The force (in pound-force) needed to keep a car from skidding on a curve varies directly with the weight of the car (in pounds) and the square of its speed (in miles per hour [mph]) and inversely with the radius (in feet) of the curve. Suppose 6125 pound force is required to keep a 2750 pound car, travelling at a speed of 35 mph, from skidding on a curve of radius 550 feet. How much pound-force is then required to keep a 3600 pound car, travelling at a speed of 50 mph, from skidding on a curve of radius 750 feet?
12000
The question describes how the force needed to prevent a car from skidding on a curve is related to several factors: the car's weight, its speed, and the radius of the curve. This relationship is given by a variation equation.
We are told that the force (\(F\)) varies directly with the weight (\(W\)) and the square of the speed (\(v^2\)), and inversely with the radius (\(r\)). This can be written as:
\[ F \propto \frac{W v^2}{r} \]
To turn this proportionality into an equation, we introduce a constant of proportionality, let's call it \(k\):
\[ F = k \frac{W v^2}{r} \]
Our goal is to first find the value of this constant \(k\) using the information from the first scenario, and then use \(k\) to calculate the force needed for the second scenario.
From the first scenario, we are given:
We can plug these values into our equation to solve for \(k\):
\[ 6125 = k \frac{2750 \times 35^2}{550} \]
First, calculate \(35^2\):
\[ 35^2 = 1225 \]
Now substitute this back into the equation:
\[ 6125 = k \frac{2750 \times 1225}{550} \]
Let's simplify the term \(\frac{2750}{550}\). \(2750 \div 550 = 5\).
\[ 6125 = k \times 5 \times 1225 \]
\[ 6125 = k \times (5 \times 1225) \]
\[ 6125 = k \times 6125 \]
Now, solve for \(k\):
\[ k = \frac{6125}{6125} \]
\[ k = 1 \]
The proportionality constant \(k\) is 1.
Now we know the relationship is simply \(F = \frac{W v^2}{r}\). For the second scenario, we are given:
We need to find the force (\(F_2\)) required to keep this car from skidding. Using the equation with \(k=1\):
\[ F_2 = 1 \times \frac{W_2 v_2^2}{r_2} \]
\[ F_2 = \frac{3600 \times 50^2}{750} \]
First, calculate \(50^2\):
\[ 50^2 = 2500 \]
Substitute this back into the equation:
\[ F_2 = \frac{3600 \times 2500}{750} \]
Now, perform the multiplication in the numerator:
\[ 3600 \times 2500 = 9,000,000 \]
So, the equation becomes:
\[ F_2 = \frac{9,000,000}{750} \]
Finally, divide to find \(F_2\):
\[ F_2 = 12000 \]
The required force is 12000 pound-force.
| Variable | Scenario 1 | Scenario 2 |
| Force (F) | 6125 lbf | ? |
| Weight (W) | 2750 lbs | 3600 lbs |
| Speed (v) | 35 mph | 50 mph |
| Radius (r) | 550 ft | 750 ft |
| Relationship | \(F = k \frac{W v^2}{r}\) | |
| Constant (k) Calculation | \(k = \frac{F_1 r_1}{W_1 v_1^2} = \frac{6125 \times 550}{2750 \times 35^2} = 1\) | |
| Force (F2) Calculation | \(F_2 = k \frac{W_2 v_2^2}{r_2} = 1 \times \frac{3600 \times 50^2}{750} = \frac{3600 \times 2500}{750} = 12000\) lbf | |
The force required to keep the 3600 pound car, travelling at 50 mph, from skidding on a curve of radius 750 feet is 12000 pound-force.
| Concept | Description | Mathematical Form |
|---|---|---|
| Direct Variation | One variable increases as another increases proportionally. | \(y = kx\) |
| Inverse Variation | One variable increases as another decreases proportionally. | \(y = k/x\) |
| Joint Variation | A variable varies directly as the product of two or more other variables. | \(z = kxy\) |
| Combined Variation | A variable varies directly with one or more variables and inversely with one or more other variables. | \(A = k \frac{BC}{D}\) (Example) |
The force discussed in this problem is related to the centripetal force required to make the car turn. When a car turns on a flat road, the centripetal force is primarily provided by the static friction force between the tires and the road. The formula \(F = m \frac{v^2}{r}\) is the standard physics formula for centripetal force, where \(m\) is mass and \(v\) is velocity (speed), and \(r\) is the radius. Since weight (\(W\)) is mass (\(m\)) times acceleration due to gravity (\(g\)), \(W = mg\), we can write \(m = W/g\). Substituting this into the centripetal force formula gives \(F = \frac{W}{g} \frac{v^2}{r}\). Comparing this to our variation equation \(F = k \frac{W v^2}{r}\), we see that the proportionality constant \(k\) is related to \(1/g\), scaled by units. Our calculation found \(k=1\), which suggests that the units used in the problem (pound-force, pounds, mph, feet) must incorporate the gravitational constant in such a way that \(k\) becomes 1. In practice, the maximum static friction force depends on the coefficient of static friction and the normal force (which is equal to the weight on a flat road). The car will skid if the required centripetal force exceeds the maximum possible static friction force.
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