Use the worked example above to help you solve this problem. A 54.0 kg skier is at the top of a slope, as shown in the figure. At the initial point, she is 8.0 m vertically above point B. (a) Setting the zero level for gravitational potential energy at B, find the gravitational potential energy of this system when the skier is at 4 and then at B. Finally, find the change in potential energy of the skier-Earth system as the skier goes from point to point Ⓡ. PE₁ = PE= ΔΡΕ = J J J (b) Repeat this problem with the zero-level at point 4. PE₁ = J J J PEf = ΔΡΕ = (c) Repeat again, with the zero level 2.00 m higher than point Ⓡ. PE₁ = J PE= J APE = J

College Physics
11th Edition
ISBN:9781305952300
Author:Raymond A. Serway, Chris Vuille
Publisher:Raymond A. Serway, Chris Vuille
Chapter1: Units, Trigonometry. And Vectors
Section: Chapter Questions
Problem 1CQ: Estimate the order of magnitude of the length, in meters, of each of the following; (a) a mouse, (b)...
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**Solution**

**(A)** Let \( y = 0 \) at \( B \). Calculate the potential energy at \( A \) and at \( B \), and calculate the change in potential energy.

Find \( PE_i \), the potential energy at \( A \).

\[ PE_i = mgy_i = (60.0 \, \text{kg})(9.80 \, \text{m/s}^2)(10.0 \, \text{m}) = 5.88 \times 10^3 \, \text{J} \]

\( PE_f = 0 \) at \( B \) by choice. Find the difference in potential energy between \( A \) and \( B \).

\[ PE_f - PE_i = 0 - 5.88 \times 10^3 \, \text{J} = -5.88 \times 10^3 \, \text{J} \]

**(B)** Repeat the problem if \( y = 0 \) at \( A \), the new reference point, so that PE = 0 at \( A \).

Find \( PE_f \), noting that point \( B \) is now at \( y = -10.0 \, \text{m} \).

\[ PE_f = mgy_f = (60.0 \, \text{kg})(9.80 \, \text{m/s}^2)(-10.0 \, \text{m}) = -5.88 \times 10^3 \, \text{J} \]

\[ PE_f - PE_i = -5.88 \times 10^3 \, \text{J} - 0 = -5.88 \times 10^3 \, \text{J} \]

**(C)** Repeat the problem, if \( y = 0 \) two meters above \( B \).

Find \( PE_i \), the potential energy at \( A \).

\[ PE_i = mgy_i = (60.0 \, \text{kg})(9.80 \, \text{m/s}^2)(8.00 \, \text{m}) = 4.70 \times 10^3 \, \text{J} \]

Find \( PE_f \), the potential energy at \( B \).

\[ PE_f = mgy_f =
Transcribed Image Text:**Solution** **(A)** Let \( y = 0 \) at \( B \). Calculate the potential energy at \( A \) and at \( B \), and calculate the change in potential energy. Find \( PE_i \), the potential energy at \( A \). \[ PE_i = mgy_i = (60.0 \, \text{kg})(9.80 \, \text{m/s}^2)(10.0 \, \text{m}) = 5.88 \times 10^3 \, \text{J} \] \( PE_f = 0 \) at \( B \) by choice. Find the difference in potential energy between \( A \) and \( B \). \[ PE_f - PE_i = 0 - 5.88 \times 10^3 \, \text{J} = -5.88 \times 10^3 \, \text{J} \] **(B)** Repeat the problem if \( y = 0 \) at \( A \), the new reference point, so that PE = 0 at \( A \). Find \( PE_f \), noting that point \( B \) is now at \( y = -10.0 \, \text{m} \). \[ PE_f = mgy_f = (60.0 \, \text{kg})(9.80 \, \text{m/s}^2)(-10.0 \, \text{m}) = -5.88 \times 10^3 \, \text{J} \] \[ PE_f - PE_i = -5.88 \times 10^3 \, \text{J} - 0 = -5.88 \times 10^3 \, \text{J} \] **(C)** Repeat the problem, if \( y = 0 \) two meters above \( B \). Find \( PE_i \), the potential energy at \( A \). \[ PE_i = mgy_i = (60.0 \, \text{kg})(9.80 \, \text{m/s}^2)(8.00 \, \text{m}) = 4.70 \times 10^3 \, \text{J} \] Find \( PE_f \), the potential energy at \( B \). \[ PE_f = mgy_f =
# PRACTICE IT

Use the worked example above to help you solve this problem. A 54.0 kg skier is at the top of a slope, as shown in the figure. At the initial point \( \text{A} \), she is 8.0 m vertically above point \( \text{B} \).

### (a)
Setting the zero level for gravitational potential energy at \( \text{B} \), find the gravitational potential energy of this system when the skier is at \( \text{A} \) and then at \( \text{B} \). Finally, find the change in potential energy of the skier-Earth system as the skier goes from point \( \text{A} \) to point \( \text{B} \).

- \( PE_i = \underline{\hspace{3cm}} \, \text{J} \)
- \( PE_f = \underline{\hspace{3cm}} \, \text{J} \)
- \( \Delta PE = \underline{\hspace{3cm}} \, \text{J} \)

### (b)
Repeat this problem with the zero-level at point \( \text{A} \).

- \( PE_i = \underline{\hspace{3cm}} \, \text{J} \)
- \( PE_f = \underline{\hspace{3cm}} \, \text{J} \)
- \( \Delta PE = \underline{\hspace{3cm}} \, \text{J} \)

### (c)
Repeat again, with the zero level 2.00 m higher than point \( \text{B} \).

- \( PE_i = \underline{\hspace{3cm}} \, \text{J} \)
- \( PE_f = \underline{\hspace{3cm}} \, \text{J} \)
- \( \Delta PE = \underline{\hspace{3cm}} \, \text{J} \)
Transcribed Image Text:# PRACTICE IT Use the worked example above to help you solve this problem. A 54.0 kg skier is at the top of a slope, as shown in the figure. At the initial point \( \text{A} \), she is 8.0 m vertically above point \( \text{B} \). ### (a) Setting the zero level for gravitational potential energy at \( \text{B} \), find the gravitational potential energy of this system when the skier is at \( \text{A} \) and then at \( \text{B} \). Finally, find the change in potential energy of the skier-Earth system as the skier goes from point \( \text{A} \) to point \( \text{B} \). - \( PE_i = \underline{\hspace{3cm}} \, \text{J} \) - \( PE_f = \underline{\hspace{3cm}} \, \text{J} \) - \( \Delta PE = \underline{\hspace{3cm}} \, \text{J} \) ### (b) Repeat this problem with the zero-level at point \( \text{A} \). - \( PE_i = \underline{\hspace{3cm}} \, \text{J} \) - \( PE_f = \underline{\hspace{3cm}} \, \text{J} \) - \( \Delta PE = \underline{\hspace{3cm}} \, \text{J} \) ### (c) Repeat again, with the zero level 2.00 m higher than point \( \text{B} \). - \( PE_i = \underline{\hspace{3cm}} \, \text{J} \) - \( PE_f = \underline{\hspace{3cm}} \, \text{J} \) - \( \Delta PE = \underline{\hspace{3cm}} \, \text{J} \)
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