Question

(a) Calculate the acceleration of a skier heading down a $10.0^\circ$ slope, assuming the coefficient of friction for waxed wood on wet snow. (b) Find the angle of the slope down which this skier could coast at a constant velocity. You can neglect air resistance in both parts, and you will find the result of Exercise 5.9 to be useful. Explicitly show how you follow the steps in the Problem-Solving Strategies.

Final Answer

a) $0.74 \textrm{ m/s}^2$

b) $5.7^\circ$

### Solution video

# OpenStax College Physics for AP® Courses, Chapter 5, Problem 11 (Problems & Exercises)

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Video Transcript

This is College Physics Answers with Shaun Dychko. We start this question by drawing a picture as we do for pretty much every question. We have a skier going down a slope that’s inclined at ten degrees. We’ve drawn a free body diagram to show the three forces on the skier. These two dotted lines arrows are the components of this force of gravity. I’ve rotated the coordinate systems so that

*x*is going down the slope and*y*is going perpendicular to the slope. In the textbook, they often label the*x*-axis here as the parallel axis and the*y*-axis as the perpendicular axis, that’ll be fine too. We know that this skier is not accelerating perpendicular to this slope, so we know that this normal force equals this*y*component of gravity. We’ll use that normal force to multiply by the coefficient of kinetic friction between waxed wood and snow, and then that’ll give us the friction force. We have a component of gravity directed down the slope, so that’s the component in the positive*x*direction and then we’ll have to calculate this friction in the negative*x*direction to figure out the net force which is going to equal mass times acceleration in the*x*direction. Now we know that this angle in here is*theta*and you can remember that by looking at this triangle here, this is a right triangle and so this angle up in here, we’ll call*alpha*. Since 90 degrees of this yellow triangle are taken up by this right angle down here, that means*alpha*plus*theta*has to equal 90, because the total angles in a triangle are 180 and 90 is already accounted for there, leaving us 90 leftover for the sum of these two. Then this is a right angle here as well between*Fgy*and the slope and so that means*alpha*plus whatever this angle is here plus, well let’s pretend we don’t know what it is, we’ll call it*gamma*, maybe that’s a bit confusing but that has to equal 90. Now we know that this*alpha*is 90 minus*theta*from here so we can plug that in up there, it’s a bit messy sorry, hopefully it’s good enough. We have 90 minus*theta*plus*gamma*equals 90 and you can subtract 90 from both sides and then add*theta*to both sides and you see that*gamma*equals*theta*. So in other words, this angle in here which I was calling*gamma*for a moment is the same as*theta*. So that’s why we can say that’s*theta*in there. Alright. So that means*Fgx*is the opposite leg of this triangle here in blue and so because it’s the opposite leg we can multiply the hypotenuse*Fg*, force of gravity, by*sin theta*.*Fg*is*mg*, and so multiply*mg*by*sin theta*to get this*x*component of gravity down the slope. This force of friction is coefficient of kinetic friction times the normal force, and then we’re gonna substitute each of this into this formula here. We have the*Fgx*is*mg sin theta*, and we have the force of friction is*mu k Fn*, and all of that equals mass times acceleration in the*x*direction. Now that’s not quite good enough because we don’t know what the normal force is, but since we know that the net force in the*y*direction, perpendicular to the slope in other words, is zero. That means*Fn*upwards minus*Fgy*downwards has to equal zero and you can add*Fgy*to both sides and you get*Fn*equals*Fgy*.*Fgy*is the adjacent leg of this blue triangle and so we use cosine*theta*multiply by the hypotenuse*Fg*to get it. Substitute*mg*in for*Fg*, we have*mg cos theta*is the normal force. So returning back to the net force in the*x*direction, we have it equal to*mg sin theta*minus*mu k*times*mg cos theta*equals*ma x*. Then divide everything by*m*to get rid of it, and then we flip the sides around so we get*a x*equals*g*, which I factored out between these two terms, times*sin theta*minus*mu k cos theta*. Then we can plug in the numbers to get our answer for the acceleration, 9.8 meters per second squared times sine of ten degrees minus 0.1 times cosine of ten degrees, gives 0.74 meters per second squared. I have two significant figures here because if you go 0.1 multiplied by*cos 10*, you get 0.09 something something something, and so it’s precise to the hundreds place and that means when you’re subtracting or adding, the result of that subtraction and adding is also going to be precise to the hundreds place. That’s why I’ve rounded this to the hundreds place. Then in part b, we’re asked to find what angle of the slope will result in no acceleration. We’ve found the formula for the acceleration already so let’s reuse that, and set it to zero. And then we can divide both sides by*g*so that*g*is gone and add*mu k cos theta*to both sides and have*sin theta*equals*mu k cos theta*. Then divide both sides by*cos theta*to have only one trigonometric function, tangent, sine over cosine is tangent. So*tan theta*is*mu k*, which means*theta*is the inverse tangent of*mu k*. Inverse tangent of 0.1 is 5.7 degrees to have no acceleration and just coast at a constant speed down the slope.