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Fundamentals Of Physics
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Short Answer

Question: Two long straight thin wires with current lie against an equally long plastic cylinder, at radius R=20.0 cm from the cylinder’s central axis.

Figure 29-58a shows, in cross section, the cylinder and wire 1 but not wire 2. With wire 2 fixed in place, wire 1 is moved around the cylinder, from angle localid="1663154367897" θ1= 0° to angle localid="1663154390159" θ1=180°, through the first and second quadrants of the xy coordinate system. The net magnetic field B at the center of the cylinder is measured as a function of θ1. Figure 29-58b gives the x component Bx of that field as a function of θ1(the vertical scale is set by Bxs=6.0 μT), and Fig. 29-58c gives the y component (the vertical scale is set by Bys = 4.0 μT). (a) At what angle θ2 is wire 2 located? What are the (b) size and (c) direction (into or out of the page) of the current in wire 1 and the (d) size and (e) direction of the current in wire 2?

a) The angle θ2 at which wire 2 is located is either +90° or-90°.

b) The size of the current in wire 1 = 4.0 A.

c) The direction of the current in wire 1= out of the page

d) The size of the current in wire 2 = 2.0 A

e) The direction of the current in wire 2 is into the page.

See the step by step solution

Step by Step Solution

Step 1: The given values and the concept.

The distance between the center of the cylinder and the wires is R = 20.0cm.

The wire 2 is fixed in place.

The magnetic field at a point due to a current carrying wire is determined using the Biot-Savart law. The direction of the magnetic field is decided by the right-hand rule. The net magnetic field at the center of the cylinder is the vector sum of the magnetic fields due to wire 1 and wire 2. Using this, we can answer the above questions.

Formula:

B=μ0i2πR

Step 2: (a) Calculate the angle  θ2 at which wire 2 is located.

The information about the net magnetic field at the center of the cylinder is given in figures (b) and (c). Using this, we can write the equations as

B= B1+B2

In the component form,

Bx= B1x+B2xBy= B1y+B2y

Bx,0= B1x,0+B2xBy,0= B1y,0+B2yBx,90= B1x,90+B2xBy,90= B1y,90+B2yBx,180= B1x,180+B2xBy,180= B1y,180+B2y

Using the values form the graph, we write

data-custom-editor="chemistry" 2= 0+B2x-4= B1y,0+B2y6= B1x,90+B2x0= 0+B2y2= 0+B2x4= B1y,180+B2y

From these equations, we can find

B2x= 2 μT and B2y=0

Hence the wire 2 must be along the y axis direction, i.e., its position must be at 90° or (i.e., 270°)

To avoid the collision of two wires, wire 2 must be at either +90° or-90°.

Hence, the angle θ2 at which wire 2 is located is either +90° or-90°.

Step 3: (b) Calculate the size of the current in wire 1

We have

B1y=μ0i12πR4× 10-6=μ0i12πRB1y,180=4 μ T

i1=4× 10-6×2π×20×10-2 4 π ×10-7 i1=40× 10-1=4.0 A

Hence, the size of the current in wire 1 = 4.0 A.

Step 4: (c) Calculate the direction of the current in wire 1

The y component of the magnetic field is positive when wire 1 is at 180°. This is possible only if the current in the wire 1 is out of the page. All the other equations are also valid for this direction of the current.

Hence, the direction of the current in wire 1= out of the page

Step 5: (d) Calculate the size of the current in wire 2

We have

B2x= 2 μ TB2x=μ0i22πR2× 10-6=μ0i22πR

i2=2× 10-6×2π×20×10-2 4 π ×10-7 i2=20× 10-1=2.0 A

Hence, the size of the current in wire 2 = 2.0 A.

Step 6: (e) Calculate the direction of the current in wire 2

The x component of the current in wire 2 is positive. Hence as seen in part (a), if the wire is at -90°, the current must be going into the page

Hence, the direction of the current in wire 2 is into the page.

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