1. Prove that f'(x) is the first derivative of f(x). 5x23 f'(x) = x² - 1* x²-1 f(x) = x* x² 2. Find the law of motion of an object acted upon by a constant force F: a. If at time t = 0, the body is at rest at the origin (x = 0). b. If x(t = 0) = 0, v(t = 0) = vo⋅ c. If x(t = 0) = xo, v(t = 0) = v0. 3. The potential energy is given by the formula u = x² (k > 0). Construct a graph and show that the motion is oscillatory.
1. Prove that f'(x) is the first derivative of f(x). 5x23 f'(x) = x² - 1* x²-1 f(x) = x* x² 2. Find the law of motion of an object acted upon by a constant force F: a. If at time t = 0, the body is at rest at the origin (x = 0). b. If x(t = 0) = 0, v(t = 0) = vo⋅ c. If x(t = 0) = xo, v(t = 0) = v0. 3. The potential energy is given by the formula u = x² (k > 0). Construct a graph and show that the motion is oscillatory.
Glencoe Physics: Principles and Problems, Student Edition
1st Edition
ISBN:9780078807213
Author:Paul W. Zitzewitz
Publisher:Paul W. Zitzewitz
Chapter6: Motion In Two Dimensions
Section6.3: Relative Velocity
Problem 27PP
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
Transcribed Image Text:1. Prove that f'(x) is the first derivative of f(x).
5x23
f'(x) = x² - 1*
x²-1
f(x) = x*
x²
2. Find the law of motion of an object acted upon by a constant force F:
a. If at time t = 0, the body is at rest at the origin (x = 0).
b. If x(t = 0) = 0, v(t = 0) = vo⋅
c. If x(t = 0) = xo, v(t = 0) = v0.
3. The potential energy is given by the formula u = x² (k > 0). Construct a graph and
show that the motion is oscillatory.
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