, *m* = 14.5 kg

Length of the steel wire, *l* = 1.0 m

Angular velocity, *ω* = 2 rev/s = 2 × 2π rad/s = 12.56 rad/s

Cross-sectional area of the wire, *a* = 0.065 cm^{2} = 0.065 × 10^{-4} m^{2}

Let Δ*l* be the elongation of the wire when the mass is at the lowest point of its path.

When the mass is placed at the position of the vertical circle, the total force on the mass is:

*F* = *m*g + *mlω*^{2}

= 14.5 × 9.8 + 14.5 × 1 × (12.56)^{2}

= 2429.53 N

Young’s modulus for steel = 2 × 10^{11} Pa

Hence, the elongation of the wire is 1.87 × 10^{–3} m.

#### Page No 244:

#### Question 9.12:

Compute the bulk modulus of water from the following data: Initial volume = 100.0 litre, Pressure increase = 100.0 atm (1 atm = 1.013 × 10^{5} Pa), Final volume = 100.5 litre. Compare the bulk modulus of water with that of air (at constant temperature). Explain in simple terms why the ratio is so large.

#### Answer:

Initial volume, *V*_{1 }= 100.0l = 100.0 × 10^{ –3} m^{3}

Final volume, *V*_{2 }= 100.5 l = 100.5 ×10^{ –3} m^{3}

Increase in volume, Δ*V* = *V*_{2} – *V*_{1 }= 0.5 × 10^{–3} m^{3}

Increase in pressure, Δ*p* = 100.0 atm = 100 × 1.013 × 10^{5} Pa

This ratio is very high because air is more compressible than water.

#### Page No 244:

#### Question 9.13:

What
is the density of water at a depth where pressure is 80.0 atm, given
that its density at the surface is 1.03 × 10^{3}
kg m^{–3}?

#### Answer:

Let the given depth be *h*.

Pressure at the given depth,* p* = 80.0 atm = 80 × 1.01 × 10^{5} Pa

Density of water at the surface, *ρ*_{1 }= 1.03 × 10^{3} kg m^{–3}

Let *ρ*_{2} be the density of water at the depth *h*.

Let *V*_{1} be the volume of water of mass *m* at the surface.

Let *V*_{2} be the volume of water of mass *m* at the depth *h*.

Let Δ*V* be the change in volume.

For equations (*i*) and (*ii*), we get:

Therefore, the density of water at the given depth (*h*) is 1.034 × 10^{3} kg m^{–3}.

#### Page No 244:

#### Question 9.14:

Compute the fractional change in volume of a glass slab, when subjected to a hydraulic pressure of 10 atm.

#### Answer:

Hydraulic pressure
exerted on the glass slab, *p *= 10 atm = 10 × 1.013 ×
10^{5} Pa

Bulk modulus of glass,
*B* = 37 × 10^{9} Nm^{–2}

Where,

= Fractional change in volume

Hence, the fractional
change in the volume of the glass slab is 2.73 × 10^{–5}.

#### Page No 244:

#### Question 9.15:

Determine
the volume contraction of a solid copper cube, 10 cm on an edge, when
subjected to a hydraulic pressure of 7.0 ×10^{6}
Pa.

#### Answer:

Length of an edge of the solid copper cube, *l* = 10 cm = 0.1 m

Hydraulic pressure, *p* = 7.0 ×10^{6} Pa

Bulk modulus of copper, *B* = 140 × 10^{9} Pa

Where,

= Volumetric strain

Δ*V* = Change in volume

*V* = Original volume.

Original volume of the cube, *V* = *l*^{3}

Therefore, the volume contraction of the solid copper cube is 5 × 10^{–2} cm^{–3}.

#### Page No 244:

#### Question 9.16:

How much should the pressure on a litre of water be changed to compress it by 0.10%?

#### Answer:

Volume of water, *V *= 1 L

It is given that water is to be compressed by 0.10%.

Therefore, the pressure on water should be 2.2 ×10^{6} Nm^{–2}.

#### Page No 244:

#### Question 9.17:

Anvils made of single crystals of diamond, with the shape as shown in Fig. 9.14, are used to investigate behaviour of materials under very high pressures. Flat faces at the narrow end of the anvil have a diameter of 0.50 mm, and the wide ends are subjected to a compressional force of 50,000 N. What is the pressure at the tip of the anvil?

#### Answer:

Diameter of the cones
at the narrow ends, *d* = 0.50 mm = 0.5 × 10^{–3}
m

Compressional force,*
F* = 50000 N

Pressure at the tip of the anvil:

Therefore, the pressure
at the tip of the anvil is 2.55 × 10^{11} Pa.

#### Page No 245:

#### Question 9.18:

A
rod of length 1.05 m having negligible mass is supported at its ends
by two wires of steel (wire **A**)
and aluminium (wire **B**)
of equal lengths as shown in Fig. 9.15. The cross-sectional areas of
wires **A**
and **B**
are 1.0 mm^{2}
and 2.0 mm^{2},
respectively. At what point along the rod should a mass *m
*be suspended in order to produce (a)
equal stresses and (b) equal strains in both steel and aluminium
wires.

#### Answer:

**Answer: (a)** 0.7
m from the steel-wire end

**(b)** 0.432
m from the steel-wire end

Cross-sectional area of wire **A**, *a*_{1} = 1.0 mm^{2
}= 1.0 × 10^{–6} m^{2}

Cross-sectional area of wire **B**, *a*_{2} = 2.0 mm^{2
}= 2.0 × 10^{–6} m^{2}

Young’s modulus for steel, *Y*_{1} = 2 ×
10^{11 }Nm^{–2}

Young’s modulus for aluminium, *Y*_{2} = 7.0 ×10^{10
}Nm^{–2}

**(a) **Let a small mass *m* be suspended to the rod at a
distance *y* from the end where wire **A** is attached.

If the two wires have equal stresses, then:

Where,

*F*_{1}
= Force exerted on the steel wire

*F*_{2}
= Force exerted on the aluminum wire

The situation is shown in the following figure.

Taking torque about the point of suspension, we have:

Using
equations (*i*) and (*ii*), we can write:

In
order to produce an equal stress in the two wires, the mass should be
suspended at a distance of 0.7 m from the end where wire **A** is
attached.

**(b)**

If the strain in the two wires is equal, then:

Taking
torque about the point where mass *m*, is suspended at a
distance *y*_{1} from the side where wire **A**
attached, we get:

*F*_{1}*y*_{1
}= *F*_{2} (1.05 – *y*_{1})

…
(*iii*)

Using
equations (*iii*) and (*iv*), we get:

In
order to produce an equal strain in the two wires, the mass should be
suspended at a distance of 0.432 m from the end where wire **A**
is attached.

#### Page No 245:

#### Question 9.19:

A mild steel wire of length 1.0 m and cross-sectional area
0.50 × 10^{–2} cm^{2 }is stretched,
well within its elastic limit, horizontally between two
pillars. A mass of 100 g is suspended from the mid-point of the wire.
Calculate the depression at the midpoint.

#### Answer:

Length of the steel wire = 1.0 m

Area of cross-section, *A* = 0.50 × 10^{–2} cm^{2 }= 0.50 × 10^{–6} m^{2}

A mass 100 g is suspended from its midpoint.

*m* = 100 g = 0.1 kg

Hence, the wire dips, as shown in the given figure.

Original length = XZ

Depression = *l*

The length after mass *m*, is attached to the wire = XO + OZ

Increase in the length of the wire:

Δ*l *= (XO + OZ) – XZ

Where,

XO = OZ =

Let *T* be the tension in the wire.

∴*m*g = 2*T* cos*θ*

Using the figure, it can be written as:

Expanding the expression and eliminating the higher terms:

Young’s modulus of steel, *Y* =

Hence, the depression at the midpoint is 0.0106 m.

#### Page No 245:

#### Question 9.20:

Two strips of metal are riveted together
at their ends by four rivets, each of diameter 6.0 mm. What is the
maximum tension that can be exerted by the riveted strip if the
shearing stress on the rivet is not to exceed 6.9 × 10^{7}
Pa? Assume that each rivet is to carry one
quarter of the load.

#### Answer:

Diameter of the metal
strip, *d* = 6.0 mm = 6.0 × 10^{–3} m

Maximum shearing stress
= 6.9 × 10^{7} Pa

Maximum force = Maximum stress × Area

=
6.9 × 10^{7} × π
× (*r*)^{ 2}

=
6.9 × 10^{7} × π
× (3 ×10^{–3})^{2}

= 1949.94 N

Each rivet carries one quarter of the load.

∴ Maximum tension on each rivet = 4 × 1949.94 = 7799.76 N

#### Page No 245:

#### Question 9.21:

The
Marina trench is located in the Pacific Ocean, and at one place it is
nearly eleven km beneath the surface of water. The water pressure at
the bottom of the trench is about 1.1 × 10^{8}
Pa. A steel ball of initial volume 0.32 m^{3}
is dropped into the ocean and
falls to the bottom of the trench. What is the change in the volume
of the ball when it reaches to the bottom?

#### Answer:

Water pressure at the bottom, *p *= 1.1 × 10^{8} Pa

Initial volume of the steel ball, *V* = 0.32 m^{3}

Bulk modulus of steel, *B* = 1.6 × 10^{11 }Nm^{–2}

The ball falls at the bottom of the Pacific Ocean, which is 11 km beneath the surface.

Let the change in the volume of the ball on reaching the bottom of the trench be Δ*V*.

Therefore, the change in volume of the ball on reaching the bottom of the trench is 2.2 × 10^{–4} m^{3}.

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