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Published byEgbert Roger Small Modified over 9 years ago
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10.1 Parametric Equations
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In chapter 1, we talked about parametric equations. Parametric equations can be used to describe motion that is not a function. Remember: To graph, if there are trig functions in the parametric equations, plug in t values between 0 and 2Ө. If not, try different t- values between –10 and 10.
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Graph the parametric curve represented by x = t 2 – 1 andy = 1 – t 2 -6 -4 -2 0 2 4 6 -6-4-2246 txy –23–3 –100 0 1 100 23–3
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Write the Cartesian equation of the parametric curve represented by x = t 2 – 1 andy = 1 – t 2 Solve for tx = t 2 – 1 ±(x + 1) 1/2 = t Substitute t into the other expression y = 1 – (±(x + 1) 1/2 ) 2 y = 1 – (x + 1) y = –x
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The formula for finding the slope of a parametrized curve is: This makes sense if we think about canceling dt. If f and g have derivatives at t, then the parametrized curve also has a derivative at t.
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The formula for finding the slope of a parametrized curve is: We assume that the denominator is not zero.
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To find the second derivative of a parametrized curve, we find the derivative of the first derivative: 1.Find the first derivative ( dy/dx ). 2. Find the derivative of dy/dx with respect to t. 3. Divide by dx/dt.
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Example:
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1.Find the first derivative ( dy/dx ).
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2. Find the derivative of dy/dx with respect to t. Quotient Rule
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3. Divide by dx/dt.
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The equation for the length of a parametrized curve is similar to our previous “length of curve” equation: (Notice the use of the Pythagorean Theorem.) (proof on pg. 533)
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Remember: –A particle is AT REST when both dy/dt and dx/dt are 0.
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Likewise, the equations for the surface area of a parametrized curve are similar to our previous “surface area” equations:
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