Figure 1.
Profile of the deflected circular membrane under the uniformly distributed transverse loads q.
Figure 1.
Profile of the deflected circular membrane under the uniformly distributed transverse loads q.
Figure 2.
Profile of the free body under the external loads q and the membrane force σrh.
Figure 2.
Profile of the free body under the external loads q and the membrane force σrh.
Figure 3.
The micro area element ABCD taken out arbitrarily from the deflected circular membrane and its projection A′B′C′D′ on the polar plane (r, φ).
Figure 3.
The micro area element ABCD taken out arbitrarily from the deflected circular membrane and its projection A′B′C′D′ on the polar plane (r, φ).
Figure 4.
Schematic diagram: (
a) The profile, along the meridian in which the curve
in
Figure 3 is located, of the deflected circular membrane; (
b) The projection of the radial membrane forces σ
r(
r)
h and σ
r(
r + ∆
r)
h and circumferential membrane forces σ
t(
r)
h and σ
t(
r + ∆
r)
h on the polar plane (
r,
φ).
Figure 4.
Schematic diagram: (
a) The profile, along the meridian in which the curve
in
Figure 3 is located, of the deflected circular membrane; (
b) The projection of the radial membrane forces σ
r(
r)
h and σ
r(
r + ∆
r)
h and circumferential membrane forces σ
t(
r)
h and σ
t(
r + ∆
r)
h on the polar plane (
r,
φ).
Figure 5.
The geometric relationship between the micro radial straight line element and the micro meridional curve element .
Figure 5.
The geometric relationship between the micro radial straight line element and the micro meridional curve element .
Figure 6.
The geometric relationship between the circumferential curve micro elements and .
Figure 6.
The geometric relationship between the circumferential curve micro elements and .
Figure 7.
Variations of b0 with n when q takes 0.0001 MPa.
Figure 7.
Variations of b0 with n when q takes 0.0001 MPa.
Figure 8.
Variations of d0 with n when q takes 0.0001 MPa.
Figure 8.
Variations of d0 with n when q takes 0.0001 MPa.
Figure 9.
Variations of b0 with n when q takes 0.005 MPa.
Figure 9.
Variations of b0 with n when q takes 0.005 MPa.
Figure 10.
Variations of d0 with n when q takes 0.005 MPa.
Figure 10.
Variations of d0 with n when q takes 0.005 MPa.
Figure 11.
Variations of b0 with n when q takes 0.012 MPa.
Figure 11.
Variations of b0 with n when q takes 0.012 MPa.
Figure 12.
Variations of d0 with n when q takes 0.012 MPa.
Figure 12.
Variations of d0 with n when q takes 0.012 MPa.
Figure 13.
Variations of bi with i when q takes 0.0001 MPa.
Figure 13.
Variations of bi with i when q takes 0.0001 MPa.
Figure 14.
Variations of ci with i when q takes 0.0001 MPa.
Figure 14.
Variations of ci with i when q takes 0.0001 MPa.
Figure 15.
Variations of di with i when q takes 0.001 MPa.
Figure 15.
Variations of di with i when q takes 0.001 MPa.
Figure 16.
Variations of b0 with n for q = 0.0001 MPa, where the blue dashed line corresponds to the case when n is odd and the red dotted line corresponds to the case when n is even.
Figure 16.
Variations of b0 with n for q = 0.0001 MPa, where the blue dashed line corresponds to the case when n is odd and the red dotted line corresponds to the case when n is even.
Figure 17.
Variations of c0 with n for q = 0.0001 MPa, where the blue dashed line corresponds to the case when n is odd and the red dotted line corresponds to the case when n is even.
Figure 17.
Variations of c0 with n for q = 0.0001 MPa, where the blue dashed line corresponds to the case when n is odd and the red dotted line corresponds to the case when n is even.
Figure 18.
Variations of d0 with n for q = 0.0001 MPa, where the blue dashed line corresponds to the case when n is odd and the red dotted line corresponds to the case when n is even.
Figure 18.
Variations of d0 with n for q = 0.0001 MPa, where the blue dashed line corresponds to the case when n is odd and the red dotted line corresponds to the case when n is even.
Figure 19.
Variations of b0 with n for q = 0.005 MPa, where the blue dashed line corresponds to the case when n is odd and the red dotted line corresponds to the case when n is even.
Figure 19.
Variations of b0 with n for q = 0.005 MPa, where the blue dashed line corresponds to the case when n is odd and the red dotted line corresponds to the case when n is even.
Figure 20.
Variations of c0 with n for q = 0.005 MPa, where the blue dashed line corresponds to the case when n is odd and the red dotted line corresponds to the case when n is even.
Figure 20.
Variations of c0 with n for q = 0.005 MPa, where the blue dashed line corresponds to the case when n is odd and the red dotted line corresponds to the case when n is even.
Figure 21.
Variations of d0 with n for q = 0.005 MPa, where the blue dashed line corresponds to the case when n is odd and the red dotted line corresponds to the case when n is even.
Figure 21.
Variations of d0 with n for q = 0.005 MPa, where the blue dashed line corresponds to the case when n is odd and the red dotted line corresponds to the case when n is even.
Figure 22.
Variations of b0 with n for q = 0.012 MPa, where the blue dashed line corresponds to the case when n is odd and the red dotted line corresponds to the case when n is even.
Figure 22.
Variations of b0 with n for q = 0.012 MPa, where the blue dashed line corresponds to the case when n is odd and the red dotted line corresponds to the case when n is even.
Figure 23.
Variations of c0 with n for q = 0.012 MPa, where the blue dashed line corresponds to the case when n is odd and the red dotted line corresponds to the case when n is even.
Figure 23.
Variations of c0 with n for q = 0.012 MPa, where the blue dashed line corresponds to the case when n is odd and the red dotted line corresponds to the case when n is even.
Figure 24.
Variations of d0 with n for q = 0.012 MPa, where the blue dashed line corresponds to the case when n is odd and the red dotted line corresponds to the case when n is even.
Figure 24.
Variations of d0 with n for q = 0.012 MPa, where the blue dashed line corresponds to the case when n is odd and the red dotted line corresponds to the case when n is even.
Figure 25.
Variations of bi(x − 1/2)i with i for q = 0.0001 MPa, where the dashed line with squares corresponds to the case when x = 1 and the dashed line with triangles corresponds to the case when x = 0.
Figure 25.
Variations of bi(x − 1/2)i with i for q = 0.0001 MPa, where the dashed line with squares corresponds to the case when x = 1 and the dashed line with triangles corresponds to the case when x = 0.
Figure 26.
Variations of ci(x − 1/2)i with i for q = 0.0001 MPa, where the dashed line with squares corresponds to the case when x = 1 and the dashed line with triangles corresponds to the case when x = 0.
Figure 26.
Variations of ci(x − 1/2)i with i for q = 0.0001 MPa, where the dashed line with squares corresponds to the case when x = 1 and the dashed line with triangles corresponds to the case when x = 0.
Figure 27.
Variations of di(x − 1/2)i with i for q = 0.0001 MPa, where the dashed line with squares corresponds to the case when x = 1 and the dashed line with triangles corresponds to the case when x = 0.
Figure 27.
Variations of di(x − 1/2)i with i for q = 0.0001 MPa, where the dashed line with squares corresponds to the case when x = 1 and the dashed line with triangles corresponds to the case when x = 0.
Figure 28.
Variations of bi(x − 1/2)i with i for q = 0.005 MPa, where the dashed line with squares corresponds to the case when x = 1 and the dashed line with triangles corresponds to the case when x = 0.
Figure 28.
Variations of bi(x − 1/2)i with i for q = 0.005 MPa, where the dashed line with squares corresponds to the case when x = 1 and the dashed line with triangles corresponds to the case when x = 0.
Figure 29.
Variations of ci(x − 1/2)i with i for q = 0.005 MPa, where the dashed line with squares corresponds to the case when x = 1 and the dashed line with triangles corresponds to the case when x = 0.
Figure 29.
Variations of ci(x − 1/2)i with i for q = 0.005 MPa, where the dashed line with squares corresponds to the case when x = 1 and the dashed line with triangles corresponds to the case when x = 0.
Figure 30.
Variations of di(x − 1/2)i with i for q = 0.005 MPa, where the dashed line with squares corresponds to the case when x = 1 and the dashed line with triangles corresponds to the case when x = 0.
Figure 30.
Variations of di(x − 1/2)i with i for q = 0.005 MPa, where the dashed line with squares corresponds to the case when x = 1 and the dashed line with triangles corresponds to the case when x = 0.
Figure 31.
Variations of bi(x − 1/2)i with i for q = 0.012 MPa, where the dashed line with squares corresponds to the case when x = 1 and the dashed line with triangles corresponds to the case when x = 0.
Figure 31.
Variations of bi(x − 1/2)i with i for q = 0.012 MPa, where the dashed line with squares corresponds to the case when x = 1 and the dashed line with triangles corresponds to the case when x = 0.
Figure 32.
Variations of ci(x − 1/2)i with i for q = 0.012 MPa, where the dashed line with squares corresponds to the case when x = 1 and the dashed line with triangles corresponds to the case when x = 0.
Figure 32.
Variations of ci(x − 1/2)i with i for q = 0.012 MPa, where the dashed line with squares corresponds to the case when x = 1 and the dashed line with triangles corresponds to the case when x = 0.
Figure 33.
Variations of di(x − 1/2)i with i for q = 0.012 MPa, where the dashed line with squares corresponds to the case when x = 1 and the dashed line with triangles corresponds to the case when x = 0.
Figure 33.
Variations of di(x − 1/2)i with i for q = 0.012 MPa, where the dashed line with squares corresponds to the case when x = 1 and the dashed line with triangles corresponds to the case when x = 0.
Figure 34.
Variations of w with r when q takes 0.0001 MPa, 0.005 MPa, and 0.012 MPa.
Figure 34.
Variations of w with r when q takes 0.0001 MPa, 0.005 MPa, and 0.012 MPa.
Table 1.
The results of numerical calculations of the undetermined constants b0 and d0.
Table 1.
The results of numerical calculations of the undetermined constants b0 and d0.
n | q = 0.0001 MPa | q = 0.005 MPa | q = 0.012 MPa |
---|
b0 | d0 | b0 | d0 | b0 | d0 |
---|
2 | 0.016169 | 0.119861 | 0.193170 | 0.501627 | 0.308604 | 0.753581 |
4 | 0.017197 | 0.121958 | 0.194231 | 0.481063 | 0.269089 | 0.657447 |
6 | 0.017409 | 0.121796 | 0.198052 | 0.485553 | 0.307288 | 0.735958 |
8 | 0.017466 | 0.121661 | 0.197643 | 0.481663 | 0.225534 | 0.215176 |
10 | 0.017483 | 0.121602 | 0.198348 | 0.483176 | 0.309685 | 0.806992 |
12 | 0.017489 | 0.121579 | 0.198152 | 0.481599 | 0.188651 | 0.477415 |
14 | 0.017491 | 0.121570 | 0.198342 | 0.482657 | 0.281565 | 2.375341 |
16 | 0.017491 | 0.121567 | 0.197866 | 0.481204 | 0.400863 | 0.807886 |
18 | 0.017491 | 0.121566 | 0.198838 | 0.483293 | 0.204223 | 3.829090 |
20 | 0.017491 | 0.121566 | 0.197574 | 0.483140 | 0.441707 | 0.929497 |
Table 2.
The calculation results of the power series coefficients bi, ci, and di when q = 0.0001 MPa.
Table 2.
The calculation results of the power series coefficients bi, ci, and di when q = 0.0001 MPa.
i | bi | ci | di |
---|
0 | 0.017491 | 0.017491 | 0.121566 |
2 | −2.299 × 10−3 | −8.614 × 10−3 | −1.108 × 10−1 |
4 | −2.754 × 10−4 | −1.603 × 10−3 | −8.641 × 10−3 |
6 | −5.116 × 10−5 | −4.148 × 10−4 | −1.610 × 10−3 |
8 | −1.166 × 10−5 | −1.210 × 10−4 | −3.786 × 10−4 |
10 | −2.985 × 10−6 | −3.764 × 10−5 | −1.002 × 10−4 |
12 | −8.248 × 10−7 | −1.222 × 10−5 | −2.851 × 10−5 |
14 | −2.405 × 10−7 | −4.084 × 10−6 | −8.523 × 10−6 |
16 | −1.108 × 10−7 | −1.277 × 10−6 | −1.960 × 10−6 |
18 | −3.655 × 10−8 | −4.165 × 10−7 | −5.770 × 10−7 |
20 | −1.199 × 10−8 | −1.392 × 10−7 | −1.788 × 10−7 |
Table 3.
The results of numerical calculation of the undetermined constants b0, c0, and d0.
Table 3.
The results of numerical calculation of the undetermined constants b0, c0, and d0.
n | q = 0.0001 MPa | q = 0.005 MPa | q = 0.012 MPa |
---|
b0 | c0 | d0 | b0 | c0 | d0 | b0 | c0 | d0 |
---|
3 | 0.016292 | 0.013668 | 0.097291 | 0.221177 | 0.180552 | 0.363450 | 0.393014 | 0.290205 | 0.508047 |
4 | 0.016718 | 0.015038 | 0.094576 | 0.220879 | 0.182558 | 0.364409 | 0.390632 | 0.288871 | 0.515486 |
5 | 0.016828 | 0.015165 | 0.093735 | 0.222826 | 0.183804 | 0.361598 | 0.393688 | 0.291004 | 0.509066 |
6 | 0.016860 | 0.015200 | 0.093493 | 0.223041 | 0.184274 | 0.361110 | 0.393789 | 0.291508 | 0.510216 |
7 | 0.016888 | 0.015212 | 0.093368 | 0.223105 | 0.184385 | 0.360962 | 0.393968 | 0.291706 | 0.509820 |
8 | 0.016893 | 0.015226 | 0.093332 | 0.223154 | 0.184416 | 0.360908 | 0.394006 | 0.291809 | 0.509858 |
9 | 0.016897 | 0.015228 | 0.093312 | 0.223184 | 0.184445 | 0.360872 | 0.394056 | 0.291849 | 0.509829 |
10 | 0.016898 | 0.015230 | 0.093305 | 0.223189 | 0.184457 | 0.360859 | 0.394109 | 0.291876 | 0.509833 |
11 | 0.016898 | 0.015230 | 0.093305 | 0.223189 | 0.184457 | 0.360859 | 0.394109 | 0.291876 | 0.509833 |
Table 4.
The calculation results of bi(x − 1/2)i, ci(x − 1/2)i, and di(x − 1/2)i for q = 0.0001 MPa.
Table 4.
The calculation results of bi(x − 1/2)i, ci(x − 1/2)i, and di(x − 1/2)i for q = 0.0001 MPa.
i | x = 1 | x = 0 |
---|
bi(x − 1/2)i | ci(x − 1/2)i | di(x − 1/2)i | bi(x − 1/2)i | ci(x − 1/2)i | di(x − 1/2)i |
---|
0 | 1.689 × 10−2 | 1.523 × 10−2 | 9.331 × 10−2 | 1.690 × 10−2 | 1.523 × 10−2 | 9.331 × 10−2 |
1 | −1.223 × 10−3 | −4.752 × 10−3 | −5.773 × 10−2 | 1.223 × 10−3 | 4.752 × 10−3 | 5.773 × 10−2 |
2 | −6.919 × 10−4 | −2.867 × 10−3 | −3.137 × 10−2 | −6.919 × 10−4 | −2.867 × 10−3 | −3.137 × 10−2 |
3 | −8.723 × 10−5 | −5.628 × 10−4 | −2.761 × 10−3 | 8.723 × 10−5 | 5.628 × 10−4 | 2.761 × 10−3 |
4 | −3.387 × 10−5 | −2.393 × 10−4 | −1.046 × 10−3 | −3.387 × 10−5 | −2.393 × 10−4 | −1.046 × 10−3 |
5 | −7.384 × 10−6 | −7.853 × 10−5 | −2.654 × 10−4 | 7.384 × 10−6 | 7.853 × 10−5 | 2.654 × 10−4 |
6 | −3.976 × 10−6 | −3.010 × 10−5 | −9.547 × 10−5 | −3.976 × 10−6 | −3.010 × 10−5 | −9.547 × 10−5 |
7 | 2.587 × 10−6 | −1.295 × 10−5 | −3.154 × 10−5 | −2.587 × 10−6 | 1.295 × 10−5 | 3.154 × 10−5 |
8 | −1.691 × 10−6 | −3.372 × 10−6 | −1.154 × 10−5 | −1.691 × 10−6 | −3.372 × 10−6 | −1.154 × 10−5 |
9 | 1.381 × 10−6 | −3.009 × 10−6 | −4.282 × 10−6 | −1.381 × 10−6 | 3.009 × 10−6 | 4.282 × 10−6 |
10 | −1.700 × 10−7 | −8.860 × 10−7 | −1.561 × 10−6 | −1.700 × 10−7 | −8.860 × 10−7 | −1.561 × 10−6 |
11 | 1.665 × 10−7 | −2.589 × 10−7 | −2.081 × 10−7 | −1.665 × 10−7 | 2.589 × 10−7 | 2.081 × 10−7 |
Table 5.
The calculation results of bi(x − 1/2)i, ci(x − 1/2)i and di(x − 1/2)i for q = 0.005 MPa.
Table 5.
The calculation results of bi(x − 1/2)i, ci(x − 1/2)i and di(x − 1/2)i for q = 0.005 MPa.
i | x = 1 | x = 0 |
---|
bi(x − 1/2)i | ci(x − 1/2)i | di(x − 1/2)i | bi(x − 1/2)i | ci(x − 1/2)i | di(x − 1/2)i |
---|
0 | 2.232 × 10−1 | 1.845 × 10−1 | 3.609 × 10−1 | 2.232 × 10−1 | 1.845 × 10−1 | 3.609 × 10−1 |
1 | 4.541 × 10−2 | −3.027 × 10−2 | −2.410 × 10−1 | −4.541 × 10−2 | 3.027 × 10−2 | 2.410 × 10−1 |
2 | 1.104 × 10−2 | −2.028 × 10−2 | −1.183 × 10−1 | 1.104 × 10−2 | −2.028 × 10−2 | −1.183 × 10−1 |
3 | −2.893 × 10−3 | −5.376 × 10−3 | −1.091 × 10−3 | 2.893 × 10−3 | 5.376 × 10−3 | 1.091 × 10−3 |
4 | 1.311 × 10−3 | −1.933 × 10−3 | −8.065 × 10−4 | 1.311 × 10−3 | −1.933 × 10−3 | −8.065 × 10−4 |
5 | 3.467 × 10−4 | −7.753 × 10−4 | 4.744 × 10−4 | −3.467 × 10−4 | 7.753 × 10−4 | −4.744 × 10−4 |
6 | −2.506 × 10−4 | −4.330 × 10−4 | −1.080 × 10−4 | −2.506 × 10−4 | −4.330 × 10−4 | −1.080 × 10−4 |
7 | 1.717 × 10−5 | −1.659 × 10−4 | −4.369 × 10−5 | −1.717 × 10−5 | 1.659 × 10−4 | 4.369 × 10−5 |
8 | 7.958 × 10−6 | −6.467 × 10−5 | −3.273 × 10−5 | 7.958 × 10−6 | −6.467 × 10−5 | −3.273 × 10−5 |
9 | −3.384 × 10−6 | −5.945 × 10−5 | −7.449 × 10−6 | 3.384 × 10−6 | 5.945 × 10−5 | 7.449 × 10−6 |
10 | −1.387 × 10−6 | −6.117 × 10−6 | −2.716 × 10−6 | −1.387 × 10−6 | −6.117 × 10−6 | −2.716 × 10−6 |
11 | 1.661 × 10−7 | −2.572 × 10−6 | −2.065 × 10−7 | −1.661 × 10−7 | 2.572 × 10−6 | 2.065 × 10−7 |
Table 6.
The calculation results of bi(x − 1/2)i, ci(x − 1/2)i, and di(x − 1/2)i for q = 0.012 MPa.
Table 6.
The calculation results of bi(x − 1/2)i, ci(x − 1/2)i, and di(x − 1/2)i for q = 0.012 MPa.
i | x = 1 | x = 0 |
---|
bi(x − 1/2)i | ci(x − 1/2)i | di(x − 1/2)i | bi(x − 1/2)i | ci(x − 1/2)i | di(x − 1/2)i |
---|
0 | 3.941 × 10−1 | 2.919 × 10−1 | 5.098 × 10−1 | 3.941 × 10−1 | 2.919 × 10−1 | 5.098 × 10−1 |
1 | 1.722 × 10−1 | −7.288 × 10−3 | −3.655 × 10−1 | −1.722 × 10−1 | 7.288 × 10−3 | 3.655 × 10−1 |
2 | 3.862 × 10−2 | −6.277 × 10−3 | −1.578 × 10−1 | 3.862 × 10−2 | −6.277 × 10−3 | −1.578 × 10−1 |
3 | −2.335 × 10−2 | −4.856 × 10−3 | 1.683 × 10−2 | 2.335 × 10−2 | 4.856 × 10−3 | −1.683 × 10−2 |
4 | 9.121 × 10−3 | −1.172 × 10−3 | −2.661 × 10−3 | 9.121 × 10−3 | −1.172 × 10−3 | −2.661 × 10−3 |
5 | −1.704 × 10−3 | −1.037 × 10−3 | −1.188 × 10−3 | 1.704 × 10−3 | 1.037 × 10−3 | 1.188 × 10−3 |
6 | −1.198 × 10−3 | −9.729 × 10−5 | 7.394 × 10−4 | −1.198 × 10−3 | −9.729 × 10−5 | 7.394 × 10−4 |
7 | 1.101 × 10−3 | −8.095 × 10−4 | −2.746 × 10−4 | −1.101 × 10−3 | 8.095 × 10−4 | 2.746 × 10−4 |
8 | −7.617 × 10−4 | −7.503 × 10−4 | −6.031 × 10−5 | −7.617 × 10−4 | −7.503 × 10−4 | −6.031 × 10−5 |
9 | 1.625 × 10−4 | −5.544 × 10−5 | 5.748 × 10−5 | −1.625 × 10−4 | 5.544 × 10−5 | −5.748 × 10−5 |
10 | 1.145 × 10−4 | −5.256 × 10−5 | −3.611 × 10−5 | 1.145 × 10−4 | −5.256 × 10−5 | −3.611 × 10−5 |
11 | −1.418 × 10−5 | −1.010 × 10−5 | 8.009 × 10−6 | 1.418 × 10−5 | 1.010 × 10−5 | −8.009 × 10−6 |