6 RBTS PAPER(PHYSICS)
6 RBTS PAPER

163165 The Young's modulus of a wire is numerically equal to the stress which will : [RBQ]

1 Not change the length of the wire
2 Double the length of the wire
3 Increase the length by \(50 \%\)
4 Change the area of cross-section of the wire to half
6 RBTS PAPER

163166 If the length of a wire decrease by \(1 \%\) on loading a \(2 \mathrm{~kg}\) weight on it. Then the linear strain in wire will be: [RBQ]

1 0.001
2 0.1
3 0.01
4 1
6 RBTS PAPER

163167 A spherical ball is compressed by \(0.01 \%\) when a pressure of 100 atmosphere is applied on it. Its bulk modulus of elasticity in dyne/cm \({ }^2\) will be approximately: [RBQ]

1 \(10^{12}\)
2 \(10^{14}\)
3 \(10^6\)
4 \(10^{24}\)
6 RBTS PAPER

163168 The approximate depth of an ocean is \(2700 \mathrm{~m}\). The compressibility of water is \(45.4 \times 10^{-11} \mathrm{~Pa}^{-1}\) and density of water is \(10^3 \mathrm{~kg} / \mathrm{m}^3\). What fractional compression of water will be obtained at the bottom of the ocean : [RBQ]

1 \(0.8 \times 10^{-2}\)
2 \(1.0 \times 10^{-2}\)
3 \(1.2 \times 10^{-2}\)
4 \(1.4 \times 10^{-2}\).
6 RBTS PAPER

163169 The breaking stress of a material is \(10^9\) pascal. If the density of material is \(3 \times 10^3 \mathrm{~kg} / \mathrm{m}^3\). The minimum length of the wire for which it breaks under its own weight will be : [RBQ]

1 \(3.4 \mathrm{~m}\)
2 \(3.4 \times 10^4 \mathrm{~m}\)
3 \(3.4 \times 10^5 \mathrm{~m}\)
4 \(3.4 \times 10^3 \mathrm{~m}\)
6 RBTS PAPER

163165 The Young's modulus of a wire is numerically equal to the stress which will : [RBQ]

1 Not change the length of the wire
2 Double the length of the wire
3 Increase the length by \(50 \%\)
4 Change the area of cross-section of the wire to half
6 RBTS PAPER

163166 If the length of a wire decrease by \(1 \%\) on loading a \(2 \mathrm{~kg}\) weight on it. Then the linear strain in wire will be: [RBQ]

1 0.001
2 0.1
3 0.01
4 1
6 RBTS PAPER

163167 A spherical ball is compressed by \(0.01 \%\) when a pressure of 100 atmosphere is applied on it. Its bulk modulus of elasticity in dyne/cm \({ }^2\) will be approximately: [RBQ]

1 \(10^{12}\)
2 \(10^{14}\)
3 \(10^6\)
4 \(10^{24}\)
6 RBTS PAPER

163168 The approximate depth of an ocean is \(2700 \mathrm{~m}\). The compressibility of water is \(45.4 \times 10^{-11} \mathrm{~Pa}^{-1}\) and density of water is \(10^3 \mathrm{~kg} / \mathrm{m}^3\). What fractional compression of water will be obtained at the bottom of the ocean : [RBQ]

1 \(0.8 \times 10^{-2}\)
2 \(1.0 \times 10^{-2}\)
3 \(1.2 \times 10^{-2}\)
4 \(1.4 \times 10^{-2}\).
6 RBTS PAPER

163169 The breaking stress of a material is \(10^9\) pascal. If the density of material is \(3 \times 10^3 \mathrm{~kg} / \mathrm{m}^3\). The minimum length of the wire for which it breaks under its own weight will be : [RBQ]

1 \(3.4 \mathrm{~m}\)
2 \(3.4 \times 10^4 \mathrm{~m}\)
3 \(3.4 \times 10^5 \mathrm{~m}\)
4 \(3.4 \times 10^3 \mathrm{~m}\)
6 RBTS PAPER

163165 The Young's modulus of a wire is numerically equal to the stress which will : [RBQ]

1 Not change the length of the wire
2 Double the length of the wire
3 Increase the length by \(50 \%\)
4 Change the area of cross-section of the wire to half
6 RBTS PAPER

163166 If the length of a wire decrease by \(1 \%\) on loading a \(2 \mathrm{~kg}\) weight on it. Then the linear strain in wire will be: [RBQ]

1 0.001
2 0.1
3 0.01
4 1
6 RBTS PAPER

163167 A spherical ball is compressed by \(0.01 \%\) when a pressure of 100 atmosphere is applied on it. Its bulk modulus of elasticity in dyne/cm \({ }^2\) will be approximately: [RBQ]

1 \(10^{12}\)
2 \(10^{14}\)
3 \(10^6\)
4 \(10^{24}\)
6 RBTS PAPER

163168 The approximate depth of an ocean is \(2700 \mathrm{~m}\). The compressibility of water is \(45.4 \times 10^{-11} \mathrm{~Pa}^{-1}\) and density of water is \(10^3 \mathrm{~kg} / \mathrm{m}^3\). What fractional compression of water will be obtained at the bottom of the ocean : [RBQ]

1 \(0.8 \times 10^{-2}\)
2 \(1.0 \times 10^{-2}\)
3 \(1.2 \times 10^{-2}\)
4 \(1.4 \times 10^{-2}\).
6 RBTS PAPER

163169 The breaking stress of a material is \(10^9\) pascal. If the density of material is \(3 \times 10^3 \mathrm{~kg} / \mathrm{m}^3\). The minimum length of the wire for which it breaks under its own weight will be : [RBQ]

1 \(3.4 \mathrm{~m}\)
2 \(3.4 \times 10^4 \mathrm{~m}\)
3 \(3.4 \times 10^5 \mathrm{~m}\)
4 \(3.4 \times 10^3 \mathrm{~m}\)
NEET Test Series from KOTA - 10 Papers In MS WORD WhatsApp Here
6 RBTS PAPER

163165 The Young's modulus of a wire is numerically equal to the stress which will : [RBQ]

1 Not change the length of the wire
2 Double the length of the wire
3 Increase the length by \(50 \%\)
4 Change the area of cross-section of the wire to half
6 RBTS PAPER

163166 If the length of a wire decrease by \(1 \%\) on loading a \(2 \mathrm{~kg}\) weight on it. Then the linear strain in wire will be: [RBQ]

1 0.001
2 0.1
3 0.01
4 1
6 RBTS PAPER

163167 A spherical ball is compressed by \(0.01 \%\) when a pressure of 100 atmosphere is applied on it. Its bulk modulus of elasticity in dyne/cm \({ }^2\) will be approximately: [RBQ]

1 \(10^{12}\)
2 \(10^{14}\)
3 \(10^6\)
4 \(10^{24}\)
6 RBTS PAPER

163168 The approximate depth of an ocean is \(2700 \mathrm{~m}\). The compressibility of water is \(45.4 \times 10^{-11} \mathrm{~Pa}^{-1}\) and density of water is \(10^3 \mathrm{~kg} / \mathrm{m}^3\). What fractional compression of water will be obtained at the bottom of the ocean : [RBQ]

1 \(0.8 \times 10^{-2}\)
2 \(1.0 \times 10^{-2}\)
3 \(1.2 \times 10^{-2}\)
4 \(1.4 \times 10^{-2}\).
6 RBTS PAPER

163169 The breaking stress of a material is \(10^9\) pascal. If the density of material is \(3 \times 10^3 \mathrm{~kg} / \mathrm{m}^3\). The minimum length of the wire for which it breaks under its own weight will be : [RBQ]

1 \(3.4 \mathrm{~m}\)
2 \(3.4 \times 10^4 \mathrm{~m}\)
3 \(3.4 \times 10^5 \mathrm{~m}\)
4 \(3.4 \times 10^3 \mathrm{~m}\)
6 RBTS PAPER

163165 The Young's modulus of a wire is numerically equal to the stress which will : [RBQ]

1 Not change the length of the wire
2 Double the length of the wire
3 Increase the length by \(50 \%\)
4 Change the area of cross-section of the wire to half
6 RBTS PAPER

163166 If the length of a wire decrease by \(1 \%\) on loading a \(2 \mathrm{~kg}\) weight on it. Then the linear strain in wire will be: [RBQ]

1 0.001
2 0.1
3 0.01
4 1
6 RBTS PAPER

163167 A spherical ball is compressed by \(0.01 \%\) when a pressure of 100 atmosphere is applied on it. Its bulk modulus of elasticity in dyne/cm \({ }^2\) will be approximately: [RBQ]

1 \(10^{12}\)
2 \(10^{14}\)
3 \(10^6\)
4 \(10^{24}\)
6 RBTS PAPER

163168 The approximate depth of an ocean is \(2700 \mathrm{~m}\). The compressibility of water is \(45.4 \times 10^{-11} \mathrm{~Pa}^{-1}\) and density of water is \(10^3 \mathrm{~kg} / \mathrm{m}^3\). What fractional compression of water will be obtained at the bottom of the ocean : [RBQ]

1 \(0.8 \times 10^{-2}\)
2 \(1.0 \times 10^{-2}\)
3 \(1.2 \times 10^{-2}\)
4 \(1.4 \times 10^{-2}\).
6 RBTS PAPER

163169 The breaking stress of a material is \(10^9\) pascal. If the density of material is \(3 \times 10^3 \mathrm{~kg} / \mathrm{m}^3\). The minimum length of the wire for which it breaks under its own weight will be : [RBQ]

1 \(3.4 \mathrm{~m}\)
2 \(3.4 \times 10^4 \mathrm{~m}\)
3 \(3.4 \times 10^5 \mathrm{~m}\)
4 \(3.4 \times 10^3 \mathrm{~m}\)