According to the kinetic theory of gases, at absolute zero (0 Kelvin or -273.15°C), the molecules of a substance have no kinetic energy and their motion theoretically stops completely. This is the lowest possible temperature. Click this more information: https://www.tiwariacademy.com/ncert-solutionsRead more
According to the kinetic theory of gases, at absolute zero (0 Kelvin or -273.15°C), the molecules of a substance have no kinetic energy and their motion theoretically stops completely. This is the lowest possible temperature.
Mercury thermometers can measure temperatures up to around 360°C because mercury stays in its liquid state up to this temperature. Beyond this, mercury begins to vaporize and cannot be used for measurements above this point. Click for more: https://www.tiwariacademy.com/ncert-solutions/class-11/physRead more
Mercury thermometers can measure temperatures up to around 360°C because mercury stays in its liquid state up to this temperature. Beyond this, mercury begins to vaporize and cannot be used for measurements above this point.
The amount of sun's radiant energy received is proportional to the power output of the sun from Stefan-Boltzmann's Law: P ∝ R²T⁴ 1. Preliminary P₁ ∝ R²T⁴ 2. After alteration - The radius increases to 2R: The area increases proportionally to (2R)² = 4R² - Temperature increases to 2T: Power increasesRead more
The amount of sun’s radiant energy received is proportional to the power output of the sun from Stefan-Boltzmann’s Law:
P ∝ R²T⁴
1. Preliminary
P₁ ∝ R²T⁴
2. After alteration
– The radius increases to 2R: The area increases proportionally to (2R)² = 4R²
– Temperature increases to 2T: Power increases proportionally to (2T)⁴ = 16T⁴
– Total power increases to:
P₂ ∝ 4R² × 16T⁴ = 64R²T⁴
3. The ratio of the new power to the old power:
P₂ / P₁ = (64R²T⁴) / (R²T⁴) = 64
Thus, the radiant energy received on Earth will increase by a factor of 64.
Pyrometers are designed to measure extremely high temperatures, such as those in the range of 2,000 to 2,500°C, and are commonly used in industrial applications like furnaces and molten metal. Click here for more: https://www.tiwariacademy.com/ncert-solutions/class-11/physics/chapter-10/
Pyrometers are designed to measure extremely high temperatures, such as those in the range of 2,000 to 2,500°C, and are commonly used in industrial applications like furnaces and molten metal.
In the case of a frictionless inclined table, the work done by the table surface on the ball can be analyzed through the forces acting on the ball. Since there is no friction, the only force acting parallel to the surface is gravity. Gravity does not do work against the normal force of the table. ThRead more
In the case of a frictionless inclined table, the work done by the table surface on the ball can be analyzed through the forces acting on the ball.
Since there is no friction, the only force acting parallel to the surface is gravity. Gravity does not do work against the normal force of the table. The normal force acts perpendicular to the displacement of the ball.
Work done (W) is given by the formula:
W = F • d • cos(θ)
Where:
– F is the force
– d is the displacement
– θ is the angle between the force and displacement
This implies that the displacement and the force exerted are perpendicular to each other, that is, θ = 90 degrees. This gives cos(90°) = 0. Thus the work done by the table surface on the ball is:
W = F • d • 0 = 0
Final Answer:
The work done by the table surface on the ball is zero.
To calculate the work done on the body, we can use the work-energy principle, which states that the work done on an object is equal to the change in its kinetic energy. Step 1: Calculate the initial kinetic energy (K.E.₁) Since the body is initially at rest, its initial kinetic energy is: K.E.₁ = (1Read more
To calculate the work done on the body, we can use the work-energy principle, which states that the work done on an object is equal to the change in its kinetic energy.
Step 1: Calculate the initial kinetic energy (K.E.₁)
Since the body is initially at rest, its initial kinetic energy is:
K.E.₁ = (1/2) m v₁²
K.E.₁ = (1/2) × 10 kg × (0 m/s)²
K.E.₁ = 0 J
Step 2: Final kinetic energy K.E.₂
When the body has achieved a velocity of 10 m/s, the final kinetic energy is:
We can find the maximum height reached by a ball after it is dropped from height h and bounces on the ground with a coefficient of restitution e using the following analysis: 1. When the ball is dropped from height h, it gains kinetic energy just before hitting the ground. The potential energy at heRead more
We can find the maximum height reached by a ball after it is dropped from height h and bounces on the ground with a coefficient of restitution e using the following analysis:
1. When the ball is dropped from height h, it gains kinetic energy just before hitting the ground. The potential energy at height h is converted to kinetic energy:
Potential Energy (PE) = mgh
Kinetic Energy (KE) at the moment of impact = mgh
2. When it bounces, some energy is lost due to the coefficient of restitution e. The coefficient of restitution is defined as the ratio of the velocity after the bounce to the velocity before the bounce:
e = (velocity after bounce) / (velocity before bounce)
3. Velocity at the instant of hitting the ground (v) is determined by the relation:
v = √(2gh)
4. Just after the bounce, the velocity is given by,
velocity after bounce = e * v = e * √(2gh)
5. Maximum height (h’) attained just after the bounce can be calculated from the K.E. at the instant of bounce
K.E. after bounce = (1/2) m (e * √(2gh))²
This kinetic energy is turned back into potential energy at the maximum height:
PE at max height = mgh’
Thus, (1/2) m (e² * 2gh) = mgh’
Simplifying gives:
h’ = e²h
Final Answer:
The maximum height after the bounce is e²h.
To find the velocity of two particles that collide and stick together, we can use the principles of conservation of momentum. Let: - Mass of each particle = m - Initial velocity of the first particle (moving north) = v - Initial velocity of the second particle (moving east) = v 1. Momentum Before CoRead more
To find the velocity of two particles that collide and stick together, we can use the principles of conservation of momentum.
Let:
– Mass of each particle = m
– Initial velocity of the first particle (moving north) = v
– Initial velocity of the second particle (moving east) = v
1. Momentum Before Collision:
– Momentum of the first particle (north): p₁ = m * v
– Momentum of the second particle (east): p₂ = m * v
2. Total Momentum Before Collision:
– The momentum vector of the first particle is (0, mv) (north direction).
– The momentum vector of the second particle is (mv, 0) (east direction).
– Therefore, the total momentum vector before the collision is:
P_initial = (mv, mv)
3. Momentum After Collision:
– Since the two particles stick together after the collision, the combined mass is 2m.
– Let the velocity of the combined mass after the collision be V, and its direction will be towards the northeast.
4. Using Pythagoras’ Theorem:
– The magnitude of the momentum vector after the collision can be found using:
P_final = √[(mv)² + (mv)²] = √[2(mv)²] = mv√2
5. Calculating the Final Velocity:
– The total momentum after the collision is equal to the momentum before the collision:
P_final = 2m * V
– Setting them equal:
mv√2 = 2m * V
– Canceling m from both sides:
v√2 = 2V
– Solving for V:
V = (v√2) / 2 = v / √2
Final Answer:
The velocity of the combined mass after the collision is v/√2.
To calculate the work done by the variable force F = x + x³ over the displacement from x = 0 m to x = 2 m, we use the work integral: Work W = ∫[0 to 2] F(x) dx Where: - F(x) = x + x³ - x₁ = 0, x₂ = 2 Step 1: Set up the integral W = ∫[0 to 2] (x + x³) dx Step 2: Split and evaluate the integral W = ∫[Read more
To calculate the work done by the variable force F = x + x³ over the displacement from x = 0 m to x = 2 m, we use the work integral:
Work W = ∫[0 to 2] F(x) dx
Where:
– F(x) = x + x³
– x₁ = 0, x₂ = 2
Step 1: Set up the integral
W = ∫[0 to 2] (x + x³) dx
Step 2: Split and evaluate the integral
W = ∫[0 to 2] x dx + ∫[0 to 2] x³ dx
1. For ∫[0 to 2] x dx:
∫ x dx = (1/2) x² |[0 to 2] = (1/2) (2²) – (1/2) (0²) = 2
2. For ∫[0 to 2] x³ dx:
∫ x³ dx = (1/4) x⁴ |[0 to 2] = (1/4) (2⁴) – (1/4) (0⁴) = (16/4) – 0 = 4
Step 3: Add the results
W = 2 + 4 = 6 J
Final Answer:
The work done by the variable force is 6 J.
The coefficient of restitution, e, is defined as the ratio of the relative velocity of separation to the relative velocity of approach between two colliding objects. For a perfectly elastic collision, the kinetic energy and momentum are conserved, and the objects rebound without any loss of energy.Read more
The coefficient of restitution, e, is defined as the ratio of the relative velocity of separation to the relative velocity of approach between two colliding objects.
For a perfectly elastic collision, the kinetic energy and momentum are conserved, and the objects rebound without any loss of energy. Therefore, the coefficient of restitution for a perfectly elastic collision is:
e = 1
Final Answer:
The coefficient of restitution, e, for a perfectly elastic collision is 1.
According to kinetic theory of gases at absolute zero of temperature
According to the kinetic theory of gases, at absolute zero (0 Kelvin or -273.15°C), the molecules of a substance have no kinetic energy and their motion theoretically stops completely. This is the lowest possible temperature. Click this more information: https://www.tiwariacademy.com/ncert-solutionsRead more
According to the kinetic theory of gases, at absolute zero (0 Kelvin or -273.15°C), the molecules of a substance have no kinetic energy and their motion theoretically stops completely. This is the lowest possible temperature.
Click this more information:
See lesshttps://www.tiwariacademy.com/ncert-solutions/class-11/physics/chapter-10/
Mercury thermometer can be used to measure temperature upto
Mercury thermometers can measure temperatures up to around 360°C because mercury stays in its liquid state up to this temperature. Beyond this, mercury begins to vaporize and cannot be used for measurements above this point. Click for more: https://www.tiwariacademy.com/ncert-solutions/class-11/physRead more
Mercury thermometers can measure temperatures up to around 360°C because mercury stays in its liquid state up to this temperature. Beyond this, mercury begins to vaporize and cannot be used for measurements above this point.
Click for more:
See lesshttps://www.tiwariacademy.com/ncert-solutions/class-11/physics/chapter-10/
If the temperature of the sun were to increase from T to 2 T and its radius from R to 2 R, then the ratio of the radiant energy received on earth to what it was previously, will be
The amount of sun's radiant energy received is proportional to the power output of the sun from Stefan-Boltzmann's Law: P ∝ R²T⁴ 1. Preliminary P₁ ∝ R²T⁴ 2. After alteration - The radius increases to 2R: The area increases proportionally to (2R)² = 4R² - Temperature increases to 2T: Power increasesRead more
The amount of sun’s radiant energy received is proportional to the power output of the sun from Stefan-Boltzmann’s Law:
P ∝ R²T⁴
1. Preliminary
P₁ ∝ R²T⁴
2. After alteration
– The radius increases to 2R: The area increases proportionally to (2R)² = 4R²
– Temperature increases to 2T: Power increases proportionally to (2T)⁴ = 16T⁴
– Total power increases to:
P₂ ∝ 4R² × 16T⁴ = 64R²T⁴
3. The ratio of the new power to the old power:
P₂ / P₁ = (64R²T⁴) / (R²T⁴) = 64
Thus, the radiant energy received on Earth will increase by a factor of 64.
Click here for more:
See lesshttps://www.tiwariacademy.com/ncert-solutions/class-11/physics/chapter-10/
For measuring temperature in the range of 2,000 to 2,500°C, we should employ
Pyrometers are designed to measure extremely high temperatures, such as those in the range of 2,000 to 2,500°C, and are commonly used in industrial applications like furnaces and molten metal. Click here for more: https://www.tiwariacademy.com/ncert-solutions/class-11/physics/chapter-10/
Pyrometers are designed to measure extremely high temperatures, such as those in the range of 2,000 to 2,500°C, and are commonly used in industrial applications like furnaces and molten metal.
Click here for more:
See lesshttps://www.tiwariacademy.com/ncert-solutions/class-11/physics/chapter-10/
A ball moves in a frictionless inclined table without slipping. The work done by the table surface on the ball is
In the case of a frictionless inclined table, the work done by the table surface on the ball can be analyzed through the forces acting on the ball. Since there is no friction, the only force acting parallel to the surface is gravity. Gravity does not do work against the normal force of the table. ThRead more
In the case of a frictionless inclined table, the work done by the table surface on the ball can be analyzed through the forces acting on the ball.
Since there is no friction, the only force acting parallel to the surface is gravity. Gravity does not do work against the normal force of the table. The normal force acts perpendicular to the displacement of the ball.
Work done (W) is given by the formula:
W = F • d • cos(θ)
Where:
– F is the force
– d is the displacement
– θ is the angle between the force and displacement
This implies that the displacement and the force exerted are perpendicular to each other, that is, θ = 90 degrees. This gives cos(90°) = 0. Thus the work done by the table surface on the ball is:
W = F • d • 0 = 0
Final Answer:
The work done by the table surface on the ball is zero.
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See lesshttps://www.tiwariacademy.com/ncert-solutions/class-11/physics/chapter-5/
A body of mass 10 kg initially at rest acquires velocity of 10 ms⁻¹. What is the work done?
To calculate the work done on the body, we can use the work-energy principle, which states that the work done on an object is equal to the change in its kinetic energy. Step 1: Calculate the initial kinetic energy (K.E.₁) Since the body is initially at rest, its initial kinetic energy is: K.E.₁ = (1Read more
To calculate the work done on the body, we can use the work-energy principle, which states that the work done on an object is equal to the change in its kinetic energy.
Step 1: Calculate the initial kinetic energy (K.E.₁)
Since the body is initially at rest, its initial kinetic energy is:
K.E.₁ = (1/2) m v₁²
K.E.₁ = (1/2) × 10 kg × (0 m/s)²
K.E.₁ = 0 J
Step 2: Final kinetic energy K.E.₂
When the body has achieved a velocity of 10 m/s, the final kinetic energy is:
K.E.₂ = (1/2) m v₂²
K.E.₂ = (1/2) × 10 kg × (10 m/s)²
K.E.₂ = (1/2) × 10 × 100
K.E.₂ = 500 J
Step 3: Work done (W)
The work done equals the change in kinetic energy
W = K.E.₂ – K.E.₁
W = 500 J – 0 J
W = 500 J
Final Answer:
Work done is 500 J.
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A ball is dropped from height h on the ground where coefficient of restitution is e. After one balance the maximum height is
We can find the maximum height reached by a ball after it is dropped from height h and bounces on the ground with a coefficient of restitution e using the following analysis: 1. When the ball is dropped from height h, it gains kinetic energy just before hitting the ground. The potential energy at heRead more
We can find the maximum height reached by a ball after it is dropped from height h and bounces on the ground with a coefficient of restitution e using the following analysis:
1. When the ball is dropped from height h, it gains kinetic energy just before hitting the ground. The potential energy at height h is converted to kinetic energy:
Potential Energy (PE) = mgh
Kinetic Energy (KE) at the moment of impact = mgh
2. When it bounces, some energy is lost due to the coefficient of restitution e. The coefficient of restitution is defined as the ratio of the velocity after the bounce to the velocity before the bounce:
e = (velocity after bounce) / (velocity before bounce)
3. Velocity at the instant of hitting the ground (v) is determined by the relation:
v = √(2gh)
4. Just after the bounce, the velocity is given by,
velocity after bounce = e * v = e * √(2gh)
5. Maximum height (h’) attained just after the bounce can be calculated from the K.E. at the instant of bounce
K.E. after bounce = (1/2) m (e * √(2gh))²
This kinetic energy is turned back into potential energy at the maximum height:
PE at max height = mgh’
Thus, (1/2) m (e² * 2gh) = mgh’
Simplifying gives:
h’ = e²h
Final Answer:
The maximum height after the bounce is e²h.
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See lesshttps://www.tiwariacademy.com/ncert-solutions/class-11/physics/chapter-5/
A particle of mass m having velocity v moving towards north collides with similar particle moving with same velocity towards east. The two particles stick together and move towards north east with a velocity
To find the velocity of two particles that collide and stick together, we can use the principles of conservation of momentum. Let: - Mass of each particle = m - Initial velocity of the first particle (moving north) = v - Initial velocity of the second particle (moving east) = v 1. Momentum Before CoRead more
To find the velocity of two particles that collide and stick together, we can use the principles of conservation of momentum.
Let:
– Mass of each particle = m
– Initial velocity of the first particle (moving north) = v
– Initial velocity of the second particle (moving east) = v
1. Momentum Before Collision:
– Momentum of the first particle (north): p₁ = m * v
– Momentum of the second particle (east): p₂ = m * v
2. Total Momentum Before Collision:
– The momentum vector of the first particle is (0, mv) (north direction).
– The momentum vector of the second particle is (mv, 0) (east direction).
– Therefore, the total momentum vector before the collision is:
P_initial = (mv, mv)
3. Momentum After Collision:
– Since the two particles stick together after the collision, the combined mass is 2m.
– Let the velocity of the combined mass after the collision be V, and its direction will be towards the northeast.
4. Using Pythagoras’ Theorem:
– The magnitude of the momentum vector after the collision can be found using:
P_final = √[(mv)² + (mv)²] = √[2(mv)²] = mv√2
5. Calculating the Final Velocity:
– The total momentum after the collision is equal to the momentum before the collision:
P_final = 2m * V
– Setting them equal:
mv√2 = 2m * V
– Canceling m from both sides:
v√2 = 2V
– Solving for V:
V = (v√2) / 2 = v / √2
Final Answer:
See lessThe velocity of the combined mass after the collision is v/√2.
The work done by an applied variable force F = x + x³ from x = 0 m to x = 2 m, where x is displacement , is
To calculate the work done by the variable force F = x + x³ over the displacement from x = 0 m to x = 2 m, we use the work integral: Work W = ∫[0 to 2] F(x) dx Where: - F(x) = x + x³ - x₁ = 0, x₂ = 2 Step 1: Set up the integral W = ∫[0 to 2] (x + x³) dx Step 2: Split and evaluate the integral W = ∫[Read more
To calculate the work done by the variable force F = x + x³ over the displacement from x = 0 m to x = 2 m, we use the work integral:
Work W = ∫[0 to 2] F(x) dx
Where:
– F(x) = x + x³
– x₁ = 0, x₂ = 2
Step 1: Set up the integral
W = ∫[0 to 2] (x + x³) dx
Step 2: Split and evaluate the integral
W = ∫[0 to 2] x dx + ∫[0 to 2] x³ dx
1. For ∫[0 to 2] x dx:
∫ x dx = (1/2) x² |[0 to 2] = (1/2) (2²) – (1/2) (0²) = 2
2. For ∫[0 to 2] x³ dx:
∫ x³ dx = (1/4) x⁴ |[0 to 2] = (1/4) (2⁴) – (1/4) (0⁴) = (16/4) – 0 = 4
Step 3: Add the results
W = 2 + 4 = 6 J
Final Answer:
The work done by the variable force is 6 J.
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The coefficient of restitute, e, for a perfectly elastic collision is?
The coefficient of restitution, e, is defined as the ratio of the relative velocity of separation to the relative velocity of approach between two colliding objects. For a perfectly elastic collision, the kinetic energy and momentum are conserved, and the objects rebound without any loss of energy.Read more
The coefficient of restitution, e, is defined as the ratio of the relative velocity of separation to the relative velocity of approach between two colliding objects.
For a perfectly elastic collision, the kinetic energy and momentum are conserved, and the objects rebound without any loss of energy. Therefore, the coefficient of restitution for a perfectly elastic collision is:
e = 1
Final Answer:
The coefficient of restitution, e, for a perfectly elastic collision is 1.
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See lesshttps://www.tiwariacademy.com/ncert-solutions/class-11/physics/chapter-5/