Home
Class 11
PHYSICS
Steel wire of length 'L' at 40^@C is sus...

Steel wire of length 'L' at `40^@C` is suspended from the ceiling and then a mass 'm' is hung from its free end. The wire is cooled down from `40^@C to 30^@C` to regain its original length 'L'. The coefficient of linear thermal expansion of the steel is `10^-5//^@C`, Young's modulus of steel is `10^11 N//m^2` and radius of the wire is 1mm. Assume that `L gt gt` diameter of the wire. Then the value of 'm' in kg is nearly

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem step by step, we will use the concepts of Young's modulus, thermal expansion, and the relationship between stress, strain, and force. ### Step 1: Understand the Problem We have a steel wire of length \( L \) at \( 40^\circ C \) that is cooled to \( 30^\circ C \). We need to find the mass \( m \) that is hung from the wire to bring it back to its original length \( L \). ### Step 2: Identify Given Values - Coefficient of linear thermal expansion \( \alpha = 10^{-5} \, ^\circ C^{-1} \) - Young's modulus \( Y = 10^{11} \, N/m^2 \) - Radius of the wire \( r = 1 \, mm = 1 \times 10^{-3} \, m \) - Change in temperature \( \Delta T = 40^\circ C - 30^\circ C = 10^\circ C \) ### Step 3: Calculate the Change in Length Due to Temperature The change in length \( \Delta L \) due to thermal expansion can be calculated using the formula: \[ \Delta L = L \alpha \Delta T \] Substituting the values: \[ \Delta L = L \cdot (10^{-5}) \cdot (10) = L \cdot 10^{-4} \] ### Step 4: Relate Stress and Strain Young's modulus is defined as: \[ Y = \frac{\text{Stress}}{\text{Strain}} \] Where: - Stress \( = \frac{F}{A} = \frac{mg}{A} \) - Strain \( = \frac{\Delta L}{L} \) Thus, we can write: \[ Y = \frac{mg/A}{\Delta L/L} \] Rearranging gives: \[ Y = \frac{mgL}{A \Delta L} \] ### Step 5: Substitute \( \Delta L \) Substituting \( \Delta L = L \cdot 10^{-4} \) into the equation: \[ Y = \frac{mgL}{A (L \cdot 10^{-4})} \] This simplifies to: \[ Y = \frac{mg}{A \cdot 10^{-4}} \] ### Step 6: Solve for Mass \( m \) Rearranging for \( m \): \[ m = \frac{Y \cdot A \cdot 10^{-4}}{g} \] ### Step 7: Calculate the Area \( A \) The area \( A \) of the wire can be calculated as: \[ A = \pi r^2 = \pi (1 \times 10^{-3})^2 = \pi \times 10^{-6} \, m^2 \] ### Step 8: Substitute Values Now substituting \( Y \), \( A \), and \( g \): \[ m = \frac{(10^{11}) \cdot (\pi \times 10^{-6}) \cdot (10^{-4})}{10} \] This simplifies to: \[ m = \frac{10^{11} \cdot \pi \cdot 10^{-10}}{10} = \frac{\pi \cdot 10^{1}}{10} = \pi \] ### Step 9: Approximate the Value of \( \pi \) Using \( \pi \approx 3.14 \): \[ m \approx 3.14 \, kg \] ### Conclusion Thus, the mass \( m \) that needs to be hung from the wire is nearly \( 3 \, kg \).

To solve the problem step by step, we will use the concepts of Young's modulus, thermal expansion, and the relationship between stress, strain, and force. ### Step 1: Understand the Problem We have a steel wire of length \( L \) at \( 40^\circ C \) that is cooled to \( 30^\circ C \). We need to find the mass \( m \) that is hung from the wire to bring it back to its original length \( L \). ### Step 2: Identify Given Values - Coefficient of linear thermal expansion \( \alpha = 10^{-5} \, ^\circ C^{-1} \) - Young's modulus \( Y = 10^{11} \, N/m^2 \) ...
Promotional Banner

Topper's Solved these Questions

  • CALORIMETRY AND THERMAL EXPANSION

    RESONANCE ENGLISH|Exercise Advanced Level Problems|13 Videos
  • CALORIMETRY AND THERMAL EXPANSION

    RESONANCE ENGLISH|Exercise Exercie-3|1 Videos
  • CALORIMETRY

    RESONANCE ENGLISH|Exercise Exercise|19 Videos
  • CAPACITOR

    RESONANCE ENGLISH|Exercise Exercise|45 Videos

Similar Questions

Explore conceptually related problems

A steel wire 2 m long is suspended from the ceiling. When a mass is hung from its lower end, the increase in length recorded is 1 cm . Determine the strain in the wire.

A steel wire of length 20 cm and uniform cross-section 1mm^(2) is tied rigidly at both the ends. If the temperature of the wire is altered from 40^(@)C to 20^(@)C , the change in tension. [Given coefficient of linear expansion of steel is 1.1xx10^(5) .^(@)C^(-1) and Young's modulus for steel is 2.0xx10^(11) Nm^(-2) ]

At 40^(@)C a brass wire of 1mm radius is hung from the ceiling. A small mass, M is hung from the free end of the wire. When the wire is cooled down from 40^(@)C to 20^(@)C it regains its original length of 0.2 m the value of M is close to (coefficient of linear expansion and young's modulus of brass are 10^(-5)//.^(@)C and 10^(11)//N//m^(2) respectively g=10ms^(-2))

A steel wire of length 20 cm and uniform cross section 1 mm^(2) is tied rigidly at both the ends. The temperature of the wire is altered from 40^(@) C to 20^(@)C Coefficient of linear expansion for steel alpha = 1.1 xx 10^(-5) l^(@)C and Y for steel is 2.0 xx 10^(11) N//m^(2) . The change in tension of the wire is

A steel rod of length 1 m is heated from 25^@ "to" 75^@ C keeping its length constant. The longitudinal strain developed in the rod is ( Given, coefficient of linear expansion of steel = 12 xx 10^-6//^@ C ).

The area of a cross-section of steel wire is 0.1 cm^(-2) and Young's modulus of steel is 2 x 10^(11) N m^(-2) . The force required to stretch by 0.1% of its length is

A metal wire of length L is suspended vertically from a rigid support. When a bob of mass M is attached to the lower end of wire, the elongation of the wire is l:

A wire of length L_0 is supplied heat to raise its temperature by T. if gamma is the coefficient of volume expansion of the wire and Y is Young's modulus of the wire then the energy density stored in the wire is

A steel wire 4.0m in length is stretched through 2.0mm .The cross -sectional area of the wire is 2.0 mm^(2) .If young's modulus of steel is 2.0xx10^(11) N//m^(2) (a) the energy density of wire, (b) the elastic potential energy stored in the wire.

A steel wire of cross-sectional area 0.5mm^2 is held between two fixed supports. If the wire is just taut at 20^@C , determine the tension when the temperature falls to 0^@C . Coefficient of linear expansion of steel is 1.2 xx 10^(-5 @)C(-1) and its Young's modulus is 2.0 xx 10^11 N m^(-2) .