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Summer 2012 PHYS 172: Modern Mechanics Lecture 5 – Gravity Read 3.1-3.10.

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Presentation on theme: "Summer 2012 PHYS 172: Modern Mechanics Lecture 5 – Gravity Read 3.1-3.10."— Presentation transcript:

1 Summer 2012 PHYS 172: Modern Mechanics Lecture 5 – Gravity Read 3.1-3.10

2 The gravitational force law m1m1 m2m2 Newton m1m1 m2m2 Cavendish Gravitational constant

3 Features of gravitational force gravity is always attractive gravity is an inverse square law the force depends upon the product of the masses

4 Distance between two objects Point object: idealized object which has no size, all mass is in one point If distance between the two objects is >> than their size, can model the objects as point-masses Real objects: have size Special case: spherical objects (spherical symmetry) Uniform-density spheres interact gravitationally in exactly the same way as if all their mass were concentrated at the center of the sphere. Can model as a point mass!

5 Clicker question #1 What is the distance between these two spheres to be used in gravitational law? A B

6 Gravitational force on a planet starplanet 1. Calculate 2. Distance 3. Unit vector: 3. Force: directionmagnitude

7 Gravitational force on a planet starplanet Checking results: 1.Diagram 2.Order of magnitude 3.Units 4.Unit vector Clicker question # 3: What is the gravitational force exerted by the planet on the star? A) The same B) C)

8 Gravitational force near the Earth’s surface RERE m ~ The same for all objects on surface Gravitational field The magnitude: g = 9.8 N/kg M E = 5.976 ×10 24 kg R E = 6.37 ×10 6 m

9 Reciprocity: Newton’s 3rd law Force magnitudes are the same Directions are opposite They act on different objects Reciprocity (Newton’s 3 rd law): The forces of two objects on each other are always equal and are directed in opposite directions NOTE: Velocity-dependent forces (e.g., magnetic forces) do not obey Newton’s 3 rd law!

10 The gravitational force exerted by a planet on one of its moons is 3e23 newtons when the moon is at a particular location. If the mass of the moon were three times as large, what would the force on the moon be? A) 1e23 N B) 3e23 N C) 6e23 N D) 9e23 N Q3.4.a

11 The gravitational force exerted by a planet on one of its moons is 3e23 newtons when the moon is at a particular location. If the distance between the moon and the planet was doubled, what would the force on the moon be? A) 6e23 N B) 3e23 N C) 1.5e23 N D) 0.75e23 N E) 0.33e23 N Q3.4.b

12 Fixed star position : m Initial planet position: m Calculate the vector that points from the star to the planet. A) m B) m C) m D) m E) We don’t have enough information to find the vector Q3.4.c:

13 The relative position vector from the star to the planet is: m. What is the distance between the star and the planet? A) 0.50e11 m B) 1.50e11 m C) 1.58e11 m D) 2.00e11 m E) 2.50e11 m Q3.4.d

14 Distance from star to planet: 1.58e11 m Star’s mass: 1e30 kg Planet’s mass: 5e24 kg G = 6.7e-11 N · m 2 /kg 2 Calculate the magnitude of the gravitational force that the star exerts on the planet. A) 1.34e-8 N B) 2.68e-2 N C) 1.34e22 N D) 2.12e33 N E) 5.3e55 N Q3.4.e:

15 Relative position vector from star to planet is m Distance from star to planet is 1.58e11 m Find the unit vector pointing from the star to the planet A) B) C) D) E) Q3.4.f:

16 Calculate the gravitational force exerted by the star on the planet (remember that force is a vector) A) N B) N C) N D) N E) N Q3.4.g:


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