## MCAT Physics and Math Review

## Chapter 1: Kinematics and Dynamics

### 1.4 Forces and Acceleration

Every change in velocity is motivated by a push or a pull—a **force**. In this section, we’ll examine how forces interact with one another, as well as how acceleration results from those forces.

FORCES

**Force **(**F**) is a vector quantity that is experienced as pushing or pulling on objects. Forces can exist between objects that aren’t even touching. While it is common for forces to be exerted by one object pushing on another, there are even more instances in which forces exist between objects nowhere near each other, such as gravity or electrostatic forces between point charges. The SI unit for force is the **newton **(**N**), which is equivalent to one

*Gravity*

When Newton observed apples falling out of trees, he was struck by the fact that they always fell perpendicularly to the ground, rather than sideways or even away from the ground. Furthermore, Newton began to wonder about the farthest reaches of gravity. If the apple feels this attractive pull toward the Earth, then what about the Moon? Indeed, what Newton came to understand he called universal gravitation.

**MCAT EXPERTISE**

Acceleration due to gravity, g, decreases with height above the Earth and increases the closer one gets to the Earth’s center of mass. Near the Earth’s surface, use

**Gravity** is an attractive force that is felt by all forms of matter. We usually think of gravity as acting on us to keep us from floating off of the Earth’s surface, or for holding the planets of our solar system in orbit. However, all objects exert gravitational forces on each other; there is a small (but measurable) force of gravity between you and this *MCAT Physics and Math Review* book, the chair you’re sitting on, and all the objects around you. Gravitational forces usually do not have much significance on the small scale because other forces tend to be much larger in magnitude. Only on the planetary level do gravitational forces really take on a significant value.

**REAL WORLD**

Newton’s third law states that the force of gravity on *m*_{1} from *m*_{2} is equal and opposite to the force of gravity on *m*_{2} from *m*_{1}. This means that the force of gravity on you from the Earth is equal and opposite to the force of gravity from you on the Earth. Because the forces are equal but the masses are very different, the accelerations must also be very different, from **F** = *m***a** (discussed later in this chapter). Because your mass is very small compared to the Earth, you experience a large acceleration from it. In contrast, because the Earth is massive, it experiences a tiny acceleration from the same magnitude of force.

The magnitude of the **gravitational force** between two objects is

**Equation 1.8**

where G is the universal gravitational constant *m*_{1} and *m*_{2} are the masses of the two objects, and *r* is the distance between their centers of mass. This equation is commonly tested in the context of proportionalities. For instance, that the magnitude of the gravitational force is inversely related to the square of the distance (that is, if *r* is halved, then *F*_{g} will quadruple). The magnitude of the gravitational force is also directly related to the masses of the objects (that is, if *m*_{1} is tripled, then *F*_{g} will triple).

**Example:**

Find the gravitational force between an electron and a proton that are 10^{–11} m apart. (Note: Mass of a proton = 1.67 × 10^{–27} kg; mass of an electron = 9.11 × 10^{–31} kg)

**Solution:**

Use Newton’s law of gravitation:

*Friction*

**Friction** is a type of force that opposes the movement of objects. Unlike other kinds of forces, such as gravity or electromagnetic force, which can cause objects either to speed up or slow down, friction forces almost always oppose an object’s motion and cause it to slow down or become stationary. There are two types of friction: static and kinetic.

**Static friction** (**f**_{s}) exists between a stationary object and the surface upon which it rests. The equation that describes the magnitude of static friction is

0 ≤ *f*_{s} ≤ *μ*_{s}*N*

**Equation 1.9**

where *μ*_{s} is the coefficient of static friction and *N* is the magnitude of the normal force. The **coefficient of static friction** is a unitless quantity that is dependent on the two materials in contact. The **normal force** is the component of the force between two objects in contact that is perpendicular to the plane of contact between the object and the surface upon which it rests.

Note the less-than-or-equal-to signs in the equation. These signify that there is a range of possible values for static friction. The minimum, of course, is zero. This would be the case if an object were resting on a surface with no applied forces. The maximum value of static friction can be calculated from the right side of the previous equation. One should not assume that objects that are stationary are experiencing a maximal static force of friction.

Consider trying to push a heavy piece of luggage. When a 25 N force is applied, the bag does not move. When a 50 N force is applied, the bag still does not move. When a 100 N force is applied, the bag slides a meter or so and slows to a rest. This setup implies that the maximal value of static friction is somewhere between 50 and 100 N; any applied force less than this threshold will not be sufficient to move the bag as there will be an equal but opposite force of static friction opposing the bag’s motion.

**KEY CONCEPT**

Contact points are the places where friction occurs between two rough surfaces sliding past each other. If the normal load—the force that squeezes the two together—rises, the total area of contact increases. That increase, more than the surface’s roughness, governs the degree of friction. This is illustrated in Figure 1.7 below.

**Figure** **1.7.** **Increases in Contact Area Increase Frictional Forces**

**Kinetic friction** (**f**_{k}) exists between a sliding object and the surface over which the object slides. Sometimes, students misidentify the presence of kinetic friction. A wheel, for example, that is rolling along a road does not experience kinetic friction because the tire is not actually sliding against the pavement. The tire maintains an instantaneous point of static contact with the road and, therefore, experiences static friction. Only when the tire begins to slide on, say, an icy patch will kinetic friction come into play. To be sure, any time two surfaces slide against each other, kinetic friction will be present and its magnitude can be measured according to this equation:

*f*_{k} = *μ*_{k}*N*

**Equation 1.10**

where *μ*_{k} is the coefficient of kinetic friction and *N* is the normal force. There are two important distinctions between this equation for kinetic friction and the previous equation for static friction. First, the kinetic friction equation has an equals sign. This means that kinetic friction will have a constant value for any given combination of a coefficient of kinetic friction and normal force. It does not matter how much surface area is in contact or even the velocity of the sliding object. Second, the two equations have a different coefficient of friction. The value of *μ*_{s} is always larger than the value of *μ*_{k}. Therefore, the maximum value for static friction will always be greater than the constant value for kinetic friction: objects will “stick” until they start moving, and then will slide more easily over one another.

**KEY CONCEPT**

The coefficient of static friction will always be larger than the coefficient of kinetic friction. It always requires more force to get an object to start sliding than it takes to keep an object sliding.

As previously mentioned in the discussion of static friction, pay close attention to the conditions set in an MCAT passage or question. Does it say that friction can be assumed to be negligible, or does it provide the coefficient of friction values, which will most likely need to be used in a calculation of friction? Friction will be incorporated into our examination of translational equilibrium later in this chapter.

MASS AND WEIGHT

Mass and weight are not the same. **Mass **(*m*) is a measure of a body’s inertia—the amount of matter in the object. Mass is a scalar quantity, and, as such, has magnitude only. The SI unit for mass is the kilogram, which is independent of gravity. One kilogram of material on Earth will have the same mass as one kilogram of material on the Moon. **Weight **(**F**_{g}), on the other hand, is a measure of gravitational force (usually that of the Earth) on an object’s mass. Because weight is a force, it is a vector quantity with the units of newtons (N).

While mass and weight are not synonymous, they are related by the equation:

**F**_{g} = *m***g**

**Equation 1.11**

where **F**_{g} is the weight of the object, *m* is its mass, and **g** is acceleration due to gravity, (usually rounded to ).

The weight of an object can be thought of as being applied at a single point in that object called the **center of mass **or **gravity**. The MCAT will not directly test your ability to determine center of mass; however, such a calculation may be an important step in a problem with the larger focus of Newtonian mechanics.

To illustrate this concept and calculation, consider a tennis racquet that has been thrown into the air. Each part of the racquet moves in its own pathway, so it’s not possible to represent the motion of the whole racquet as a single particle. However, one point within the racquet moves in a simple parabolic path, very similar to the flight of a ball. It is this point within the racquet that is known as the center of mass. This is clearly shown in Figure 1.8.

**Figure** **1.8.** **Center of Mass of a Tennis Racquet** *The center of mass of a racquet thrown into the air travels along a parabolic pathway.*

For a system in which particles are distributed in all three dimensions, the center of mass is defined by the three coordinates:

**Equation 1.12**

where *m*_{1}, *m*_{2}, and *m*_{3} are the three sample masses, and the *x*-, *y*- and *z*-values are coordinates. The center of gravity is related and corresponds to the single point at which one can conceptualize gravity acting on an object. Only for a homogeneous body (with symmetrical shape and uniform density) should one expect the center of gravity be located at its geometric center. For example, we can approximate the center of gravity for a metal ball as the geometric center of the sphere. The same cannot be said, however, for a human body, television, or any asymmetrical, non-uniform object.

**KEY CONCEPT**

The center of mass of a uniform object is at the geometric center of the object.

ACCELERATION

**Acceleration **(**a**) is the rate of change of velocity that an object experiences as a result of some applied force. Acceleration, like velocity, is a vector quantity and is measured in SI units of meters per second squared. Acceleration in the direction opposite the initial velocity may be called**deceleration**. **Average acceleration** is defined as

**Equation 1.13**

where is the average acceleration, Δ**v **is the change in velocity, and Δ*t* is the change in time.

**Instantaneous acceleration** is defined as the average acceleration as Δ*t* approaches zero.

**Equation 1.14**

On a graph of velocity *vs.* time, the tangent to the graph at any time *t*, which corresponds to the slope of the graph at that time, indicates the instantaneous acceleration. If the slope is positive, the acceleration is positive and is in the direction of the velocity. If the slope is negative, the acceleration is negative (deceleration) and is in the direction opposite of the velocity.

**MCAT Concept Check 1.4:**

Before you move on, assess your understanding of the material with these questions.

1. When calculating frictional forces, how is directionality assigned?

2. When no force is being applied, the velocity must be:

3. True or False: The Earth creates a larger force on you than you create on the Earth.

4. Name two forces in addition to mechanical manipulation (pushing or pulling forces created by contact with an object):

·

·